Differentiate between organic and inorganic analysis.
Respond to one of the following:
Option 1: Differentiate between organic and inorganic analysis. Differentiate between qualitative and quantitative measurement
Option 2: Gas chromatography is one of the basic analysis procedures for the crime lab. Describe this process and the theory upon which it is based.
Option 3: Describe the Mass Spectrometry process.
Option 4: Describe the X-ray diffraction process.
Option 5: Our text describes five types of microscopes commonly used in forensic analysis. List them and briefly describe the function of each.
Option 6: Below is a series of twenty-three questions about drugs or drug use. For your original posting, answer one of these questions that has not been answered by anyone else as yet by identifying which question you are answering by number. There should be enough questions that each of you can answer a separate one.
Following are descriptions of behavior that are characteristic among users of certain classes of drugs. For each description, indicate the class of drug (narcotics, stimulants, and so forth) for which the behavior is most characteristic.
1. slurred speech, slow reaction time, impaired judgment, reduced coordination
2. intense emotional responses, anxiety, altered sensory perceptions
3. alertness, feelings of strength and confidence, rapid speech and movement, decreased appetite
4. drowsiness, intense feelings of well-being, relief from pain
Following are descriptions of behavior that are characteristic among users of certain classes of drugs. Name at least one drug that produces the described effects.
5. slurred speech, slow reaction time, impaired judgment, reduced coordination
6. intense emotional responses, anxiety, altered sensory perceptions
7. alertness, feelings of strength and confidence, rapid speech and movement, decreased appetite
8. drowsiness, intense feelings of well-being, relief from pain
Following are descriptions of hypothetical drugs. According to the Controlled Substances Act, under which drug schedule would each substance be classified?
9. This drug has a high potential for psychological dependence, it currently has accepted medical uses in the United States, and the distributor is not required to report to the U. S. Drug Enforcement Administration.
10. This drug has medical use in the United States, is not limited by manufacturing quotas, and may be exported without a permit.
11. This drug must be stored in a vault or safe, requires separate records keeping, and may be distributed with a prescription.
12. This drug may not be imported or exported without a permit, is subject to manufacturing quotas, and currently has no medical use in the United States.
The figure on page 143 shows a chromatogram of a known mixture of barbiturates. Based on the figure, answer one of the following questions.
13, Which barbiturate detected by the chromatogram had the longest retention time?
14. Which barbiturate had the shortest retention time?
15. What is the approximate retention time of amobarbital?
Do you like having multiple choices from which to select a response, or do you prefer everyone answering the same question? GB
I MUST HAVE IT BY WEDNESDAY
Death by Tylenol
In 1982, two firefighters from a Chicago suburb were casually discussing four bizarre deaths that had recently taken place in a neighboring area. As they discussed the circumstances of the deaths, they realized that each of the victims had taken Tylenol. Their suspicions were immediately reported to police investigators. Tragically, before the general public could be alerted, three more victims died after taking poison- laced Tylenol capsules. Seven individuals, all in the Chicago area, were the first victims to die from what has become known as product tampering. A forensic chemical analysis of Tylenol capsules recovered from the victims’ residences showed that the capsules were filled with potassium cyanide in a quantity ten thousand times what was needed to kill an average person. It was quickly determined that the
cyanide was not introduced into the bottles at the factory. Instead, the perpetrator methodically
emptied each of twenty to thirty capsules and then refilled them with potassium cyanide. The tampered capsules were rebottled, carefully repackaged,
and placed on the shelves of six different stores. The case of the Tylenol murders remains unsolved, and the $100,000 reward offered by Tylenol’s manufacturer remains unclaimed.
headline news
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After studying this chapter you should be able to: • Define and distinguish elements and compounds
• Contrast the differences among a solid, liquid, and gas
• Define and distinguish organic and inorganic compounds
• Understand the difference between qualitative and quantitative analysis
• Describe and explain the process of chromatography
• List and describe the parts of a gas chromatograph
• Explain the differences among thin-layer chromatography, gas chromatography, and electrophoresis
• Understand the differences between the wave and particle theories of light
• Describe the electromagnetic spectrum
• Name the parts of a simple absorption spectrophotometer
• Describe the utility of ultraviolet and infrared spectroscopy for the identification of organic compounds
• Describe the concept and utility of mass spectrometry for identification analysis
organic analysis
chromatography compound electromagnetic
spectrum electrophoresis element fluoresce frequency gas (vapor) infrared inorganic ion laser liquid matter monochromatic light monochromator organic periodic table phase photon physical state pyrolysis solid spectrophotometry sublimation ultraviolet visible light wavelength X-ray
KEY TERMS
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gas (vapor) A state of matter in which the attractive forces between molecules are small enough to permit them to move with complete freedom
liquid A state of matter in which molecules are in contact with one another but are not rigidly held in place
solid A state of matter in which the molecules are held closely together in a rigid state
physical state A condition or stage in the form of matter; a solid, liquid, or gas
compound A pure substance composed of two or more elements
element A fundamental particle of matter; an element cannot be broken down into simpler substances by chemical means
matter All things of substance; matter is composed of atoms or molecules
120 CHAPTER 5
The Nature of Matter In the previous chapter, some physical properties were described and used to characterize glass and soil evidence. Before we can apply other physical properties, as well as chemical properties, to the identification and comparison of evidence, we need to gain an insight into the composition of matter. Beginning with knowledge of the fundamental building block of all substances—the element—it will be convenient for us to classify all evidence as either organic or inorganic. The procedures used to measure the properties associated with each class are distinctly different and merit separate chapters for their description. In later chapters, we will continually return to these procedures as we discuss the examination of the various kinds of physical evidence. This chap- ter will be devoted, in large part, to reviewing a variety of techniques and instruments that have become the indispensable tools of the forensic scientist for examining organic evidence.
Elements and Compounds Matter is anything that has mass and occupies space. As we examine the world that surrounds us and consider the countless variety of materials that we encounter, we must consider one of humankind’s most remarkable accomplishments: the discovery of the concept of the atom to explain the composition of all matter. This search had its earliest contribution from the ancient Greek philosophers, who suggested air, water, fire, and earth as matter’s fundamental building blocks. It culminated with the development of the atomic theory and the discovery of matter’s simplest identity, the element.
An element is the simplest substance known and provides the building block from which all matter is composed. At present, 118 elements have been identified (see Table 5–1); of these, 89 occur naturally on the earth, and the remainder have been created in the laboratory. In Figure 5–1, all of the elements are listed by name and symbol in a form that has become known as the periodic table. This table is most useful to chemists because it systematically arranges elements with similar chemical properties in the same vertical row or group.
For convenience, chemists have chosen letter symbols to represent the elements. Many of these symbols come from the first letter of the element’s English name—for example, carbon (C), hydrogen (H), and oxygen (O). Others are two-letter abbreviations of the English name—for example, calcium (Ca) and zinc (Zn). Some symbols are derived from the first letters of Latin or Greek names. Thus, the symbol for silver, Ag, comes from the Latin name argentum; copper, Cu, from the Latin cuprum; and helium, He, from the Greek name helios.
The smallest particle of an element that can exist and still retain its identity as that element is the atom. When we write the symbol C we mean one atom of carbon; the chemical symbol for carbon dioxide, CO2, signifies one atom of carbon combined with two atoms of oxygen. When two or more elements are combined to form a substance, as with carbon dioxide, a new substance is created, different in its physical and chemical properties from its elemental components. This new material is called a compound. Compounds contain at least two elements. Considering that there are eighty-nine natural elements, it is easy to imagine the large number of possible elemental combinations that may form compounds. Not surprisingly, more than 16 million known compounds have already been identified.
Just as the atom is the basic particle of an element, the molecule is the smallest unit of a com- pound. Thus, a molecule of carbon dioxide is represented by the symbol CO2, and a molecule of table salt is symbolized by NaCl, representing the combination of one atom of the element sodium (Na) with one atom of the element chlorine (Cl).
States of Matter As we look around us and view the materials that make up the earth, it becomes an awesome task even to attempt to estimate the number of different kinds of matter that exist. A much more logical approach is to classify matter according to the physical form it takes. These forms are called physical states. There are three such states: solid, liquid, and gas (vapor). A solid is rigid and therefore has a definite shape and volume. A liquid also occupies a specific volume, but its fluidity causes it to take the shape of the container in which it is residing. A gas has neither a definite shape nor volume, and it will completely fill any container into which it is placed.
periodic table A chart of elements arranged in a systematic fashion; vertical rows are called groups or families, and horizontal rows are called series; elements in a given row have similar properties
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ORGANIC ANALYSIS 121
TABLE 5–1 List of Elements with Their Symbols and Atomic Masses
Element Symbol Atomic Massa (amu)
Lead Pb 207.2 Lithium Li 6.941 Lutetium Lu 174.97 Magnesium Mg 24.305 Manganese Mn 54.9380 Meitnerium Mt (266) Mendelevium Md (256) Mercury Hg 200.59 Molybdenum Mo 95.94 Neodymium Nd 144.24 Neon Ne 20.179 Neptunium Np 237.0482 Nickel Ni 58.71 Niobium Nb 92.9064 Nitrogen N 14.0067 Nobelium No (254) Osmium Os 190.2 Oxygen O 15.9994 Palladium Pd 106.4 Phosphorus P 30.9738 Platinum Pt 195.09 Plutonium Pu (244) Polonium Po (209) Potassium K 39.102 Praseodymium Pr 140.9077 Promethium Pm (145) Protactinium Pa 231.0359 Radium Ra 226.0254 Radon Rn (222) Rhenium Re 186.2 Rhodium Rh 102.9055 Roentgenium Rg (272) Rubidium Rb 85.4678 Ruthenium Ru 101.07 Rutherfordium Rf (257) Samarium Sm 105.4 Scandium Sc 44.9559 Seaborgium Sg (263) Selenium Se 78.96 Silicon Si 28.086 Silver Ag 107.868 Sodium Na 22.9898 Strontium Sr 87.62 Sulfur S 32.06 Tantalum Ta 180.9479 Technetium Tc 98.9062 Tellurium Te 127.60 Terbium Tb 158.9254 Thallium Tl 204.37 Thorium Th 232.0381 Thulium Tm 168.9342
Element Symbol Atomic Massa (amu)
Actinum Ac (227) Aluminum Al 26.9815 Americium Am (243) Antimony Sb 121.75 Argon Ar 39.948 Arsenic As 74.9216 Astatine At (210) Barium Ba 137.34 Berkelium Bk (247) Beryllium Be 9.01218 Bismuth Bi 208.9806 Bohrium Bh (262) Boron B 10.81 Bromine Br 79.904 Cadmium Cd 112.40 Calcium Ca 40.08 Californium Cf (251) Carbon C 12.011 Cerium Ce 140.12 Cesium Cs 132.9055 Chlorine Cl 35.453 Chromium Cr 51.996 Cobalt Co 58.9332 Copernicium Cp (285) Copper Cu 63.546 Curium Cm (247) Darmstadtium Ds (271) Dubnium Db (260) Dysprosium Dy 162.50 Einsteinium Es (254) Erbium Er 167.26 Europium Eu 151.96 Fermium Fm (253) Fluorine F 18.9984 Francium Fr (223) Gadolinium Gd 157.25 Gallium Ga 69.72 Germanium Ge 72.59 Gold Au 196.9665 Hafnium Hf 178.49 Hassium Hs (265) Helium He 4.00260 Holmium Ho 164.9303 Hydrogen H 1.0080 Indium In 114.82 Iodine I 126.9045 Iridium Ir 192.22 Iron Fe 55.847 Krypton Kr 83.80 Lanthanum La 138.9055 Lawrencium Lr (257)
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sublimation A physical change from the solid state directly into the gaseous state
122 CHAPTER 5
CHANGES OF STATE Substances can change from one state to another. For example, as water is heated, it is converted from a liquid form into a vapor. At a high enough temperature (100°C), water boils and rapidly changes into steam. Similarly, at 0°C, water solidifies or freezes into ice. Under certain conditions, some solids can be converted directly into a gaseous state. For instance, a piece of dry ice (solid carbon dioxide) left standing at room temperature quickly forms carbon dioxide vapor and disappears. This change of state from a solid to a gas is called sublimation.
In each of these examples, no new chemical species are formed; matter is simply being changed from one physical state to another. Water, whether in the form of liquid, ice, or steam, remains chemically H2O. Simply, what has been altered are the attractive forces between the water molecules. In a solid, these forces are very strong, and the molecules are held closely to- gether in a rigid state. In a liquid, the attractive forces are not as strong, and the molecules have more mobility. Finally, in the vapor state, appreciable attractive forces no longer exist among the molecules; thus, they may move in any direction at will.
1 H
3 Li
11 Na
19 K
37 Rb
55 Cs
87 Fr
4 Be
12 Mg
20 Ca
38 Sr
56 Ba
88 Ra
IIIB
39 Y
57 La
89 Ac
IVB
40 Zr
72 Hf
104 Rf
VB
41 Nb
73 Ta
105 Db
VIB
42 Mo
74 W
106 Sg
VIIB
43 Tc
75 Re
107 Bh
44 Ru
76 Os
108 Hs
VIII
45 Rh
77 Ir
109 Mt
46 Pd
78 Pt
110 Ps
IB
47 Ag
79 Au
111 Rg
IIB
48 Cd
80 Hg
112 Cp
5 B
13 Al
IIIA
49 In
81 Tl
113 Uut
6 C
14 Si
IVA
50 Sn
82 Pb
114 Uuq
7 N
15 P
VA
51 Sb
83 Bi
115 Uup
8 O
16 S
VIA
52 Te
84 Po
116 Uuh
9 F
17 Cl
VIIA
53 I
85 At
117 Uus
2 He
10 Ne
18 Ar
O
54 Xe
21 Sc
22 Ti
23 V
24 Cr
25 Mn
26 Fe
27 Co
28 Ni
29 Cu
30 Zn
31 Ga
32 Ge
33 As
34 Se
35 Br
36 Kr
86 Rn
118 Uuo
58 Ce
90 Th
59 Pr
91 Pa
60 Nd
92 U
61 Pm
93 Np
62 Sm
94 Pu
63 Eu
95 Am
64 Gd
96 Cm
65 Tb
97 Bk
66 Dy
98 Cf
67 Ho
99 Es
68 Er
100 Fm
69 Tm
101 Md
70 Yb
102 No
71 Lu
103 Lr
1
2
3
4
5
6
7
a
b
aLanthanide series
bActinide series
Period IA IIA Group
FIGURE 5–1 The periodic table.
TABLE 5–1 Continued
Element Symbol Atomic Massa (amu)
Tin Sn 118.69 Titanium Ti 47.90 Tungsten W 183.85 Copernicium Cp (292) Ununoctium Uuo (294) Ununpentium Uup (288) Ununquadium Uuq (289) Ununseptium Uus (?)
Element Symbol Atomic Massa (amu)
Ununtrium Uut (284) Uranium U 238.029 Vanadium V 50.9414 Xenon Xe 131.3 Ytterbium Yb 173.04 Yttrium Y 88.9059 Zinc Zn 65.57 Zirconium Zr 91.22
aBased on the assigned relative atomic mass of C � exactly 12; parentheses denote the mass number of the isotope with the longest half-life.
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inorganic Describes a chemical compound not based on carbon
organic Describes a substance composed of carbon and often smaller amounts of hydrogen, oxygen, nitrogen, chlorine, phosphorus, or other elements
ORGANIC ANALYSIS 123
PHASES Chemists are forever combining different substances, no matter whether they are in the solid, liquid, or gaseous states, hoping to create new and useful products. Our everyday observa- tions should make it apparent that not all attempts at mixing matter can be productive. For instance, oil spills demonstrate that oil and water do not mix. Whenever substances can be distinguished by a visible boundary, different phases are said to exist. Thus, oil floating on water is an example of a two-phase system. The oil and water each constitute a separate liquid phase, clearly distinct from each other. Similarly, when sugar is first added to water, it does not dissolve, and two distinctly different phases exist: the solid sugar and the liquid water. However, after stirring, all the sugar dissolves, leaving just one liquid phase.
Selecting an Analytical Technique Now that the basic components of matter have been defined, proper selection of analytical tech- niques that enable the forensic scientist to identify or compare matter can best be understood by categorizing all substances into one of two broad groups: organics and inorganics.
Organic vs. Inorganic Substances Organic substances contain carbon, commonly in combination with hydrogen, oxygen, nitrogen, chlorine, phosphorus, or other elements. Inorganic substances encompass all other known chem- ical substances. Each of these two broad groups has distinctive and characteristic properties. Thus, once the analyst has determined whether a material is organic or inorganic, the properties to be measured and the choice of analytical techniques to be used are generally the same for all materials in each group.
Most evidence received by crime laboratories requires identification of organic compounds. These compounds may include substances such as commonly abused drugs (such as alcohol, marijuana, heroin, amphetamines, and barbiturates), synthetic fibers, petroleum products, paint binders, and high-order explosives. As we have already observed, organic compounds are composed of a combination of a relatively small number of elements that must include carbon; fortunately, the nature of the forces or bonds between these elements is such that the resultant compounds can readily be characterized by their absorption of light.
The study of the absorption of light by chemical substances, known as spectrophotometry, is a basic tool for the characterization and identification of organic materials. Although spectrophotome- try is most applicable to organic analysis, its optimal use requires that a material be in a relatively pure state. Because the purity of physical evidence is almost always beyond the control of the crim- inalist, this criterion often is not met. For this reason, the analytical technique of chromatography is widely applied for the analysis of physical evidence. Chromatography is a means of separating and tentatively identifying the components of a mixture. We will discuss both techniques in this chapter.
Qualitative vs. Quantitative Measurement Another consideration in selecting an analytical technique is the need for either a qualitative or a quantitative determination. The former relates just to the identity of the material, whereas the lat- ter refers to the percentage combination of the components of a mixture. Hence, a qualitative identification of a powder may reveal the presence of heroin and quinine, whereas a quantitative analysis may conclude the presence of 10 percent heroin and 90 percent quinine. Obviously, a qualitative identification must precede any attempt at quantitation, for little value is served by attempting to quantitate a material without first determining its identity. Essentially, a qualitative analysis of a material requires the determination of numerous properties using a variety of ana- lytical techniques. On the other hand, a quantitative measurement is usually accomplished by the precise measurement of a single property of the material.
Chromatography Chromatography as a technique for separating the components of a mixture is particularly useful for analyzing the multicomponent specimens that are frequently received in the crime laboratory. For example, illicit drugs sold on the street are not manufactured to meet government labeling standards; instead, they may be diluted with practically any material at the disposal of the drug
chromatography Any of several analytical techniques for separating organic mixtures into their components by attraction to a stationary phase while being propelled by a moving phase
spectrophotometry An analytical method for identifying a substance by its selective absorption of different wavelengths of light
phase A uniform body of matter; different phases are separated by definite visible boundaries
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124 CHAPTER 5
dealer to increase the quantity of product available to prospective customers. Hence, the task of identifying an illicit-drug preparation would be arduous without the aid of chro- matographic methods to first separate the mixture into its components.
Theory of Chromatography The theory of chromatography is based on the observation that chemical substances tend to partially escape into the surrounding environment when dissolved in a liquid or when absorbed on a solid surface. This is best illustrated by a gas dissolved in a beaker of water kept at a constant temperature. It will be convenient for us to characterize the water in the beaker as the liquid phase and the air above it as the gas phase. If the beaker is covered with a bell jar, as shown in Figure 5–2, some of the gas molecules (represented by the green balls) escape from the water into the surrounding enclosed air. The molecules that remain are said to be in the liquid phase; the molecules that have escaped into the air are said to be in the gas phase. As the gas molecules escape into the surrounding air, they accumulate above the water; here, random motion carries some of them back into the water. Eventually, a point is reached at which the number of molecules leaving the water is equal to the number returning. At this time, the liquid and gas phases are in equilibrium. If the temperature of the water is increased, the equilibrium state readjusts itself to a point at which more gas molecules move into the gas phase.
This behavior was first observed in 1803 by a British chemist, William Henry. His explanation of this phenomenon, known appropriately as Henry’s law, may be stated as follows: When a volatile chemical compound is dissolved in a liquid and is brought to equi- librium with air, there is a fixed ratio between the concentration of the volatile compound in air and its concentration in the liquid, and this ratio remains constant for a given temperature.
The distribution or partitioning of a gas between the liquid and gas phases is determined by the solubility of the gas in the liquid. The higher its solubility, the greater the tendency of the gas molecules to remain in the liquid phase. If two different gases are simultaneously dissolved in the same liquid, each will reach a state of equilibrium with the surrounding air independently of the other. For example, as shown in Figure 5–3, gas A (green balls) and gas B (blue balls) are both dissolved in water. At equilibrium, gas A has a greater number of molecules dissolved in the water than does gas B. This is so because
gas A is more soluble in water than gas B.
Basic Chromatographic Process Now return to the concept of chromatography. In Figures 5–2 and 5–3, both phases—liquid and gas—were kept stationary; that is, they were not moving. During a chromatographic process, this is not the case; instead, one phase is always made to move continuously in one direction over a stationary or fixed phase. For example, in Figure 5–3, showing the two gases represented by blue and green balls dissolved in water, chromatography will occur only when the air is forced to move continuously in one direction over the water. Because gas B has a greater percentage of its mol- ecules in the moving gas phase than does gas A, its molecules will travel over the liquid at a faster pace than those of gas A. Eventually, when the moving phase has advanced a reasonable distance, gas B will become entirely separated from gas A and the chromatographic process will be com- plete. This process is illustrated in Figure 5–4.
Simply, we can think of chromatography as being analogous to a race between chemical compounds. At the starting line, all the participating substances are mixed together; however, as the race progresses, materials that prefer the moving phase slowly pull ahead of those that prefer to remain in the stationary phase. Finally, at the end of the race, all the participants are separated, each crossing the finish line at different times.
The different types of chromatographic systems are as varied as the number of stationary and moving-phase combinations that can be devised. However, three chromatographic processes—gas chromatography, high-performance liquid chromatography, and thin-layer chromatography—are most applicable for solving many analytical problems in the crime laboratory.
Gas Chromatography (GC) Gas chromatography (GC) separates mixtures on the basis of their distribution between a sta- tionary liquid phase and a moving gas phase. This technique is widely used because of its ability to resolve a highly complex mixture into its components, usually within minutes.
FIGURE 5–2 Evaporation of a liquid.
FIGURE 5–3 At equilibrium, there are more gas A molecules (green balls) than gas B molecules (blue balls) in the liquid phase.
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ORGANIC ANALYSIS 125
BASIC THEORY OF GC In gas chromatography, the moving phase is actually a gas called the carrier gas, which flows through a column constructed of stainless steel or glass. The stationary phase is a thin film of liquid within the column. Two types of columns are used: the packed column and the capillary column. With the packed column, the stationary phase is a thin film of liquid that is fixed onto small granular particles packed into the column. This column is usually constructed of stainless steel or glass and is 2 to 6 meters long and about 3 millimeters in diame- ter. Capillary columns are composed of glass and are much longer than packed columns—15 to 60 meters long. These types of columns are very narrow, ranging from 0.25 to 0.75 millimeter in diameter. Capillary columns can be made narrower than packed columns because their stationary liquid phase is actually coated as a very thin film directly onto the column’s inner wall. In any case, as the carrier gas flows through the packed or capillary column, it carries with it the com- ponents of a mixture that have been injected into the column. Components with a greater affinity for the moving gas phase travel through the column more quickly than those with a greater affin- ity for the stationary liquid phase. Eventually, after the mixture has traversed the length of the column, it emerges separated into its components.
THE GC PROCESS A simplified scheme of the gas chromatograph is shown in Figure 5–5. The operation of the instrument can be summed up briefly as follows: A gas stream, the so-called carrier gas, is fed into the column at a constant rate. The carrier gas is chemically inert and is generally nitrogen or helium. The sample under investigation is injected as a liquid into a heated injection port with a syringe, where it is immediately vaporized and swept into the column by the carrier gas. The column itself is heated in an oven in order to keep the sample in a vapor state as it travels through the column. In the column, the components of the sample travel in the direction of the carrier gas flow at speeds that are determined by their distribution between the stationary and moving phases. If the analyst has selected the proper liquid phase and has made the column long enough, the components of the sample will be completely separated as they emerge from the column.
Liquid phase
Liquid phase
Direction of moving air
Stationary liquid phase
Direction of moving air
Stationary liquid phase
Direction of moving air
Stationary liquid phase
(a)
(b)
(c)
FIGURE 5–4 In this illustration of chromatography, the molecules represented by the blue balls have a greater affinity for the upper phase and hence will be pushed along at a faster rate by the moving air. Eventually, the two sets of molecules will separate from each other, completing the chromatographic process.
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126 CHAPTER 5
1
3
2
4
56
7 8
1. Sample
2. Injector
3. Carrier gas
4. Column
5. Detector
6. Power supply
7. Recorder
8. Chromatogram
FIGURE 5–5 Basic gas chromatography. Gas chromatography permits rapid separation of complex mixtures into individual compounds and allows identification and quantitative determination of each compound. As shown, a sample is introduced by a syringe (1) into a heated injection chamber (2). A constant stream of nitrogen gas (3) flows through the injector, carrying the sample into the column (4), which contains a thin film of liquid. The sample is separated in the column, and the carrier gas and separated components emerge from the column and enter the detector (5). Signals developed by the detector activate the recorder (7), which makes a permanent record of the separation by tracing a series of peaks on the chromatograph (8). The time of elution identifies the component present, and the peak area identifies the concentration. Courtesy Varian Inc., Palo Alto, Calif.
As each component emerges from the column, it enters a detector. One type of detector uses a flame to ionize the emerging chemical substance, thus generating an electrical signal. The signal is recorded onto a strip-chart recorder as a function of time. This written record of the separation is called a chromatogram. A gas chromatogram is a plot of the recorder response (vertical axis) versus time (horizontal axis). A typical chromatogram shows a series of peaks, each peak corre- sponding to one component of the mixture. The time required for a component to emerge from the column from the time of its injection into the column is known as the retention time, which is a useful identifying characteristic of a material. Figure 5–6(a) shows the chromatogram of two bar- biturates; each barbiturate has tentatively been identified by comparing its retention time to those of known barbiturates, shown in Figure 5–6(b). (See Appendix III for chromatographic condi- tions.) However, because other substances may have comparable retention times under similar chromatographic conditions, gas chromatography cannot be considered an absolute means of iden- tification. Conclusions derived from this technique must be confirmed by other testing procedures.
An added advantage of gas chromatography is that it is extremely sensitive and can yield quantitative results. The amount of substance passing through the GC detector is proportional to the peak area recorded; therefore, by chromatographing a known concentration of a material and comparing it to the unknown, the amount of the sample may be determined by proportion. Gas chromatography has sufficient sensitivity to detect and quantitate materials at the nanogram (0.000000001 gram or 1 � 10�9 gram) level.1
PYROLYSIS GC An important extension of the application of gas chromatography to forensic sci- ence is the technique of pyrolysis gas chromatography. Many solid materials commonly encountered as physical evidence—for example, paint chips, fibers, and plastics—cannot be readily dissolved in a solvent for injection into the gas chromatograph. Thus, under normal conditions these substances cannot be subjected to gas chromatographic analysis. However, materials such as these can be heated or pyrolyzed to high temperatures (500–1000°C) so that they will decompose into numerous gaseous products. Pyrolyzers permit these gaseous products to enter the carrier gas stream, where they flow into and through the GC column. The pyrolyzed material can then be characterized by the pattern pro- duced by its chromatogram or pyrogram. Figure 5–7 illustrates the pyrogram of a paint chip. The complexity of the paint pyrogram serves as a “fingerprint” of the material and gives the examiner many points to compare with other paints that are analyzed in a similar fashion.
1 Powers of 10 are quite useful and simple for handling large or small numbers. The exponent expresses the number of places the decimal point must be moved. If the exponent is positive, the decimal point is moved to the right; if it is negative, the decimal point is moved to the left. Thus, to express 1 � 10�9 as a number, the decimal point is simply moved nine places to the left of 1.
pyrolysis The decomposition of organic matter by heat
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High-Performance Liquid Chromatography (HPLC) Recall that a chromatographic system requires a moving phase and a stationary phase in contact with each other. The previous section described gas chromatography, in which the stationary phase is a thin film and the moving phase is a gas. However, by changing the nature of these phases, one can create different forms of chromatography. One form finding increasing utility in crime laboratories is high-performance liquid chromatography (HPLC). Its moving phase is a liquid that is pumped through a column filled with fine solid particles. In one form of HPLC, the
0 1 2 3 4 5 6 7 8 9 10 11 12
0 1 2 3 4 5 6 7 8 9 10 11 12
Pentobarbital
Secobarbital
TIME (MINUTES)(a)
Butabarbital
Amobarbital
Pentobarbital
Secobarbital
Phenobarbital
TIME (MINUTES)(b)
FIGURE 5–6 (a) An unknown mixture of barbiturates is identified by comparing its retention times to (b), a known mixture of barbiturates. Courtesy Varian Inc., Palo Alto, Calif.
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surfaces of these solid particles are chemically treated and act as the stationary phase. As the liq- uid moving phase is pumped through the column, a sample is injected into the column. As the liquid carries the sample through the column, different components are retarded to different degrees, depending on their interaction with the stationary phase. This leads to a separation of the different components making up the sample mixture.
The major advantage of HPLC is that the entire process takes place at room temperature. With GC, the sample must first be vaporized and made to travel through a heated column. Hence, any materials sensitive to high temperatures may not survive their passage through the column. In such situations, the analyst may turn to HPLC as the method of choice. Organic explosives are gener- ally heat sensitive and therefore more readily separated by HPLC. Likewise, heat-sensitive drugs, such as LSD, lend themselves to analysis by HPLC.
Thin-Layer Chromatography (TLC) The technique of thin-layer chromatography (TLC) uses a solid stationary phase and a moving liquid phase to separate the constituents of a mixture.
THE TLC PROCESS A thin-layer plate is prepared by coating a glass plate with a thin film of a granular material, usually silica gel or aluminum oxide. This granular material serves as the solid stationary phase and is usually held in place on the plate with a binding agent such as plaster of Paris. If the sample to be analyzed is a solid, it must first be dissolved in a suitable solvent and a few microliters of the solution spotted with a capillary tube onto the granular surface near the lower edge of the plate. A liquid sample may be applied directly to the plate in the same manner. The plate is then placed upright into a closed chamber that contains a selected liquid, with care that the liquid does not touch the sample spot.
The liquid slowly rises up the plate by capillary action. This rising liquid is the moving phase in thin-layer chromatography. As the liquid moves past the sample spot, the components of the sample become distributed between the stationary solid phase and the moving liquid phase. The components with the greatest affinity for the moving phase travel up the plate faster than
0 TIME (MINUTES)
2 4 6 8 10 12 14
FIGURE 5–7 Pyrogram of a GM automobile paint. Courtesy Varian Inc., Palo Alto, Calif.
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those that have greater affinity for the stationary phase. When the liquid front has moved a sufficient distance (usually 10 cm), the development is complete, and the plate is removed from the chamber and dried (see Figure 5–8). An example of the chromatographic separation of ink is shown in Figure 5–9.
VISUALIZING SUBSTANCES Because most compounds are colorless, no separation will be noticed after development unless the materials are visualized. To accomplish this, the plates are placed under ultraviolet light, revealing select materials that fluoresce as bright spots on a dark background. When a fluorescent dye has been incorporated into the solid phase, nonfluorescent substances appear as dark spots against a fluorescent background when exposed to the ultravio- let light. In a second method of visualization, the plate is sprayed with a chemical reagent that reacts with the separated substances and causes them to form colored spots. Figure 5–10 shows the chromatogram of a marijuana extract that has been separated into its components by TLC and visualized by having been sprayed with a chemical reagent.
Sample spot
Very thin coating of silica gel or aluminum oxide
(a) (b)
Rising solvent; original spot has separated into several spots
FIGURE 5–8 (a) In thin-layer chromatography, a liquid sample is spotted onto the granular surface of a gel-coated plate. (b) The plate is placed into a closed chamber that contains a liquid. As the liquid rises up the plate, the components of the sample distribute themselves between the coating and the moving liquid. The mixture is separated, with substances with a greater affinity for the moving liquid traveling up the plate at a faster speed.
FIGURE 5–9 (a) The liquid phase begins to move up the stationary phase. (b) Liquid moves past the ink spot carrying the ink components up the stationary phase. (c) The moving liquid has separated the ink into its several components. Courtesy Richard Megna, Fundamental Photographs, NYC
fluoresce To emit visible light when exposed to light of a shorter wavelength— that is, ultraviolet light
(a) (b) (c)
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130 CHAPTER 5
IDENTIFYING SUBSTANCES Once the components of a sample have been separated, their iden- tification must follow. For this, the questioned sample must be developed alongside an authentic or standard sample on the same TLC plate. If both the standard and the unknown travel the same distance up the plate from their origins, they can tentatively be identified as being the same. For example, suppose a sample suspected of containing heroin and quinine is chromatographed alongside known heroin and quinine standards, as shown in Figure 5–11. The identity of the sus- pect material is confirmed by comparing the migration distances of the heroin and quinine stan- dards against those of the components of the unknown material. If the distances are the same, a tentative identification can be made. However, such an identification cannot be considered definitive because numerous other substances can migrate the same distance up the plate when chromatographed under similar conditions. Thus, thin-layer chromatography alone cannot pro- vide an absolute identification; it must be used in conjunction with other testing procedures to prove absolute identity.
The distance a spot has traveled up a thin-layer plate can be assigned a numerical value known as the Rf value. This value is defined as the distance traveled by the component divided by the distance traveled by the moving liquid phase. For example, in Figure 5–11 the moving phase traveled 10 centimeters up the plate before the plate was removed from the tank. After visualization, the heroin spot moved 8 centimeters, which has an Rf value of 0.8; the quinine migrated 4 centimeters, for an Rf value of 0.4.
FIGURE 5–10 Thin-layer chromatogram of a marijuana extract. Courtesy Sirchie Finger Print Laboratories, Youngsville, N.C., www.sirchie.com
FIGURE 5–11 Chromatograms of known heroin (1) and quinine (2) standards alongside suspect sample (3).
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Thousands of possible combinations of liquid and solid phases can be chosen in thin-layer chromatography. Fortunately, years of research have produced much published data relating to the proper selection of TLC conditions for separating and identifying specific classes of substances—for example, drugs, dyes, and petroleum products. These references, along with the experience of the analyst, will aid in the proper selection of TLC conditions for specific problems.
Thin-layer chromatography is a powerful tool for solving many of the analytical prob- lems presented to the forensic scientist. The method is both rapid and sensitive; moreover, less than 100 micrograms of suspect material are required for the analysis. In addition, the equipment necessary for TLC work has minimal cost and space requirements. Importantly, numerous samples can be analyzed simultaneously on one thin-layer plate. The principal application of this technique is in the detection and identification of components in complex mixtures.
Electrophoresis Electrophoresis is somewhat related to thin-layer chromatography in that it separates materials according to their migration rates on a stationary solid phase. However, it does not use a mov- ing liquid phase to move the material; instead, an electrical potential is placed across the sta- tionary medium. The nature of this medium can vary; most forensic applications call for a starch or agar gel coated onto a glass plate. Under these conditions, only substances that possess an electrical charge migrate across the stationary phase (see Figure 5–12). The technique is partic- ularly useful for separating and identifying complex biochemical mixtures. In forensic science, electrophoresis finds its most successful application in the characterization of DNA in dried blood (see Figure 5–13).
Because many substances in blood carry an electrical charge, they can be separated and identified by electrophoresis. As shown in Figure 5–12, mixtures of DNA fragments can be sep- arated by gel electrophoresis by taking advantage of the fact that the rate of movement of DNA across a gel-coated plate depends on the molecule’s size. Smaller DNA fragments move at a faster rate along the plate than larger DNA fragments. This technique will be discussed in further detail in Chapters 10 and 11.
electrophoresis A technique for separating molecules through migration on a support medium while under the influence of an electrical potential
Power source Mixtures of DNA fragments of different sizes placed on gel-coated plate
Gel-coated plate
(a)
Power source
Electric potential applied to plate
Substances with an electrical charge migrate across plate
(b)
Power source
Completed gel
Longer fragments move more slowly
Shorter fragments move more quickly
Separated bands allow analyst to characterize DNA in dried blood
(c)
FIGURE 5–12
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visible light Colored light ranging from red to violet in the electromagnetic spectrum
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132 CHAPTER 5
Spectrophotometry We have already seen that when white light passes through a glass prism, it is dispersed into a continuous spectrum of colors. This phenomenon demonstrates that white light is not homoge- neous but is actually composed of a range of colors that extends from red through violet. Simi- larly, the observation that a substance has a color is also consistent with this description of white light. For example, when light passes through a red glass, the glass absorbs all the component col- ors of light except red, which passes through or is transmitted by the glass. Likewise, one can de- termine the color of an opaque object by observing its ability to absorb some of the component colors of light while reflecting others back to the eye. Color is thus a visual indication that ob- jects absorb certain portions of visible light and transmit or reflect others. Scientists have long recognized this phenomenon and have learned to characterize different chemical substances by the type and quantity of light they absorb.
Theory of Light To understand why materials absorb light, one must first comprehend the nature of light. Two simple models explain light’s behavior. The first model describes light as a continuous wave; the second depicts it as a stream of discrete energy particles. Together, these two very different de- scriptions explain all of the observed properties of light, but by itself, no one model can explain all the facets of the behavior of light.
LIGHT AS A WAVE The wave concept depicts light as having an up-and-down motion of a con- tinuous wave, as shown in Figure 5–14. Several terms are used to describe such a wave. The dis- tance between two consecutive crests (or one trough to the next trough) is called the wavelength; the Greek letter lambda (�) is used as its symbol, and the unit of nanometers is frequently used to express its value. The number of crests (or troughs) passing any one given point in a unit of time is defined as the frequency of the wave. Frequency is normally designated by the letter f and is expressed in cycles per second (cps). The speed of light in a vacuum is a universal constant at 300 million meters per second and is designated by the symbol c. Frequency and wavelength are inversely proportional to one another, as shown by the relationship expressed in Equation (5–1):
F � c/� (5–1)
THE ELECTROMAGNETIC SPECTRUM Actually, visible light is only a small part of a large fam- ily of radiation waves known as the electromagnetic spectrum. All electromagnetic waves travel at the speed of light (c) and are distinguishable from one another only by their different wavelengths or frequencies. (Figure 5–15 illustrates the various types of electromagnetic waves in order of decreasing frequency.) Hence, the only property that distinguishes X-rays from radio waves is the different frequencies the two types of waves possess. Similarly, the range of colors that make up the visible spectrum can be correlated with frequency. For instance, the lowest frequencies of visi-
FIGURE 5–13 DNA fragments separated by gel electrophoresis are visualized under a UV light. Courtesy Cytographics, Visuals Unlimited
frequency The number of waves that pass a given point per second
wavelength The distance between crests of adjacent waves
electromagnetic spectrum The entire range of radiation energy from the most energetic cosmic rays to the least energetic radio waves
X-ray A high-energy, short-wavelength form of electromagnetic radiation
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ble light are red; waves with a lower frequency fall into the invisible infrared (IR) region. The high- est frequencies of visible light are violet; waves with a higher frequency extend into the invisible ul- traviolet (UV) region. No definite boundaries exist between any colors or regions of the electromagnetic spectrum; instead, each region is composed of a continuous range of frequencies, each blending into the other.
Ordinarily, light in any region of the electromagnetic spectrum is a collection of waves pos- sessing a range of wavelengths. Under normal circumstances, this light comprises waves that are all out of step with each other (incoherent light). However, scientists can now produce a beam of light that has all of its waves pulsating in unison (see Figure 5–16). This is called coherent light or a laser (light amplification by the stimulated emission of radiation) beam. Light in this form is very intense and can be focused on a very small area. Laser beams can be focused to pinpoints that are so intense that they can zap microscopic holes in a diamond.
LIGHT AS A PARTICLE As long as electromagnetic radiation is moving through space, its be- havior can be described as that of a continuous wave; however, once radiation is absorbed by a substance, the model of light as a stream of discrete particles must be invoked to best describe its behavior. Here, light is depicted as consisting of energy particles that are known as photons. Each
λ
λ
FIGURE 5–14 The frequency of the lower wave is twice that of the upper wave.
Visible light
Gamma rays
High frequency Low frequency
Short wavelength Energy increases
Long wavelength
X rays Ultraviolet Infrared Microwaves Radio waves
FIGURE 5–15 The electromagnetic spectrum.
laser An acronym for light amplification by stimulated emission of radiation; light that has all its waves pulsating in unison
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photon has a definite amount of energy associated with its behavior. This energy is related to the frequency of light, as shown by Equation (5–2):
E � hf (5–2)
where E specifies the energy of the photon, f is the frequency of radiation, and h is a univer- sal constant called Planck’s constant. As shown by Equation (5–2), the energy of a photon is directly proportional to its frequency. Therefore, the photons of ultraviolet light will be more energetic than the photons of visible or infrared light, and exposure to the more energetic photons of X-rays presents more danger to human health than exposure to the photons of radio waves.
Absorption of Electromagnetic Radiation Just as a substance can absorb visible light to produce color, many of the invisible radiations of the electromagnetic spectrum are likewise absorbed. This absorption phenomenon is the basis for spectrophotometry, an important analytical technique in chemical identification. Spec- trophotometry measures the quantity of radiation that a particular material absorbs as a function of wavelength or frequency.
We have already observed in the description of color that an object does not absorb all the visible light it is exposed to; instead, it selectively absorbs some frequencies and reflects or trans- mits others. Similarly, the absorption of other types of electromagnetic radiation by chemical sub- stances is also selective. These key questions must be asked: Why does a particular substance absorb only at certain frequencies and not at others? And are these frequencies predictable? The answers are not simple. Scientists find it difficult to predict with certainty all the frequencies at which any one substance will absorb in a particular region of the electromagnetic spectrum. What is known, however, is that a chemical substance absorbs photons of radiation with a frequency that corresponds to an energy requirement of the substance, as defined by Equation (5–2). Different materials have different energy requirements and therefore absorb at different frequencies. Most important to the analyst is that these absorbed frequencies are measurable and can be used to char- acterize a material.
The selective absorption of a substance is measured by an instrument called a spectrophotometer, which produces a graph or absorption spectrum that depicts the absorption of light as a function of wavelength or frequency. The absorption of UV, visible, and IR radiation is
Coherent radiation
Incoherent radiation
FIGURE 5–16 Coherent and incoherent radiation.
photon A small packet of electromagnetic radiation energy; each photon contains a unit of energy equal to the product of Planck’s constant and the frequency of radiation: E � hf
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particularly applicable for obtaining qualitative data pertaining to the identification of organic substances.
Absorption at a single wavelength or frequency of light is not 100 percent complete— some radiation is transmitted or reflected by the material. Just how much radiation a sub- stance absorbs is defined by a fundamental relationship known as Beer’s law, shown in Equation (5–3):
A � kc (5–3)
Here, A symbolizes the absorption or the quantity of light taken up at a single frequency, c is the concentration of the absorbing material, and k is a proportionality constant. This relationship shows that the quantity of light absorbed at any frequency is directly proportional to the concen- tration of the absorbing species; the more material you have, the more radiation it will absorb. By defining the relationship between absorbance and concentration, Beer’s law permits spectropho- tometry to be used as a technique for quantification.
The Spectrophotometer The spectrophotometer measures and records the absorption spectrum of a chemical substance. The basic components of a simple spectrophotometer are the same regardless of whether it is designed to measure the absorption of UV, visible, or IR radiation. These components are illus- trated in Figure 5–17. They include (1) a radiation source, (2) a monochromator or frequency selector, (3) a sample holder, (4) a detector to convert electromagnetic radiation into an electrical signal, and (5) a recorder to produce a record of the signal.
The choice of source will vary with the type of radiation desired. For visible radiation, an ordinary tungsten bulb provides a convenient source of radiation. In the UV region, a hydrogen or deuterium discharge lamp is normally used, and a heated molded rod containing a mixture of rare-earth oxides is a good source of IR light.
The function of the monochromator is to select a single wavelength or frequency of light from the source—monochromatic light. Some inexpensive spectrophotometers pass the light through colored glass filters to remove all radiation from the beam except for a desired range of wavelengths. More precise spectrophotometers use a prism or diffraction grating to disperse radiation into its component wavelengths or frequencies.2 The desired wavelength is obtained when the dispersed radiation is focused onto a narrow slit that permits only selected wavelengths to pass through.
Most laboratory infrared spectrophotometers use Fourier transform analysis to measure the wavelengths of light at which a material will absorb in the infrared spectrum. This approach does not use any dispersive elements that select single wavelengths or frequencies of light emitted from a source; instead, the heart of a Fourier transform infrared (FT-IR) spectrometer is the Michelson interferometer. The interferometer uses a beam-splitting prism and two mirrors, one movable and one stationary, to direct light toward a sample. As the wavelengths pass through the sample and reach a detector, they are all measured simultaneously. A mathematical opera- tion, the Fourier transform method, is used to decode the measured signals and record the wavelength data. These Fourier calculations are rapidly carried out by a computer. In a matter of seconds, a computer-operated FT-IR instrument can produce an infrared absorption pattern compatible to one generated by a prism instrument.
Sample preparation varies with the type of radiation being studied. Absorption spectra in the UV and visible regions are usually obtained from samples that have been dissolved in an appro- priate solvent. Because the cells holding the solution must be transparent to the light being measured, glass cells are used in the visible region and quartz cells in the ultraviolet region. Prac- tically all substances absorb in some region of the IR spectrum, so sampling techniques must be modified to measure absorption in this spectral region; special cells made out of sodium chloride or potassium bromide are commonly used because they will not absorb light over a wide range of the IR portion of the electromagnetic spectrum.
monochromatic light Light having a single wavelength or frequency
monochromator A device for isolating individual wavelengths or frequencies of light
2A diffraction grating is made by scratching thousands of parallel lines on a transparent surface such as glass. As light passes through the narrow spacings between the lines, it spreads out and produces a spectrum similar to that formed by a prism.IS
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Detector RecorderRadiation source(a) Monochromator
Prism disperses radiation into component wavelengths
Prism
Sample cell
Slit
FIGURE 5–17 Parts of a simple spectrophotometer.
DetectorRadiation source(b) Monochromator
Prism
Sample cell
Slit
Recorder
Slit allows only selected wavelengths or frequencies of radiation to pass through
DetectorRadiation source(c) Monochromator Sample cell Recorder
Prism Slit
Radiation passes through sample, which absorbs certain frequencies
Detector measures absorption of radiation by the sample and converts the radiation into an electrical signal
Radiation source
(d)
Monochromator Sample cell
Recorder
Prism Slit
DetectorRadiation source
(e)
Monochromator
Prism
Sample cell
Slit
Recorder
Recorder translates electrical signal into recording of the absorption spectrum
The absorption spectrum of a chemical substance allows spectrophotometry to be used for identification.
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The detector measures the quantity of radiation that passes through the sample by converting it to an electrical signal. UV and visible spectrophotometers employ photoelectric tube detectors. A signal is generated when the photons strike the tube surface to produce a current that is directly proportional to the intensity of the light transmitted through the sample. When this signal is com- pared to the intensity of light that is transmitted to the detector in the absence of an absorbing ma- terial, the absorbance of a substance can be determined at each wavelength or frequency of light selected. The signal from the detection system is then fed into a recorder, which plots absorbance as a function of wavelength or frequency. Modern spectrophotometers are designed to trace an entire absorption spectrum automatically.
Ultraviolet, Visible, and Infrared Spectrophotometry Ultraviolet and visible spectrophotometry measure the absorbance of UV and visible light as a function of wavelength or frequency. For example, the UV absorption spectrum of heroin shows a maximum absorption band at a wavelength of 278 nanometers (see Figure 5–18). This shows that the simplicity of a UV spectrum facilitates its use as a tool for determining a ma- terial’s probable identity. For instance, a white powder may have a UV spectrum comparable to heroin and therefore may be tentatively identified as such. (Fortunately, sugar and starch, common diluents of heroin, do not absorb UV light.) However, this technique will not provide a definitive result; other drugs or materials may have a UV absorption spectrum similar to that of heroin. But this lack of specificity does not diminish the value of the technique because the analyst has quickly eliminated thousands of other possible drugs from consideration and can now proceed to conduct other confirmatory tests, such as thin-layer or gas chromatography, to complete the identification.
In contrast to the simplicity of a UV spectrum, absorption in the infrared region provides a far more complex pattern. Figure 5–19 depicts the IR spectra of heroin and secobarbital. Here, the absorption bands are so numerous that each spectrum can provide enough characteristics to identify a substance specifically. Different materials always have distinctively different in- frared spectra; each IR spectrum is therefore equivalent to a “fingerprint” of that substance and no other. This technique is one of the few tests available to the forensic scientist that can be considered specific in itself for identification. The IR spectra of thousands of organic compounds have been collected, indexed, and cataloged to serve as invaluable references for identifying organic substances.
infrared Invisible short frequencies of light before red in the visible spectrum
ultraviolet Invisible long frequencies of light beyond violet in the visible spectrum
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Heroin
Ab so
rb an
ce
250 300 350 Wavelength in nanometers
FIGURE 5–18 The ultraviolet spectrum of heroin.
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Mass Spectrometry Aprevious section discussed the operation of the gas chromatograph. This instrument is one of the most important tools in a crime laboratory. Its ability to separate the components of a complex mixture is unsurpassed. However, gas chromatography (GC) does have one important drawback—its inability to produce specific identification. A forensic chemist cannot unequivocally state the identification of a substance based solely on a retention time as determined by the gas chromatograph. Fortunately, coupling the gas chromatograph to a mass spectrometer has largely overcome this problem.
The separation of a mixture’s components is first accomplished on the gas chromatograph. A di- rect connection between the GC column and the mass spectrometer then allows each component to flow into the spectrometer as it emerges from the gas chromatograph. In the mass spectrometer, the material enters a high-vacuum chamber where a beam of high-energy electrons is aimed at the sample
0.00
100.00 %T
4000 3500 3000 2500 2000 1500 1000 500 Wavenumber cm–1
FIGURE 5–19 (a) Infrared spectrum of heroin. (b) Infrared spectrum of secobarbital.
0.00
100.00 %T
4000 3500 3000 2500 2000 1500 1000 500 Wavenumber cm–1
(a)
(b)
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molecules. The electrons collide with the molecules, causing them to lose electrons and to acquire a positive charge (commonly called ions). These positively charged molecules or ions are unstable or are formed with excess energy and almost instantaneously decompose into numerous smaller frag- ments. The fragments then pass through an electric or magnetic field, where they are separated ac- cording to their masses. The unique feature of mass spectrometry is that under carefully controlled conditions, no two substances produce the same fragmentation pattern. In essence, one can think of this pattern as a “fingerprint” of the substance being examined (see Figure 5–20).
The technique thus provides a specific means for identifying a chemical structure. It is also sensitive to minute concentrations. At present, mass spectrometry finds its widest application in the identification of drugs; however, further research is expected to yield significant applications for identifying other types of physical evidence. Figure 5–21 illustrates the mass spectra of heroin
ion An atom or molecule bearing a positive or negative charge
D
C
B
A
A B
C
D
Chromatogram Spectra
Separation Identification
GC MS
FIGURE 5–20 How GC/MS works. Left to right, the sample is separated into its components by the gas chromatograph, and then the components are ionized and identified by characteristic fragmentation patterns of the spectra produced by the mass spectrometer. Courtesy Agilent Technologies, Inc., Palo Alto, Calif.
43
94 146
204 215
268
327
369
100 200 300 Mass/charge
(a)
Ab un
da nc
e
42
122 150
182
272
82
303
100 150 300 Mass/charge
(b)
Ab un
da nc
e
25020050
FIGURE 5–21 (a) Mass spectrum of heroin. (b) Mass spectrum of cocaine.
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and cocaine; each line represents a fragment of a different mass (actually the ratio of mass to charge), and the line height reflects the relative abundance of each fragment. Note how different the fragmentation patterns of heroin and cocaine are. Each mass spectrum is unique to each drug and therefore serves as a specific test for identifying it.
The combination of the gas chromatograph and mass spectrometer is further enhanced when a computer is added to the system. The integrated gas chromatograph/mass spectrometer/computer system provides the ultimate in speed, accuracy, and sensitivity. With the ability to record and store in its memory several hundred mass spectra, such a system can detect and identify substances pres- ent in only one-millionth-of-a-gram quantities. Furthermore, the computer can be programmed to compare an unknown spectrum against a comprehensive library of mass spectra stored in its mem- ory. The advent of personal computers and microcircuitry has made it possible to design mass spec- trometer systems that can fit on a small table. Such a unit is pictured in Figure 5–22. Research-grade mass spectrometers are found in laboratories as larger floor-model units (see Figure 5–23).
WEBEXTRA 5.5 Watch an Animation of a Mass Spectrometer http://www.mycrimekit.com
1. Injection port 3. Ion source
4. Quadrupole 6. Data system
5. Detector2. GC column
FIGURE 5–22 A tabletop mass spectrometer. (1) The sample is injected into a heated inlet port, and a carrier gas sweeps it into the column. (2) The GC column separates the mixture into its components. (3) In the ion source, a filament wire emits electrons that strike the sample molecules, causing them to fragment as they leave the GC column. (4) The quadrupole, consisting of four rods, separates the fragments according to their mass. (5) The detector counts the fragments passing through the quadrupole. The signal is small and must be amplified. (6) The data system is responsible for total control of the entire GC/MS system. It detects and measures the abundance of each fragment and displays the mass spectrum. Courtesy Agilent Technologies, Inc., Palo Alto, Calif.
FIGURE 5–23 A scientist injecting a sample into a research- grade mass spectrometer. Courtesy Geoff Tompkinson/Science Photo Library, Photo Researchers, Inc.
Virtual Forensics Lab
Thin-Layer Chromatography of Ink To perform a virtual thin-layer chromatography lab, go to www. pearsoncustom.com/us/vlm/
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ORGANIC ANALYSIS 141
The proper selection of analytical techniques that will allow the forensic scientist to identify or compare matter can best be un- derstood by categorizing all substances into one of two broad groups: organics and inorganics. In general, organic substances contain carbon. Inorganic materials encompass all other known chemical substances. Another consideration in selecting an an- alytical technique is the need for either a qualitative or a quan- titative determination. The former relates just to the identity of the material, whereas the latter requires the determination of the percentage composition of the components of a mixture.
Chromatography, spectrophotometry, and mass spectrome- try are all readily used by a forensic scientist to identify or compare organic materials. Chromatography is a means of sep- arating and tentatively identifying the components of a mixture. Spectrophotometry is the study of the absorption of light by chemical substances. Mass spectrometry characterizes organic molecules by observing their fragmentation pattern after their collision with a beam of high-energy electrons. Gas chromatog- raphy (GC) separates mixtures on the basis of their distribution between a stationary liquid phase and a mobile gas phase. In GC, the moving phase is actually a gas called the carrier gas, which flows through a column. The stationary phase is a thin film of liquid contained within the column. After a mixture has tra- versed the length of the column, it emerges separated into its
components. The written record of this separation is called a chromatogram.Adirect connection between the GC column and the mass spectrometer allows each component to flow into the mass spectrometer as it emerges from the GC. Fragmentation of each component by high-energy electrons produces a “finger- print” pattern of the substance being examined.
Other forms of chromatography applicable to forensic science are high-performance liquid chromatography (HPLC) and thin-layer chromatography (TLC). HPLC separates com- pounds using a stationary phase and a mobile liquid phase and is used with temperature-sensitive compounds. TLC uses a solid stationary phase, usually coated onto a glass plate, and a mobile liquid phase to separate the components of the mixture. A technique analogous to TLC is electrophoresis, in which ma- terials are forced to move across a gel-coated plate under the in- fluence of an electrical potential. In this manner, substances such as proteins and DNA can be separated and characterized.
Most forensic laboratories use ultraviolet (UV) and in- frared (IR) spectrophotometers to characterize chemical com- pounds. In contrast to the simplicity of a UV spectrum, absorption in the infrared region provides a far more complex pattern. Different materials always have distinctively different infrared spectra; each IR spectrum is therefore equivalent to a “fingerprint” of that substance.
chapter summary
review questions
1. Anything that has mass and occupies space is defined as ___________.
2. The basic building blocks of all substances are the ___________.
3. The number of elements known today is ___________.
4. An arrangement of elements by similar chemical prop- erties is accomplished in the ___________ table.
5. A(n) ___________ is the smallest particle of an element that can exist.
6. Substances composed of two or more elements are called ___________.
7. A(n) ___________ is the smallest unit of a compound formed by the union of two or more atoms.
8. The physical state that retains a definite shape and vol- ume is a(n) ___________.
9. A gas (has, has no) definite shape or volume.
10. During the process of ___________, solids go directly to the gaseous state, bypassing the liquid state.
11. The attraction forces between the molecules of a liquid are (greater, less) than those in a solid.
12. Different ___________ are separated by definite visible boundaries.
13. Carbon-containing substances are classified as ___________.
14. ___________ substances encompass all non-carbon- containing materials.
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142 CHAPTER 5
15. A(n) ___________ analysis describes the identity of a material, and a(n) ___________ analysis relates to a determination of the quantity of a substance.
16. The study of the absorption of light by chemical substances is known as ___________.
17. A mixture’s components can be separated by the tech- nique of ___________.
18. True or False: Henry’s law describes the distribution of a volatile chemical compound between its liquid and gas phases. ___________
19. The (higher, lower) the solubility of a gas in a liquid, the greater its tendency to remain dissolved in that liquid.
20. True or False: In order for chromatography to occur, one phase must move continuously in one direction over a sta- tionary phase. ___________
21. A technique that separates mixtures on the basis of their distribution between a stationary liquid phase and a moving gas phase is ___________.
22. The time required for a substance to travel through the gas chromatographic column is a useful identifying characteristic known as ___________.
23. Solid materials that are not readily dissolved in solvents for injection into the gas chromatograph can be ___________ into numerous gaseous products before entering the gas chromatograph.
24. A major advantage of high-performance liquid chro- matography is that the entire process takes place at ___________ temperature.
25. A technique that uses a moving liquid phase and a sta- tionary solid phase to separate mixtures is ___________.
26. Because most chemical compounds are colorless, the fi- nal step of the thin-layer development usually requires that they be ___________ by spraying with a chemical reagent.
27. The distance a spot has traveled up a thin-layer plate can be assigned a numerical value known as the ___________ value.
28. True or False: Thin-layer chromatography yields the positive identification of a material. ___________
29. The migration of materials along a stationary phase un- der the influence of an electrical potential describes the technique of ___________.
30. True or False: Color is a usual indication that substances selectively absorb light. ___________
31. The distance between two successive identical points on a wave is known as ___________.
32. True or False: Frequency and wavelength are directly proportional to one another. ___________
33. Light, X-rays, and radio waves are all members of the ___________ spectrum.
34. Red light is (higher, lower) in frequency than violet light.
35. A beam of light that has all of its waves pulsating in uni- son is called a(n) ___________.
36. One model of light depicts it as consisting of energy par- ticles known as ___________.
37. True or False: The energy of a light particle (photon) is directly proportional to its frequency. ___________
38. Red light is (more, less) energetic than violet light.
39. The selective absorption of electromagnetic radiation by materials (can, cannot) be used as an aid for identifi- cation.
40. The amount of radiation a substance will absorb is di- rectly proportional to its concentration as defined by ___________ law.
41. The ___________ is the instrument used to measure and record the absorption spectrum of a chemical substance.
42. The function of the ___________ is to select a single frequency of light emanating from the spectrophotome- ter’s source.
43. An (ultraviolet, infrared) absorption spectrum provides a unique “fingerprint” of a chemical substance.
44. The technique of ___________ exposes molecules to a beam of high-energy electrons in order to fragment them.
45. True or False: A mass spectrum is normally considered a specific means for identifying a chemical substance. ___________
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ORGANIC ANALYSIS 143
application and critical thinking
1. Forensic drug analyst Rose Thomas receives a potential drug sample for analysis. The appearance of the powder suggests that it is adulterated and may contain more than one substance. Would spectrometry be a good analytical tool in this case? If not, what other technique could be used?
2. Because of a budget cut at the crime lab, Rose Thomas must use an analytical technique that will be relatively cheap and accommodate many samples at one time. Which chromatographic method would be best in this case? Why?
3. The figure below shows a chromatogram of a known mixture of barbiturates. Based on this figure, answer the following questions:
a. What barbiturate detected by the chromatogram had the longest retention time?
b. Which barbiturate had the shortest retention time?
c. What is the approximate retention time of amobarbital?
further references
Northrop, David, “Forensic Applications of High-Performance Liquid Chromatography and Capillary Electrophoresis,” in R. Saferstein, ed., Forensic Science Handbook, vol. 1, 2nd ed. Upper Saddle River, N.J.: Prentice Hall, 2002.
Saferstein, Richard, “Forensic Applications of Mass Spec- trometry,” in R. Saferstein, ed., Forensic Science Hand- book, vol. 1, 2nd ed. Upper Saddle River, N.J.: Prentice Hall, 2002.
Stafford, David T., “Forensic Capillary Gas Chromatogra- phy,” in R. Saferstein, ed., Forensic Science Handbook, vol. 2, 2nd ed. Upper Saddle River, N.J.: Prentice Hall, 2005.
Suzuki, Edward M., “Forensic Applications of Infrared Spec- troscopy,” in R. Saferstein, ed., Forensic Science Hand- book, Vol. 3, 2nd ed. Upper Saddle River, N.J.: Prentice Hall, 2010.
0 1 2 3 4 5 6 7 8 9 10 11 12
Butabarbital
Amobarbital
Pentobarbital
Secobarbital
Phenobarbital
TIME (MINUTES)(b)
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What Killed Napoleon?
Napoleon I, emperor of France, was sent into exile on the remote island of St. Helena by the British after his defeat at the Battle of Waterloo in 1815. St. Helena was hot, unsanitary, and rampant with disease. There, Napoleon was confined to a large reconstructed agricultural building known as Longwood House. Boredom and unhealthy living conditions gradually took their toll on Napoleon’s mental and physical state. He began suffering from severe abdominal pains and experienced swelling of the ankles and general weakness of his limbs. From the fall of 1820, Napoleon’s health began to deteriorate rapidly until death arrived on May 5, 1821. An autopsy concluded the cause of death to be stomach cancer.
It was inevitable that dying under British control, as Napoleon did, would bring with it numerous conspiratorial theories to account for his death. One of the more fascinating inquiries was conducted by a Swedish dentist, Sven Forshufvud, who systematically correlated the clinical symptoms of Napoleon’s last days to those of arsenic poisoning. For Forshufvud, the key to unlocking the cause of Napoleon’s death rested with Napoleon’s hair. Forshufvud arranged to have Napoleon’s hair measured for arsenic content by neutron activation analysis and
found it consistent with arsenic poisoning over a lengthy period of time. Nevertheless, the cause of Napoleon’s demise is still a
matter for debate and speculation. Other Napoleon hairs collected in 1805 and 1814 have also shown high concentrations of arsenic, giving rise to the speculation that Napoleon was
innocently exposed to arsenic. Even hair collected from Napoleon’s three sisters, son, and first wife show significant levels of arsenic. Some question whether Napoleon even had clinical symptoms associated with arsenic poisoning. In truth, forensic science may never be able to answer the question “What killed Napoleon?”
headline news
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After studying this chapter you should be able to: • Describe the usefulness of trace elements for forensic
comparison of various types of physical evidence
• Distinguish continuous and line emission spectra
• Understand the parts of a simple emission spectrograph
• List the parts of a simple atomic absorption spectrophotometer
• Define and distinguish protons, neutrons, and electrons
• Define and distinguish atomic number and atomic mass number
• Appreciate the phenomenon of how an atom absorbs and releases energy in the form of light
• Explain the concept of an isotope
• Understand how elements can be made radioactive
• Describe why an X-ray diffraction pattern is useful for chemical identification
inorganic analysis
alpha particle atomic mass atomic number beta particle continuous spectrum electron electron orbital emission spectrum excited state gamma ray isotope line spectrum neutron nucleus proton radioactivity X-ray diffraction
KEY TERMS
chapter 6 Le
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ng O
b je
ct iv
es > > > > > > > > > > > >
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146 CHAPTER 6
TABLE 6–1 Elemental Abundances as Percentages in the Earth’s Crust
Element Percentage by Weight
Oxygen 47.3 Silicon 27.7 Aluminum 7.9 Iron 4.5 Calcium 3.5 Sodium 2.5 Potassium 2.5 Magnesium 2.2 Titanium 0.5 Hydrogen 0.2 Other elements 1.2
Inorganics as Forensic Evidence In the previous chapter, analytical techniques were described for characterizing a class of matter known as organics. Generally, these materials contain carbon. Although organic substances con- stitute a substantial portion of the physical evidence submitted to crime laboratories, carbon does not appear among the earth’s most abundant elements. Surprisingly, about three-quarters of the weight of the earth’s crust is composed of only two elements—oxygen and silicon. In fact, only ten elements make up approximately 99 percent of the earth’s crust (see Table 6–1). The remain- ing elements may almost be considered impurities, although exceedingly important ones. Carbon, the element that is a constituent of most chemical compounds, constitutes less than 0.1 percent of the earth’s crust.
Considering these facts, it is certainly reasonable that non-carbon-containing substances—that is, inorganics—are encountered as physical evidence at crime scenes. One only has to consider the prevalence of metallic materials, such as iron, steel, copper, and aluminum, in our society to understand the possibilities of finding tools, coins, weapons, and metal scrapings at crime scenes.
Less well known, but perhaps almost as significant to the criminalist, is the use of inorganic chemicals as pigments in paints and dyes, the incorporation of inorganics into explosive formu- lations, and the prevalence of inorganic poisons such as mercury, lead, and arsenic.
To appreciate fully the role of inorganic analysis in forensic science, we must first examine its application to the basic objectives of the crime laboratory—identification and comparison of physical evidence. Identification of inorganic evidence is exemplified by a typical request to ex- amine an explosive formulation suspected of containing potassium chlorate, or perhaps to exam- ine a poisonous powder thought to be arsenic. In each case, the forensic scientist must perform tests that will ultimately determine the specific chemical identity of the suspect materials to the ex- clusion of all others. Only after completing the tests and finding their results identical to previously recorded tests for a known potassium chlorate or a known arsenic can the forensic scientist draw a valid conclusion about the chemical identity of the evidence.
However, comparing two or more objects in order to ascertain their common origin presents a different problem. For example, a criminalist may be asked to determine whether a piece of brass pipe found in the possession of a suspect compares to a broken pipe found at the crime scene. The condition of the two pipes may not allow for comparison by physically fitting together any bro- ken edges. Under these circumstances, the only alternative will be to attempt a comparison through chemical analysis. It is not enough for the analyst to conclude that the pipes are alike because they are brass (an alloy of copper and zinc). After all, hundreds of thousands of brass pipes exist, a situation that is hardly conducive to proving that these two particular pipes were at one time a single unit. The examiner must go a step further to try to distinguish these pipes from all others. Although this may not be possible, a comparison of the pipes’ trace elements—that is, elements present in small quantities—will provide a meaningful criterion for at least increasing the probability that the two pipes originated from the same source.
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INORGANIC ANALYSIS 147
TABLE 6–2 Elemental Analysis of Brass Alloys
Element High-Tensile Brass
(percentage) Manganese Brass
(percentage)
Copper 57.0 58.6 Aluminum 2.8 1.7 Zinc 35.0 33.8 Manganese 2.13 1.06 Iron 1.32 0.90 Nickel 0.48 1.02 Tin 0.64 1.70 Lead 0.17 0.72 Silicon 0.08 Nil
Source: R. L. Williams, “An Evaluation of the SEM with X-Ray Microanalyzer Accessory for Forensic Work,” in O. Johari and I. Corvin, eds., Scanning Electron Microscopy/1971 (Chicago: IIT Research Institute, 1971), p. 541.
Trace Elements Considering that most of our raw materials originate from the earth’s crust, it is not surprising that they are rarely obtained in pure form; instead, they include numerous elemental impurities that usually have to be eliminated through industrial processing. However, in most cases it is not economically feasible to completely exclude all such minor impurities, especially when their presence will have no effect on the appearance or performance of the final product. For this rea- son, many manufactured products, and even most natural materials, contain small quantities of elements present in concentrations of less than 1 percent.
For the criminalist, the presence of trace elements is particularly useful because they provide “in- visible” markers that may establish the source of a material or at least provide additional points for comparison. Table 6–2 illustrates how two types of brass alloys can readily be distinguished by their elemental composition. Similarly, the comparison of trace elements present in paint or other types of metallic specimens may provide particularly meaningful data with respect to source or origin. Foren- sic investigators have examined the evidential value of trace elements present in soil, fibers, and glass, as well as in all types of metallic objects. One example of this application occurred with the exami- nation of the bullet and bullet fragments recovered after the assassination of President Kennedy.
Evidence in the Assassination of President Kennedy Ever since President Kennedy was killed in 1963, questions have lingered about whether Lee Harvey Oswald was part of a conspiracy to assassinate the president or, as the Warren Commis- sion concluded, a lone assassin. In arriving at its conclusions, the Warren Commission recon- structed the crime as follows: Oswald fired three shots from behind the president while positioned in the Texas School Book Depository building. The president was struck by two bullets, with one bullet totally missing the president’s limousine. One bullet hit the president in the back, exited his throat, and then went on to strike Governor Connally, who was sitting in a jump seat in front of the president. The bullet hit Connally first in his back, then exited his chest, struck his right wrist, and temporarily lodged in his left thigh. This bullet was later found on the governor’s stretcher at the hospital. A second bullet in the skull fatally wounded the president.
In a room at the Texas School Book Depository, a 6.5-mm Mannlicher-Carcano military rifle was found with Oswald’s palm print on it. Also found were three spent 6.5-mm Western Cartridge Co./ Mannlicher-Carcano (WCC/MC) cartridge cases. Oswald, an employee of the depository, had been seen there that morning and also a few minutes after the assassination, disappearing soon there- after. He was apprehended a few miles from the depository nearly two hours after the shooting.
Critics of the Warren Commission have long argued that evidence exists that would prove Oswald did not act alone. Eyewitness accounts and acoustical data interpreted by some experts
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148 CHAPTER 6
President John F. Kennedy, Governor John Connally of Texas, and Mrs. Jacqueline Kennedy ride through Dallas moments before the assassination. Courtesy CORBIS-NY
have been used to advocate the contention that someone else fired at the president from a region in front of the limousine (the so-called grassy knoll). Furthermore, it is argued that the Warren Commission’s reconstruction of the crime relied on the assumption that only one bullet caused both the president’s throat wound and Connally’s back wound. Critics contend that such damage would have deformed and mutilated a bullet. Instead, the recovered bullet showed some flatten- ing, no deformity, and only about 1 percent weight loss.
In 1977, at the request of the U.S. House of Representatives Select Committee on Assassi- nations, the bullet taken from Connally’s stretcher along with bullet fragments recovered from the car and various wound areas were examined for trace element levels.
Lead alloys used for the manufacture of bullets contain an assortment of trace elements. For example, antimony is often added to lead as a hardening agent; copper, bismuth, and silver are other trace elements commonly found in bullet lead. In this case, the bullet and bullet frag- ments were compared for their antimony and silver content. Previous studies had amply demonstrated that the levels of these two elements are particularly important for characterizing WCC/MC bullets. Bullet lead from this type of ammunition ranges in antimony concentration from 20 to 1,200 parts per million (ppm) and 5 to 15 ppm in silver content.
As can be seen in Table 6–3, the samples designated Q1 and Q9 (the Connally stretcher bul- let and fragments from Connally’s wrist, respectively) are indistinguishable from one another in antimony and silver content. The samples Q2; Q4, 5; and Q14 (Q4, 5 being fragments from Kennedy’s brain, and Q2 and Q14 being fragments recovered from two different areas in the car) also are indistinguishable in antimony and silver content but are different from Q1 and Q9.
The conclusions derived from studying these results are as follows:
1. There is evidence of only two bullets—one composed of 815 ppm antimony and 9.3 ppm sil- ver, the other composed of 622 ppm antimony and 8.1 ppm silver.
2. Both bullets have a composition highly consistent with WCC/MC bullet lead, although other sources cannot entirely be ruled out.
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line spectrum A type of emission spectrum showing a series of lines separated by black areas; each line represents a definite wavelength or frequency
continuous spectrum A type of emission spectrum showing a continuous band of colors all blending into one another
emission spectrum Light emitted from a source and separated into its component colors or frequencies
INORGANIC ANALYSIS 149
TABLE 6–3 Antimony and Silver Concentrations in the Kennedy Assassination Bullets
Silver (parts
per million)a
Antimony (parts
per million) Sample Description
Q1 8.8 � 0.5 833 � 9 Connally stretcher bullet Q9 9.8 � 0.5 797 � 7 Fragments from Connally’s wrist Q2 8.1 � 0.6 602 � 4 Large fragment from car Q4, 5 7.9 � 0.3 621 � 4 Fragments from Kennedy’s brain Q14 8.2 � 0.4 642 �6 Small fragments found in car
aOne part per million equals 0.0001 percent. Source: Reprinted with permission from V. P. Guinn, “JFK Assassination: Bullet Analyses,” Analytical Chemistry, 51 (1979), 484 A. Copyright 1979, American Chemical Society.
3. The bullet found on the Connally stretcher also damaged Connally’s wrist. The absence of bullet fragments from the back wounds of Kennedy and Connally prevented any effort at linking these wounds to the stretcher bullet.
None of these conclusions can totally verify the Warren Commission’s reconstruction of the assassination, but the results are at least consistent with the commission’s findings. Further, in 2003, an ABC television broadcast showed the results of a ten-year 3-D computer animation study of the events of November 22, 1963. The animation graphically showed that the bullet wounds were completely consistent with Kennedy’s and Governor Connally’s positions at the time of shooting, and that by following the bullet’s trajectory backward they could be found to have originated from a narrow cone including only a few windows of the sixth floor of the School Book Depository.
The analyses on the Kennedy assassination bullets were performed by neutron activation analysis. The remainder of this chapter describes this and other techniques currently used to examine inorganic physical evidence.
The Emission Spectrum of Elements We have already observed that organic molecules can readily be characterized by their selective absorption of ultraviolet, visible, or infrared radiation. Equally significant to the analytical chemist is the knowledge that elements also selectively absorb and emit light. These observations form the basis of two important analytical techniques designed to determine the elemental com- position of materials—emission spectroscopy and atomic absorption spectrophotometry.
Types of Spectra The statement that elements emit light should not come as a total surprise, for one need only observe the common tungsten incandescent lightbulb or the glow of a neon light to confirm this observation. When the light emitted from a bulb or from any other light source is passed through a prism, it is separated into its component colors or frequencies. The resulting display of colors is called an emission spectrum.
When sunlight or the light from an incandescent bulb is passed through a prism, we have already observed that a range of rainbow colors is produced. This emission spectrum is called a continuous spectrum because all the colors merge or blend into one another to form a continu- ous band. However, not all light sources produce such a spectrum. For example, if the light from a sodium lamp, a mercury arc lamp, or a neon light were passed through a prism, the resultant spectrum would consist not of a continuous band but of several individual colored lines separated by dark spaces. Here, each line represents a definite wavelength or frequency of light that is separate and distinct from all others present in the spectrum. This type of spectrum is called a line spectrum. Figure 6–1 shows the line spectra of three elements.
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150 CHAPTER 6
Hydrogen
Helium
Mercury
FIGURE 6–1 Some characteristic emission spectra.
Lens Prism Photographic
plate
Sample between carbon electrodes
FIGURE 6–2 Parts of a simple carbon arc emission spectrograph.
Heated matter in a solid or liquid state produces a continuous spectrum that is not very in- dicative of its composition. However, if this same matter is vaporized and “excited” by exposure to high temperature, each element present emits light composed of select frequencies that are characteristic of the element. This spectrum is in essence a “fingerprint” of an element and offers a practical method of identification. Sodium vapor, for example, always shows the same line spectrum, which differs from the spectrum of all other elements.
Carbon Arc Emission Spectrometry An emission spectrograph is an instrument used to obtain and record the line spectra of elements. Es- sentially, this instrument requires a means for vaporizing and exciting the atoms of elements so that they emit light, a means for separating this light into its component frequencies, and a means of record- ing the resultant spectrum. A simple carbon arc emission spectrograph is depicted in Figure 6–2.
The specimen under investigation is excited when it is inserted between two carbon electrodes through which a direct current arc is passed. The arc produces enough heat to vaporize and excite the specimen’s atoms. The resultant emitted light is collected by a lens and focused onto a prism that disperses it into component frequencies. The separated frequencies are then directed toward a pho- tographic plate, where they are recorded as line images. Normally, a specimen consists of numer- ous elements; hence, the typical emission spectrum contains many lines. Each element present in the spectrum can be identified when it is compared to a standard chart that shows the position of the principal spectral lines of all the elements. However, forensic analysis more commonly requires
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INORGANIC ANALYSIS 151
FIGURE 6–3 A comparison of paint chips 1 and 2 by emission spectrographic analysis. A line-for- line comparison shows that the paints have the same elemental composition.
Sample aerosol
Coil
Ions
++ ++ + +
+ ++
++ +
Rf generator
Plasma discharge
FIGURE 6–4 The creation of charged particles in the torch of an ICP discharge.
simply a rapid comparison of the elemental composition of two or more specimens. This can read- ily be accomplished when the emission spectra are matched line for line, an approach illustrated in Figure 6–3, in which the emission spectra of two paint chips are shown to be comparable.
Inductively Coupled Plasma Emission Spectrometry (ICP) Carbon arc emission spectrometry has been supplanted by inductively coupled plasma (ICP) emission spectrometry. Like the former, ICP identifies and measures elements through light en- ergy emitted by excited atoms. However, instead of using an electrical arc, the atoms are excited by placing the sample in a hot plasma torch. The torch is designed as three concentric quartz tubes through which argon gas flows. A radio frequency (RF) coil that carries a current is wrapped around the tubes. The RF current creates an intense magnetic field.
THE ICP PROCESS The process begins when a high-voltage spark is applied to the argon gas flowing through the torch. This strips some electrons from their argon atoms. These electrons are then caught and accelerated in the magnetic field such that they collide with other argon atoms, stripping off still more electrons. The collision of electrons and argon atoms continues in a chain reaction, breaking down the gas into argon atoms, argon ions, and electrons and forming an inductively coupled plasma discharge. The discharge is sustained by RF energy that is continu- ously transferred to it from the coil. The plasma discharge acts like an intense continuous flame generating extremely high temperatures in the range of 7,000–10,000°C. The sample, in the form of an aerosol, is then introduced into the hot plasma, where it collides with the energetic argon electrons generating charged particles (ions) that emit light of characteristic wavelengths corre- sponding to the identity of the elements present (see Figure 6–4).
APPLICATIONS OF ICP Two areas of forensic casework in which ICP has been applied are the identification and characterization of mutilated bullets1 and glass fragments.2 Mutilated bullets often are not suitable for traditional microscopic comparisons against an exemplar test-fired bullet. In such situations, ICP has been used to obtain an elemental profile of the questioned bullet fragment
1 R. D. Koons and J. Buscaglia, “Forensic Significance of Bullet Lead Compositions,” Journal of Forensic Sciences 50 (2005): 341.
2 S. Montero, A. L. Hobbs, T. A. French, and J. Almirall, “Elemental Analysis of Glass Fragments by ICP-MS as Evidence of Association: Analysis of a Case,” Journal of Forensic Sciences 48 (2003): 1101.
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Acetylene AirLiquid sample
Hollow cathode tube
Flame
Monochromator
Detector Recorder
FIGURE 6–5 Parts of a simple flame atomic absorption spectrophotometer.
for comparison against an unfired bullet generally found in the possession of the suspect. For a num- ber of years forensic scientists have taken advantage of significant compositional differences among lead sources for the manufacture of lead-based bullets. Compositional differences in the trace ele- ments that constitute lead bullets are typically reflected in the copper, arsenic, silver, antimony, bis- muth, cadmium, and tin profiles of lead bullets. When two or more bullets have comparable elemental compositions, evidence of their similarity may be offered in a court of law.
In this respect, the comparison of lead bullets faces the same quandary as most common types of class physical evidence—how can a forensic analyst explain to a jury that such a finding has meaningful consequences to a criminal inquiry without being able to provide statistical or prob- ability data to support such a contention? Furthermore, the creation of meaningful databases to statistically define the significance of bullets compared by their elemental profiles is currently an unrealistic undertaking. Nevertheless, the significant diversity of bullet lead compositions in our population, like other class evidence such as fibers, hairs, paint, plastics, and glass, makes their chance occurrence at a crime scene and subsequent link to a defendant a highly unlikely event. However, care must be taken to avoid giving the trier of fact the impression that elemental pro- files constitute a definitive match. Given the millions of bullets produced each year, one cannot conclusively rule out the possibility of a coincidental match with a non-case-related bullet.
Atomic Absorption Spectrophotometry When an atom is vaporized, it absorbs many of the same frequencies of light that it emits in an excited state. The selective absorption of light by atoms is the basis for a technique known as atomic absorption spectrophotometry. A simple atomic absorption spectrophotometer is illus- trated in Figure 6–5.
The Spectrophotometry Process In atomic absorption spectrophotometry, the specimen is heated to a temperature that is hot enough to vaporize its atoms while leaving a substantial number of atoms in an unexcited state. Normally, the specimen is inserted into an air-acetylene flame to achieve this temperature. The vaporized atoms are then exposed to radiation emitted from a light source. The technique achieves great specificity by using as its radiation source a discharge tube made of the same element being analyzed in the speci- men. When the discharge lamp is turned on, it emits only the frequencies of light that are present in the emission spectrum of the element. Likewise, the sample absorbs these frequencies only when it contains the same element. Therefore, to determine the presence of antimony in a specimen, the atomic absorption spectrophotometer must be fitted with a discharge lamp that is constructed of an- timony. Under these conditions, the sample will absorb light only when it contains antimony.
Once the radiation has passed through the sample, a monochromator, consisting of a prism or a diffraction grating and a slit, isolates the desired radiation frequency and transmits it to a detector. The detector converts the light into an electrical signal, the intensity of which is observed on a digital recorder.
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nucleus The core of an atom containing the protons and neutrons
electron A negatively charged particle that is one of the fundamental structural units of the atom
proton A positively charged particle that is one of the basic structures in the nucleus of an atom
INORGANIC ANALYSIS 153
The absorption of light by the element of interest is the phenomenon that is being measured in atomic absorption spectrophotometry. The concentration of the absorbing element is directly pro- portional to the quantity of the light absorbed. The higher the concentration of the element, the more light is absorbed. For this reason, atomic absorption spectroscopy is most useful for accurately determining an element’s concentration in a sample. Furthermore, the technique is sufficiently sen- sitive to find wide application in detecting and quantitating elements that are present at trace levels. However, the technique does have one drawback in that the analyst can determine only one element at a time, each time having to select the proper lamp to match the element under investigation.
Applications of Spectrophotometry Although atomic absorption spectrophotometry has been used for chemical analysis since 1955, it has not yet found wide application for solving forensic problems. However, a modification in the design of the instrument promises to change this situation. By substituting a heated graphite furnace or a heated strip of metal (tantalum) for the flame, analysts have achieved a more efficient means of atomic volatilization and as a result have substantially increased the sensitivity of the technique. Many elements can now be detected at levels that approach one-trillionth of a gram.
The high sensitivity of “flameless” atomic absorption now equals or surpasses that of most known analytical procedures. Considering the relative simplicity and low cost of the technique, atomic absorption spectrophotometry has become an attractive method for detecting and meas- uring the smallest levels of trace elements present in physical evidence.
The Origin of Emission and Absorption Spectra Any proposed theory that attempts to explain the origin of emission and absorption spectra must relate to the fundamental structure of the element—the atom. Scientists now know that the atom is composed of even more elementary particles that are collectively known as subatomic parti- cles. The most important subatomic particles are the proton, electron, and neutron. The masses of the proton and neutron are each about 1,837 times the mass of an electron. The proton has a positive electrical charge; the electron has a negative charge equal in magnitude to that of the proton; and the neutron is a neutral particle having neither a positive nor a negative charge. The properties of the proton, neutron, and electron are summarized in the following table:
3 Actually, the electrons are moving so rapidly around the nucleus as to best be visualized as being in the form of an electron cloud spread out over the surface of the atom.
neutron A particle with no electrical charge that is one of the basic structures in the nucleus of an atom
Particle Symbol Relative Mass Electrical Charge
Proton P 1 �1 Neutron n 1 0 Electron e 1/1,837 �1
Atomic Structure A popular descriptive model of the atom, and the one that will be adopted for the purpose of this discussion, pictures an atom as consisting of electrons orbiting around a central nucleus—an image that is analogous to our solar system, in which the planets revolve around the sun.3 The nucleus of the atom is composed of positively charged protons and neutrons that have no charge. Because the atom has no net electrical charge, the number of protons must always be equal to the number of negatively charged electrons in orbit around the nucleus.
With this knowledge, we can now begin to describe the atomic structure of the elements; for example, hydrogen has a nucleus consisting of one proton and no neutrons, and it has one orbiting electron. Helium has a nucleus comprising two protons and two neutrons, with two electrons in orbit around the nucleus (see Figure 6–6).
The behavior and properties that distinguish one element from another must be related to the dif- ferences in the atomic structure of each element. One such distinction is that each element possesses
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excited state The state in which an atom absorbs energy and an electron moves from a lower to a higher energy level
atomic number The number of protons in the nucleus of an atom; each element has its own unique atomic number
154 CHAPTER 6
(a) (b)
FIGURE 6–7 (a) The absorption of light by an atom, causing an electron to jump into a higher orbital. (b) The emission of light by an atom, caused by an electron falling back to a lower orbital.
a different number of protons. This number is called the atomic number of the element. As we look back at the periodic table illustrated in Figure 5–1, we see that the elements are numbered consecu- tively. Those numbers represent the atomic number or number of protons associated with each ele- ment. An element is therefore a collection of atoms that all have the same number of protons. Thus, each atom of hydrogen has one and only one proton, each atom of helium has 2 protons, each atom of silver has 47 protons, and each atom of lead has 82 protons in its nucleus.
Electron Orbitals To explain the origin of atomic spectra, our attention must now focus on the electron orbitals of the atom. As electrons move around the nucleus, they are confined to a path from which they can- not stray. This orbital path is associated with a definite amount of energy and is therefore called an energy level. Each element has its own set of characteristic energy levels at varying distances from the nucleus. Some levels are occupied by electrons; others are empty.
An atom is in its most stable state when all of its electrons are positioned in their lowest possi- ble energy orbitals in the atom. When an atom absorbs energy, such as heat or light, its electrons are pushed into higher-energy orbitals. In this condition, the atom is in an excited state. However, be- cause energy levels have fixed values, only a definite amount of energy can be absorbed in moving an electron from one level to another. This is a most important observation, for it means that atoms absorb only a definite value of energy, and all other energy values will be excluded. In atomic ab- sorption spectrophotometry, a photon of light interacts with an electron, causing it to jump into a higher orbital, as shown in Figure 6–7(a). A specific frequency of light is required to cause this tran- sition, and its energy must correspond to the exact energy difference between the two orbitals in- volved in the transition. This energy difference is expressed by the relationship E � hf, where E represents the energy difference between the two orbitals, f is the frequency of absorbed light, and h is a universal constant called Planck’s constant. Any energy value that is more or less than this dif- ference will not produce the transition. Hence, an element is selective in the frequency of light it will absorb, and this selectivity is determined by the electron energy levels each element possesses.
In the same manner, if atoms are exposed to intense heat, enough energy is generated to push electrons into unoccupied higher-energy orbitals. Normally, the electron does not remain in this excited state for long, and it quickly falls back to its original energy level. As the electron falls back, it releases energy. An emission spectrum testifies to the fact that this energy loss comes about in the form of light emission [see Figure 6–7(b)]. The frequency of light emitted is again determined by the relationship E � hf, where E is the energy difference between the upper and lower energy levels and f is the frequency of emitted light. Because each element has its own characteristic set of energy levels, each emits a unique set of frequency values. The emission spectrum thus provides a “picture” of the energy levels that surround the nucleus of each element.
Thus, we see that as far as atoms are concerned, energy is a two-way street. Energy can be put into the atom at the same time that energy is given off; what goes in must come out. The chemist can study the atom using either approach. Atomic absorption spectrophotometry carefully measures the value and amount of light energy going into the atom; emission spectroscopy collects and measures
1P
Hydrogen
2P 2n
Helium
FIGURE 6–6 The atomic structures of hydrogen and helium.
electron orbital The path of electrons as they move around the nuclei of atoms; each orbital is associated with a particular electronic energy level
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isotope An atom differing from another atom of the same element in the number of neutrons in its nucleus
atomic mass The sum of the number of protons and neutrons in the nucleus of an atom
INORGANIC ANALYSIS 155
the various light energies given off. The result is the same: atoms are identified by the existence of characteristic energy levels.
Neutron Activation Analysis Once scientists realized that it was possible to change the number of subatomic particles in the atom’s nucleus, the unleashing of a new source of energy—nuclear energy—was inevitable. This energy has proven so awesome in its power that the survival of civilization will depend on our ability to refrain from using its destructive forces. Of course, this threat does not obscure the fact that controlled nuclear energy promises to be a source of power capable of relieving our depend- ency on the earth’s dwindling reserves of fossil fuels. For the chemist, nuclear chemistry provides a new tool for identifying and quantitating the elements.
Isotopes Until now, our discussion of subatomic particles has been limited to the proton and electron. How- ever, to understand the principles of nuclear chemistry, we must look at the other important subatomic particle, the neutron. Although the atoms of a single element must have the same number of protons, nothing prevents them from having different numbers of neutrons. The total number of protons and neutrons in a nucleus is known as the atomic mass number.
Atoms with the same number of protons but differing solely in the number of neutrons are called isotopes. For example, hydrogen consists of three isotopes; besides ordinary hydrogen, which has one proton and no neutrons, two other isotopes exist, deuterium and tritium. Deuterium (or heavy hydrogen) also has one proton but contains one neutron as well. Tritium has one pro- ton and two neutrons in its nucleus. The atomic structures of these isotopes are shown in Figure 6–8. Therefore, all the isotopes of hydrogen have an atomic number of 1 but differ in their atomic mass numbers. Hydrogen has an atomic mass number of 1, deuterium a mass of 2, and tritium a mass of 3. Ordinary hydrogen makes up 99.98 percent of all the hydrogen atoms found in nature.
Radioactivity Like hydrogen, most elements are known to have two or more isotopes. Tin, for example, has ten isotopes. Many of these isotopes are quite stable, and for all intents and purposes, the isotopes of any one element have indistinguishable properties. Others, however, are not as stable and decompose with time by a process known as radioactive decay. Radioactivity is the emission of radiation that accompanies the spontaneous disintegration of unstable nuclei. Radioactivity is actually composed of three types of radiation: alpha particles, beta particles, and gamma rays.
Alpha particles are positively charged particles, each with a mass approximately four times that of a hydrogen atom. These particles are helium atoms stripped of their orbiting electrons. Beta particles are actually electrons, and gamma rays are electromagnetic radiations similar to X-rays but of a higher frequency and energy (refer to the electromagnetic spectrum in Figure 5–15). Fortunately, most naturally occurring isotopes are not radioactive, and those that are—radium, uranium, and thorium—are found in such small quantities in the earth’s crust that their radioactivity presents no hazard to human survival.
Because of their large mass, alpha particles do not tend to travel far and are not very pene- trating; a sheet of paper or your skin easily stops them. However, radioisotopes that emit alpha
gamma ray A high-energy form of electromagnetic radiation emitted by a radioactive element
beta particle A type of radiation emitted by a radioactive element; the radiation consists of electrons
alpha particle A type of radiation emitted by a radioactive element; the radiation is composed of helium atoms minus their orbiting electrons
radioactivity The particle and/or gamma-ray radiation emitted by the unstable nucleus of some isotopes
Hydrogen Deuterium Tritium
1P 1P 1n
1P 2n
FIGURE 6–8 Isotopes of hydrogen.
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y Death by Radiation Poisoning In November 2006, Alexander V. Litvinenko lay at death’s door in a London hospital. He was in excruciating pain and had symp- toms that included hair loss, the inability to make blood cells, and gastrointestinal distress. His organs slowly failed as he lingered for three weeks and then died. British investigators soon con- firmed that Litvinenko died from the intake of polonium-210, a radioactive element, in what appeared to be its first use as a murder weapon (see Figure 1).
Litvinenko’s death almost immediately set off an interna- tional uproar. Litvinenko, a former KGB operative, had be- come a vocal critic of the Russian spy agency FSB, the domestic successor to the KGB. In 2000, he fled to London where he was granted asylum. Litvinenko continued to voice his criticisms of the Russian spy agency and also became highly critical of Russia’s president, Vladimir Putin. Just be- fore his death, he was believed to have compiled, on behalf of a British company looking to invest millions in a project in Russia, an incriminating report regarding the activities of sen- ior Kremlin officials.
Suspicions immediately fell onto Andrei Lugovoi and Dmitri Kovtun, business associates of Mr. Litvinenko. Lugovoi was himself a former KGB officer. On the day he fell ill, Litvinenko met Lugovoi and Kovtun at the Pine Bar of the Millennium Hotel in London. At the meeting, Mr. Litvinenko drank tea out of a teapot later found to be highly radioactive. British officials have accused Lugovoi of
FIGURE 1 Alexander Litvinenko, former KGB agent, before and after he became sick. (left) Courtesy AP Wide World Photos (right) Courtesy Getty Images, Inc.-Getty News
poisoning Litvinenko. The precise nature of the evidence against him has not been made clear, though investigators have linked him and Mr. Kovtun to a trail of polonium-210 radioactivity stretching from hotel rooms, restaurants, bars, and offices in London to Hamburg, Germany, and to British Airways planes that had flown to Moscow. Each man has denied killing Mr. Litvinenko.
Polonium-210 is highly radioactive and very toxic. By weight, it is about 250 million times as toxic as cyanide, so a particle the size of a dust particle could be fatal. It emits a radioactive ray known as an alpha particle. This form of radiation cannot penetrate the skin, so polonium-210 is effective as a poison only if it is swallowed, breathed in, or injected. The particles disperse through the body and first destroy fast-growing cells, like those in bone marrow, blood, hair, and the digestive tract. That would be consistent with Mr. Litvinenko’s symptoms. There is no antidote for polo- nium poisoning.
Polonium does have industrial uses and is produced by commercial or institutional nuclear reactors. Polonium-210 has been found to be ideal for making antistatic devices that remove dust from film and lenses as well as paper and textile plants. Its non-body-penetrating rays produce an electric charge on nearby air. Bits of dust with static attract the charged air, which neutralizes them. Once free of static, the dust is easy to blow or brush away. Manufacturers of such antistatic devices take great pains to make the polonium hard to remove from their products.
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rays are dangerous when ingested. The radioisotope polonium-210, an emitter of alpha particles, was recently implicated in the murder of an ex-KGB agent (see the case study below).
The existence of isotopes would be of little importance to the forensic chemist were it not for the fact that scientists have mastered the techniques for synthesizing radioactive isotopes. If the only distinction between isotopes of an element is the number of neutrons each possesses, is it not reasonable to assume that when atoms are bombarded with neutrons, some neutrons will be captured to make new isotopes? This is exactly what happens in a nuclear reactor. A nuclear reactor is simply a source of neutrons that can be used to bombard the atoms of a specimen, thereby creating radioactive isotopes. When the nucleus of an atom captures a neutron, a new iso- tope with one additional neutron is formed. In this state, the nuclei are said to be activated, and many immediately begin to decompose by emitting radioactivity.
The Process of Neutron Activation Analysis To identify the activated isotope, it is necessary to measure the energy of the gamma rays emitted as radioactivity. The gamma rays of each element can be associated with a characteristic energy value. Furthermore, once the element has been identified, its concentration can be measured by the intensity of its gamma-ray radiation; intensity is directly proportional to the concentration of the element in a specimen. The technique of bombarding specimens with neutrons and measur- ing the resultant gamma-ray radioactivity is known as neutron activation analysis. The process is depicted in Figure 6–9.
The major advantage of neutron activation analysis is that it provides a nondestructive method for identifying and quantitating trace elements. A median detection sensitivity of one- billionth of a gram (one nanogram) makes neutron activation analysis one of the most sensitive methods available for the quantitative detection of many elements. Further, neutron activation can simultaneously analyze 20 to 30 elements. A major drawback to the technique is its expense
Atom
n
n
n
Neutron
Neutrons bombard specimen
Atom
n
n
Neutron
Energy
In te
ns ity
Energy
In te
ns ity
Energy
In te
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Detector measures the energies and intensities of the gamma rays
Multichannel analyzer
Each element is associated with a characteristic energy value. Intensity indicates the element concentration in the specimen
Atom
Gamma Rays
Gamma Rays
FIGURE 6–9 The neutron activation process requires the capture of a neutron by the nucleus of an atom. The new atom is now radioactive and emits gamma rays. A detector permits identification of the radioactive atoms present by measuring the energies and intensities of the gamma rays emitted.
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TABLE 6–4 Concentration of Trace Elements in Copper Wire
Selenium Gold Antimony Silver
Control Wire
A1 2.4 0.047 0.16 12.7 A2 3.5 0.064 0.27 17.2 A3 2.6 0.050 0.20 13.3 A4 1.9 0.034 0.21 12.6
Suspect Wire
B 2.3 0.042 0.15 13.0
Note: Average concentration measured in parts per million.
Source: R. K. H. Chan, “Identification of Single-Stranded Copper Wires by Nondestructive Neutron Activation Analysis,” Journal of Forensic Sciences 17 (1972), 93. Reprinted by permission of the American Society for Testing and Materials, copyright 1972.
and regulatory requirements. Only a handful of crime laboratories worldwide have access to a nuclear reactor; in addition, sophisticated analyzers are needed to detect and discriminate gamma-ray emissions.
Applications of Neutron Activation Analysis As far as forensic analysis is concerned, neutron activation has been used to characterize trace el- ements present in metals, drugs, paint, soil, gunpowder residues, and hair. A typical illustration of its application occurred during the investigation of a theft of copper telegraphic wires in Canada. Four lengths of copper wire (A1, A2, A3, A4) found at the scene of the theft were compared by neu- tron activation with a length of copper wire (B) seized at a scrap yard and suspected of being stolen. All were bare, single-strand wire with the same general physical appearance and a diameter of 0.28 centimeter. Prior experiments had revealed that significant variations could be expected in the concentration levels of the trace elements selenium, gold, antimony, and silver for wires originat- ing from different sources. A comparison of these elements present in the wire involved in the theft was undertaken. After exposing the wires to neutrons in a nuclear reactor, neutron activation analysis revealed a match between A1 and B that was well within experimental error (see Table 6–4). The findings suggested a common origin of the control and suspect wires.
X-Ray Diffraction Until now, we have discussed methods for detecting and identifying the elements. Emission spec- troscopy, atomic absorption, and neutron activation analysis tell us what elements are present in a particular substance, but they do not provide any information as to how the elements are com- bined into compounds. One way to elicit this information is to aim a beam of X-rays at a crystal and study how the X-rays interact with the atoms that compose the substance under investigation. This technique is known as X-ray diffraction.
X-ray diffraction can be applied only to the study of solid, crystalline materials—that is, solids with a definite and orderly arrangement of atoms. For example, sodium chloride (common table salt), pictured in Figure 4–8, is crystalline. Fortunately, many substances, including 95 percent of all inorganic compounds, are crystalline and thus identifiable by X-ray diffraction analysis. The atoms in a crystal can be thought of as being composed of a series of parallel planes. As the X-rays penetrate the crystal, a portion of the beam is reflected by each of the atomic planes. As the reflected beams leave the crystal’s planes, they combine with one another to form a series of light and dark bands known as a diffraction pattern. Every compound produces a unique diffraction pattern, thus giving analysts a means for “fingerprinting” compounds.
A diagram depicting the X-ray diffraction process is illustrated in Figure 6–10. Diffraction patterns for potassium nitrate and potassium chlorate, two common constituents of homemade explosives, are shown in Figure 6–11. Comparing a questioned specimen with a known X-ray pattern is a rapid and specific way to prove chemical identity.
X-ray diffraction An analytical technique for identifying crystalline materials
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One drawback to X-ray diffraction is its lack of sensitivity. The technique is suitable for iden- tifying the major constituents of a mixture, but it often fails to detect the presence of substances constituting less than 5 percent of a mixture. For this reason, the forensic chemist must use more sensitive techniques—emission spectroscopy, atomic absorption, and neutron activation analy- sis—to identify trace elements that may be present.
INORGANIC ANALYSIS 159
Photographic plate
FIGURE 6–10 A beam of X-rays being reflected off the atomic planes of a crystal. The diffraction patterns that form are recorded on photographic film. These patterns are unique for each crystalline substance.
(a)
FIGURE 6–11 X-ray diffraction patterns for (a) potassium nitrate and (b) potassium chlorate.
(b)
sampling airborne particles from the country’s nuclear bomb tests. Nuclear forensics matured as a science when the Soviet empire disintegrated and concerns arose over the security of nuclear materials located in states of the former Soviet Union. Fears that these materials might fall into the hands of terrorist organizations engendered scenarios of dirty nuclear bombs attacks on the United States and other Western nations.
Nuclear forensics is becoming an increasingly important tool in the fight against illegal smuggling
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Nuclear forensics has emerged as a critical pro- fession on the forefront in the war on terrorism. Nuclear forensic scientists are responsible for developing ways to analyze nuclear materials recovered from either intercepted intact nuclear materials or postexplosion debris created as a result of a nuclear explosion. Nuclear forensics can trace its origin to the cold war era, when U.S. planes surreptitiously flew over Soviet airspace
(Continued)
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> > > > > > > > > > > > > > > > > and trafficking of radiological and nuclear materi- als. These include materials intended for industrial and medical use, nuclear materials such as those produced in the nuclear fuel cycle of a nuclear power plant (see Figure 1), and much more dan- gerous nuclear materials that can be used in weapons, such as plutonium and highly enriched uranium. Since the early 1990s, more than two hun- dred cases of illicitly trafficked nuclear materials have been reported.
In the United States, Lawrence Livermore National Laboratory along with seven other Department of Energy (DOE) national laboratories have been tasked by the FBI and the Department of Homeland Security with developing the nation’s technical forensics capability for nuclear and radiological materials. Organizations such as the European Commission’s Institute for Transuranium Elements located in Karlsruhe, Germany, have extend nuclear forensic capabilities onto an inter- national scale.
A major focus of nuclear forensics is identifying signatures, which are the physical, chemical, and isotopic characteristics that distinguish one nuclear or radiological material from another. Signatures enable researchers to identify the processes used to initially create a material, which ultimately may yield clues as to the origin of the seized material.
Nuclear forensics can be performed on a broad spec- trum of substances. An example is stolen containers of uranium diverted during one of the mining, milling, conversion, enrichment, or fuel fabrication steps used to convert uranium ore to enriched fuel for nuclear power plants; uranium varies in isotopic composition and impurities according to where the uranium was mined and how it was processed. An- other example is commercial radioactive materials used in applications such as medical diagnostics and food sterilization.
Researchers analyze the material’s chemical and isotopic composition, which includes measur- ing the amounts of trace elements as well as the ratio of parent isotopes to daughter isotopes. These measurements help determine the source location and sample’s age. They also examine the material’s morphological characteristics such as shape, size, and texture. Analytical methods include electron microscopy, X-ray diffraction, and mass spectrometry. In addition, as a sample is moved from place to place, it picks up trace evidence such as pollen, hairs, fibers, plant DNA, and fingerprints. These so-called route materials may provide infor- mation about who has handled a sample and the path it has traveled.
When comparing a sample’s signature against known signatures from uranium mines and fabri- cation plants, researchers can benefit by assem- bling a library of nuclear materials of known origin from around the world. Nuclear scientists have developed relationships with domestic suppliers of nuclear materials to assemble such a library. Contracts with major U.S. uranium fuel suppliers have provided researchers with samples and manufacturing data. Forensic scientists are also seeking to obtain samples of uranium products worldwide to analyze the products’ isotopic and trace-element content, grain size, and microstruc- ture. Nations with nuclear capabilities are begin- ning to share information about their nuclear fuel processes and materials. The development of databases is essential to the nuclear forensic scientist’s mission of identifying the origin of nuclear materials intercepted in the black market or associated with a terrorist event.
Nuclear Forensics (continued)
Figure 1 © Royalty-Free/CORBIS
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INORGANIC ANALYSIS 161
review questions
1. The elements ___________ and ___________ make up 75 percent of the weight of the earth’s crust.
2. Only ___________ elements make up about 99 percent of the weight of the earth’s crust.
3. The presence of ___________ elements in materials pro- vides useful “invisible” markers when comparing phys- ical evidence.
4. The knowledge that elements selectively ___________ and ___________ light provides the basis for important analytical techniques designed to detect the presence of elements in materials.
5. A(n) ___________ is a display of colors or frequencies emitted from a light source.
6. True or False: A continuous spectrum consists of a blend- ing of colors. ___________
7. A(n) ___________ spectrum shows distinct frequencies or wavelengths of light.
8. A line spectrum of an element (is, is not) characteristic of the element.
9. True or False: Matter in a solid or liquid state pro- duces an emission spectrum that is characteristic of its composition. ___________
10. The ___________ is an instrument used to obtain and record the line spectrum of elements.
11. Excitation of a specimen can be accomplished when it is inserted between two ___________ electrodes.
12. The selective absorption of light by atoms is the basis for a technique known as ___________.
13. The composition of the discharge lamp (does, does not) have to be taken into consideration when per- forming an analysis by atomic absorption for a partic- ular element.
14. True or False: One advantage of atomic absorption analysis is that it can simultaneously detect 20 to 30 elements. ___________
15. Three important subatomic particles of the atom are the ___________, ___________, and ___________.
chapter summary
Inorganic substances are encountered by forensic scientists as tools, explosives, poisons, and metal scrapings as well as trace components in paints and dyes. Many manufactured products and even most natural materials contain small quantities of elements in concentrations of less than 1 percent. For the crim- inalist, the presence of these trace elements is particularly use- ful because they provide “invisible” markers that may establish the source of a material or at least provide additional points for comparison.
Emission spectroscopy, inductively coupled plasma, and atomic absorption spectrophotometry are three techniques available to forensic scientists for determining the elemental composition of materials. An emission spectrograph vaporizes and heats samples to a high temperature so that the atoms pres- ent in the material achieve an “excited” state. Under these cir- cumstances, the excited atoms emit light. If the light is separated into its components, one observes a line spectrum. Each element present in the spectrum can be identified by its characteristic line frequencies. In inductively coupled plasma, the sample, in the form of an aerosol, is introduced into a hot plasma, creating charged particles that emit light of characteristic wavelengths corresponding to the identity of the elements present.
In atomic absorption spectrophotometry, the specimen is heated to a temperature that is hot enough to vaporize its atoms while leaving a substantial number of atoms in an unexcited state. The vaporized atoms are then exposed to radiation emitted from a light source specific for a particular element. If the element is present in the material under investigation, a portion of the light is absorbed by the substance. In this manner, many elements can be detected at levels that ap- proach one-trillionth of a gram. Neutron activation analysis measures the gamma-ray frequencies of specimens that have been bombarded with neutrons. This method provides a highly sensitive and nondestructive analysis for simultaneously iden- tifying and quantitating 20 to 30 trace elements. Because this technique requires access to a nuclear reactor, however, it has limited value to forensic analysis.
X-ray diffraction is used to study solid, crystalline materi- als. As the X-rays penetrate the crystal, a portion of the beam is reflected by each atomic plane. As the reflected beams leave the crystal’s planes, they combine with one another to form a series of light and dark bands known as a diffraction pattern. Every compound produces a unique diffraction pattern, thus giving analysts a means for “fingerprinting” inorganic compounds.
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, Tenth Edition, by Richard Saferstein. Published by Prentice Hall. Copyright © 2011 by Pearson Education, Inc.
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162 CHAPTER 6
application and critical thinking
1. A forensic analyst at the local crime lab receives pieces of a disfigured bullet from a crime scene. He or she then obtains an exemplar bullet fired by the firearms analyst from the suspect’s firearm. What is the next step in analysis?
2. Only a handful of crime laboratories worldwide have ac- cess to a nuclear reactor to carry out neutron activation analysis. What are some possible reasons why this is so?
3. If a forensic analyst wanted to analyze a particular sam- ple for the presence of trace amounts of an inorganic sub- stance, would X-ray diffraction be a suitable analytical tool? Why or why not?
further references
Forensic Analysis: Weighing Bullet Lead Evidence. Washington, D.C.: National Academies Press, 2004.
Guinn, V. P., “The Elemental Comparison of Bullet-Lead Evidence Specimens,” in S. M. Gerber, ed., Chemistry and Crime. Washington, D.C.: American Chemical Society, 1983.
Houck, Max M., ed., Mute Witnesses: Trace Evidence Analy- sis. Burlington, Mass.: Elsevier Academic Press, 2001.
Houck, Max M., ed., Trace Evidence Analysis—More Cases in Mute Witnesses. Burlington, Mass.: Elsevier Academic Press, 2004.
Settle, F. A., ed., Handbook of Instrumental Techniques for Analytical Chemistry. Upper Saddle River, N.J.: Prentice Hall, 1998.
16. The proton and electron (are, are not) of approximately equal mass.
17. A proton imparts the nucleus of an atom with a ___________ charge.
18. The number of protons (is, is not) always equal to the number of electrons in orbit around the nucleus of an atom.
19. Each atom of the same element always has the same number of ___________ in its nucleus.


