An ideal gas, having ratio of specific heat Υ undergoes a process in which its internal energy relates to the volume as U=α√V, where α is a constant. If the gas is expanded from volume V1 and V2. The work performed by gas is:
A
2α(Υ−1)[√V2−√V1]
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B
α(Υ−1)[√V2−√V1]
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C
2α(Υ−1)[V2−V1]
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D
α(Υ−1)[V2−V1]
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