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First, the graphical representation of the most
important exponential curves. |
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The typical curves everybody should know. The
blue curve in the first quadrant (positive x values) corresponds
to the energy dependence of the ubiquitous
Boltzmann factor exp (E/kT) |
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Slightly more tricky. Note that the purple branch
in the 1. quadrant corresponds to the temperature dependence of the ubiquitous Boltzmann
factor exp (E /kT) |
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The inverted functions, e.g. y =
ln x are easily pictured, too; below the y = ln x and the y = ln
(1/x) functions are shown. |
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The graphs, in case you forgot, also illustrate
some basic algebraic relations, e.g.
- e x = 1/ex
- ln x = ln (1/x)
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The essential identities are |
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| ex |
= |
1
e x |
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(ex)y |
= |
ex · y |
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| ex ·
ey |
= |
ex + y |
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(ex)1/y |
= |
ex /y |
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ex
ey |
= |
ex y |
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eln x |
= |
x |
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| ln (x · y) |
= |
ln x + ln y |
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| ln |
x
y |
= |
ln x ln y |
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| ln xy |
= |
y · ln x |
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Here some approximations. |
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| ex |
= |
1 + |
x
1! |
+ |
x2
2! |
+ |
x3
3! |
+ .. |
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| ln (1 + x) |
= |
x |
x2
2 |
+ |
x3
3 |
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x4
4 |
+ .. |
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| ln (1 x) |
= |
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æ
è |
x + |
x2
2 |
+ |
x3
3 |
+ |
x4
4 |
+ .. |
ö
ø |
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While many equations
contain exponential terms of some variable which "disappear" if you
substitute the ln of the variable (as in the Arrhenius plot), we mostly prefer the
lg of some observable quantity to the ln. As an example, plotting
the vacancy
concentration cV in an Arrhenius plot would be
straight forward with the ln: |
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On order to get a straight slope we
have to switch to new variables according to |
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| ln cV |
= ln A |
HF
kT |
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1
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for
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For y and
x we get straight line with slope
HF/k and intercept = A |
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What do we have to do if we want to
plot lg (cV) instead of
ln (cV)? |
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We have to multiply everything with
lg e = 0,4342.., because |
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| lg x |
= |
(lg e) · (ln x) |
1) |
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We obtain |
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| lg (cV) |
= |
0,434 · ln A 0,434 · |
HV
k |
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1
T |
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© H. Föll (MaWi 1 Skript)