A monatomic ideal gas expands in a reversibleadiabatic process. The initial temperature of the gasamounts to T¡ and the mole number is equal to n. Thefinal temperature Tf = Ti/4. Calculate the change inits volume.O a. Vf/V¡=1/8O b. Vf/Vj=1/8O c. Vf/Vj=4O d. Vf/Vj=2O e. Vi/V;=8

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A monatomic ideal gas expands in a reversible diabatic process. The initial temperature of the gas mounts to T¡ and the mole number is equal to n. The inal temperature Tf = Ti/4. Calculate the change in Is volume. O a. Vf/Vj=1/8 O b. Vf/V;=1/8 O c. Vf/V;=4 O d. Vf/Vj=2 O e. Vf/Vj=8

A monatomic ideal gas expands in a reversible diabatic process. The initial temperature of the gas mounts to T¡ and the mole number is equal to n. The inal temperature Tf = Ti/4. Calculate the change in Is volume. O a. Vf/Vj=1/8 O b. Vf/V;=1/8 O c. Vf/V;=4 O d. Vf/Vj=2 O e. Vf/Vj=8

College Physics

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ISBN:9781305952300

Author:Raymond A. Serway, Chris Vuille

Publisher:Raymond A. Serway, Chris Vuille

Chapter1: Units, Trigonometry. And Vectors

Section: Chapter Questions

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Concept explainers

Maxwell speed distribution

Maxwell-Boltzmann distribution or commonly known as Maxwell speed distribution, explains the division of the energy levels of the molecules of an ideal gas on the basis of the statistical theory. In 1859, Scottish physicist James Clerk Maxwell established the context for the distribution of molecular velocities for random molecules moving in a closed environment. This theory was generalized in 1871 by German physicist Ludwig Boltzmann. He improvised the theory to express the distribution of energy levels among different molecules.

Question

A monatomic ideal gas expands in a reversible
adiabatic process. The initial temperature of the gas
amounts to T¡ and the mole number is equal to n. The
final temperature Tf = Ti/4. Calculate the change in
its volume.
O a. Vf/V¡=1/8
O b. Vf/Vj=1/8
O c. Vf/Vj=4
O d. Vf/Vj=2
O e. Vi/V;=8

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