Statistical Thermodynamics. Chapter 1: The Boltzmann Distribution.

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Derivation of the Boltzmann distribution equation for a closed system formed by non-interacting particles with constant total energy.
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Please are there more videos you made on statistical THERMODYNAMICS? I have looked for them here but I couldn't find them.

Africatv
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Thank you so much for such a detailed explanation! Your lecture is really helpful!

hallo_qing
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Very interesting system. It is greatly related to the course statistical physics.

gizachewdiga
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Can you please make videos on BE and FD distributions? This was really helpful!

anditsracist
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thank you so much ! I hope you will do a video to demonstrate that b=1/KT

linuxAF_NETLINK
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Can you continue with the last part of boltzman distribution??? Where beta is the inverse of KT

enmainbhapdahkasiej
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Find the ratio of N1/N2 in w(N1, N2) which be maximum. N1+N2=N?
Please 🙏🏻

الاستاذثائرالأسدي
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The second lecture???? I need to understand the beta!!!

coobit
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Hi. There cannot be that total energy is constant, thus you cannot ignore this assumption, there is no point to ignore it in other words. What is constant is the energy of each macrostate. Thus, lnΩ or lnW should be lnW_i, where W_i is one of the macrostates. And n_k (I prefer n_j) should in reality be n_ik, where k = 0 to S-1, S is the number of energy levels. Sum(Ω_i) = Ω = (energy levels)^N

georgevendras
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Is it me or does this
actually relate to subject?
Particle in a box model

Thanks for your well produced video.

Your viewers might enjoy seeing my personal amateur science project in the visual aid linked below.

It uses a sheet of spring-like material buckled from the ends to form a Gaussian curve. This is to represents a two dimensional field with the ends bounded.

Seeing the mechanical effect may also takes some of the mystery of what the math is showing.

See the load verse deflection graph in the white paper found elsewhere on my YouTube channel.

SampleroftheMultiverse