In an adiabatic process, in the usual notation, W =(A) \(\frac{P_iV_i-P_fV_f}{\gamma-1}\)(B) \(\frac{nR∆T}\gamma\)(C) nR\(\gamma\)(Ti - Tf)(D) \(\frac{P_iV_i-P_fV_f}{\gamma}\)

In an adiabatic process, in the usual notation, W =(A) \(\frac{P_iV_i

1.	In an adiabatic process, in the usual notation, W =(A) \(\frac{P_iV_i-P_fV_f}{\gamma-1}\)(B) \(\frac{nR∆T}\gamma\)(C) nR\(\gamma\)(Ti - Tf)(D) \(\frac{P_iV_i-P_fV_f}{\gamma}\)
Answer» (A) \(\frac{P_iV_i-P_fV_f}{\gamma-1}\)

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In an adiabatic process, in the usual notation, W =(A) \(\frac{P_iV_i-P_fV_f}{\gamma-1}\)(B) \(\frac{nR∆T}\gamma\)(C) nR\(\gamma\)(Ti - Tf)(D) \(\frac{P_iV_i-P_fV_f}{\gamma}\)

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