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

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2.
Consider a system with 1000 particles that can only have two energies, &, and ɛ, with
E, > E,. The difference between these two values is Aɛ = ɛ, -&,. Assume that gi = g2 = 1. Using the
equation for the Boltzmann distribution graph the number of particles, ni and n2, in states &, and s, as a
function of temperature for a Aɛ = 1×10-2' J and for a temperature range from 2 to 300 K. (Note: kB -
1.380×10-23 JK-!.
n 8.* or n
= e
n,
g;
Transcribed Image Text:2. Consider a system with 1000 particles that can only have two energies, &, and ɛ, with E, > E,. The difference between these two values is Aɛ = ɛ, -&,. Assume that gi = g2 = 1. Using the equation for the Boltzmann distribution graph the number of particles, ni and n2, in states &, and s, as a function of temperature for a Aɛ = 1×10-2' J and for a temperature range from 2 to 300 K. (Note: kB - 1.380×10-23 JK-!. n 8.* or n = e n, g;
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