To solve this question, we need to understand the relationships between thermodynamic variables for an ideal gas in a closed system. The variables involved here are enthalpy (\(H\)), pressure (\(P\)), temperature (\(T\)), and volume (\(V\)). Let's analyze each option:
- \((\frac{∂H}{∂V})_T=0\):
For an ideal gas, enthalpy (\(H = U + PV\)) depends only on temperature (\(T\)) because the internal energy (\(U\)) and the product (\(PV\)) both depend only on \(T\) in an ideal gas. Therefore, at constant temperature, a change in volume does not affect the enthalpy of an ideal gas, making this statement true.
- \((\frac{∂T}{∂P})_H=0\):
At constant enthalpy for an ideal gas, there is no direct dependency between temperature and pressure. The ideal gas law (\(PV=nRT\)) implies that temperature changes would require changes in pressure and volume proportionally, but under constant \(H\), any pressure change does not directly impact temperature. Hence, this relation holds true.
- \((\frac{∂H}{∂P})_T=0\):
At constant temperature for an ideal gas, enthalpy is unaffected by changes in pressure since enthalpy is only a function of temperature in this case. Thus, this relation is true.
- \((\frac{∂H}{∂T})_P=0\):
This is not valid for an ideal gas, as enthalpy (\(H = U + PV\)) does change with temperature even at constant pressure, because internal energy and the product \(PV\) both change with \(T\).
Thus, the correct relations for an ideal gas in a closed system are: \((\frac{∂H}{∂V})_T=0\), \((\frac{∂T}{∂P})_H=0\), and \((\frac{∂H}{∂P})_T=0\).