CHAPTER 14
14.1 A=εclwhere the proportionality constant εis the molar absorption co-
efficient, or extinction coefficient, the concentration of the absorber
is c, the pathlength of the sample is l, the intensity of the incident
light is I, and the intensity of the exiting light is I 0.14.2 (a)(b)(c)14.3 (a)(b)(c)14.4 (a)A=0.27(b)14.5 (a)A=0.0154(b)14.6
14.7 (a)A=cεl=(1 × 10 −^6 M)(1 × 104 M−^1 cm−^1 )(1 cm) =0.01
(b)A=cεl=(2 × 10 −^4 M)(1 × 104 M−^1 cm−^1 )(1 cm) = 214.8
14.9 w′=B′ρ[]
(, )(. ) ( )(.
Trp =11 300MM−−^11 0 239 − 1500 0 71 77
11 300 5380 1500 1960
112
)
( , )( ) ( )( )
.
MM−−−
= 8 81 10× −^5 M
[]
()(.)()(.)
Tyr =5380 MM−−^11 0 717 − 1960 0 239
(( , )( ) ( )( )
.
11 300 5380 1500 1960
11585
MM−−−
=× 10 −^5 M
cA
l==.
×
=
−
ε −−10
10 1
01
1
31 1Mcm cm mMcA
l (. )( )==.
×
=
−
ε −−10
154 10 1
6
1
41 1Mcm cm^551065
×=−^6 MM. μc
.=× =.%. %
1
27
01 0037
λ
ν==
×
×
=×
−
−c (^310) −
110
310
81
12 1ms 4
sm→infraredλ
ν==
×
×
=× →
−
−c 310
110310
81
61ms 2
smrradiowaveλ
ν==
×
×
=×
−
−c (^310) −
110
310
81
18 1ms 10
smm→X-rayν
λ==.
×
×
=×
−
−c 310
31010 10
81
2ms 10
mm→microwaveν
λ==.
×
×
=×
−
−c 310
51060 10
81
7ms 14
mm→→visibleν
λ==
×
×
=× →
−
−c 310
110310
81
9ms 17
mm X-rayANSWERS TO PROBLEMS 473
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