Consider a system with 1000 particles that can only have two energies, &, and &, with E, > E,. The difference between these two values is Aɛ = ɛ, -E. Assume that gi = g2 = 1. Using the equation for the Boltzmann distribution graph the number of particles, ni and n2, in states &, and &, as a function of temperature for a Aɛ = 1×102" J and for a temperature range from 2 to 300 K. (Note: kB = 1.380x10-23 J K-. n, or = e п,

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Consider a system with 1000 particles that can only have two energies, ɛ, and
with
ɛ, > E,. The difference between these two values is Aɛ = ɛ, -& . Assume that gi = g2 = 1. Using the
%3D
%3D
equation for the Boltzmann distribution graph the number of particles, ni and m, in states &
n2,
E
and
E, as a
function of temperature for a Aɛ = 1×10-2' J and for a temperature range from 2 to 300 K. (Note: kg =
1.380x10-23 J K-!.
%3D
%3D
(s,-s,)
gLe
Aɛ/
n2
or
= e
n,
Transcribed Image Text:Consider a system with 1000 particles that can only have two energies, ɛ, and with ɛ, > E,. The difference between these two values is Aɛ = ɛ, -& . Assume that gi = g2 = 1. Using the %3D %3D equation for the Boltzmann distribution graph the number of particles, ni and m, in states & n2, E and E, as a function of temperature for a Aɛ = 1×10-2' J and for a temperature range from 2 to 300 K. (Note: kg = 1.380x10-23 J K-!. %3D %3D (s,-s,) gLe Aɛ/ n2 or = e n,
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