This physics problem tests your understanding of fundamental physical laws and their applications. The step-by-step solution below breaks down the problem using relevant equations and physical reasoning.
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Here's the proof for the definitions of heat capacities at constant volume and constant pressure.
i. Prove that
Step 1: Start with the First Law of Thermodynamics. The change in internal energy () for a system is given by: where is the heat absorbed by the system and is the work done on the system. For a reversible process, the work done is . Substituting this into the First Law:
Step 2: Consider a process at constant volume. If the volume () is kept constant, then . In this case, the work done is zero (). The First Law simplifies to: where is the heat absorbed at constant volume.
Step 3: Define heat capacity at constant volume (). Heat capacity at constant volume is defined as the amount of heat required to raise the temperature of a substance by one degree Celsius (or Kelvin) at constant volume:
Step 4: Substitute into the definition of . Since at constant volume, we can replace with : This proves the first relation. C_V = \left[\frac{\partial E{\partial T}\right]_V}
ii. Prove that
Step 1: Start with the definition of enthalpy (). Enthalpy is defined as: where is internal energy, is pressure, and is volume. Taking the total differential of :
Step 2: Substitute from the First Law of Thermodynamics. From Step 1 of part (i), we know . Substitute this into the expression for :
Step 3: Consider a process at constant pressure. If the pressure () is kept constant, then . The expression for simplifies to: where is the heat absorbed at constant pressure.
Step 4: Define heat capacity at constant pressure (). Heat capacity at constant pressure is defined as the amount of heat required to raise the temperature of a substance by one degree Celsius (or Kelvin) at constant pressure:
Step 5: Substitute into the definition of . Since at constant pressure, we can replace with : This proves the second relation. C_P = \left[\frac{\partial H{\partial T}\right]_P}
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Here's the proof for the definitions of heat capacities at constant volume and constant pressure.
This physics problem tests your understanding of fundamental physical laws and their applications. The step-by-step solution below breaks down the problem using relevant equations and physical reasoning.