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An Expansion Process on an Ideal Diatomic Gas Has a Linear

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An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is the initial volume is and the initial temperature is The final pressure is and the final temperature is The change in the internal (thermal) energy of the gas is closest to A) -3100 J. B) -1800 J. C) 3100 J. D) 1800 J. E) 0.00 J. the initial volume is An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is the initial volume is and the initial temperature is The final pressure is and the final temperature is The change in the internal (thermal) energy of the gas is closest to A) -3100 J. B) -1800 J. C) 3100 J. D) 1800 J. E) 0.00 J. and the initial temperature is An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is the initial volume is and the initial temperature is The final pressure is and the final temperature is The change in the internal (thermal) energy of the gas is closest to A) -3100 J. B) -1800 J. C) 3100 J. D) 1800 J. E) 0.00 J. The final pressure is An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is the initial volume is and the initial temperature is The final pressure is and the final temperature is The change in the internal (thermal) energy of the gas is closest to A) -3100 J. B) -1800 J. C) 3100 J. D) 1800 J. E) 0.00 J. and the final temperature is An expansion process on an ideal diatomic gas has a linear path between the initial and final states on a pV diagram.The initial pressure is the initial volume is and the initial temperature is The final pressure is and the final temperature is The change in the internal (thermal) energy of the gas is closest to A) -3100 J. B) -1800 J. C) 3100 J. D) 1800 J. E) 0.00 J. The change in the internal (thermal) energy of the gas is closest to


A) -3100 J.
B) -1800 J.
C) 3100 J.
D) 1800 J.
E) 0.00 J.

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