Why we needed to define enthelpy?

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The discussion centers on the concept of enthalpy and its relevance in thermodynamics, particularly regarding heat transfer at constant pressure. It highlights that while the change in internal energy (dU) can be expressed as dU = dq + dw, measuring internal energy directly is challenging, especially when accounting for volumetric work. The introduction of enthalpy (H = U + p·V) simplifies this by allowing the expression dH = dq at constant pressure, making it easier to measure heat changes in practical scenarios. This approach eliminates the complexities associated with varying volume during calorimetric measurements, as maintaining constant pressure is more feasible in experimental settings. Thus, enthalpy serves as a valuable term for analyzing heat transfer processes beyond just constant pressure conditions.
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If we know that at constant pressure heat absorbed or gained is path independent then what was the need for introducing this new enthalpy term.
If its answer is that it is not only for a special case in which pressure is constant then how can we even use it because we cannot measure the internal energy.
Thanks
 
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I don't understand your question. Please provide a specific problem (with actual temperatures, pressures, amounts of material, etc) that better illustrates what your issue is.
 
Hemant said:
If we know that at constant pressure heat absorbed or gained is path independent then what was the need for introducing this new enthalpy term.

The change of internal energy is dU = dq + dw. It is easy to eliminate non-volumetric work. But than you still have dU = dq - p·dV. Eliminating the volumetric work would require keeping the volume constant which is difficult in practice. That means that an accurate calorimetric measurement would always need to be accompanied by a measurement of the change in volume.

This problem is solved by the definition of enthalpy H = U + p·V. That results in dH = dU + p·dV + V·dp, without non-volumentric work in dH = dq + V·dp and under constant pressure in dH = dq. If you manage to keep the pressure constant (which is quite easy in practice) the calorimetric measurement directly gives you the change of enthalpy.
 

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