Prove that de=pdv

Physics

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de=pdv

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To prove the relationship de=pdvde = pdv, we need to consider the First Law of Thermodynamics under specific conditions and a particular sign convention for work. Here, 'e' represents the internal energy of the system, 'p' is the pressure, and 'dv' is the infinitesimal change in volume.

  1. State the First Law of Thermodynamics.

    The First Law of Thermodynamics states that the change in internal energy (dede) of a system is equal to the heat added to the system (dqdq) plus the work done on the system (dwondw_{on}).

    de=dq+dwonde = dq + dw_{on}
  2. Define work done on the system.

    For a reversible process involving a change in volume, the infinitesimal work done on the system (dwondw_{on}) by its surroundings is given by:

    dwon=pdvdw_{on} = p dv

    (Note: This convention defines work done on the system as positive. In some contexts, work done by the system is defined as dwby=pdvdw_{by} = p dv, in which case dwon=−pdvdw_{on} = -p dv.)

  3. Consider an adiabatic process.

    An adiabatic process is a thermodynamic process where no heat is exchanged between the system and its surroundings. Therefore, the infinitesimal change in heat (dqdq) is zero.

    dq=0dq = 0
  4. Substitute into the First Law.

    Substitute the expressions for dqdq and dwondw_{on} into the First Law of Thermodynamics:

    de=0+pdvde = 0 + p dv de=pdvde = p dv

    This equation holds true for a reversible adiabatic process where work done on the system is considered positive.

    The final answer is de=pdv\boxed{de = pdv}.

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