Change in internal energy of an ideal gas

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The change in internal energy (ΔU) of an ideal gas can be expressed as Δ(3/2)PV, provided both initial and final pressure and volume are known. This approach allows for the determination of ΔU using a P-V diagram. However, the first law of thermodynamics, ΔU = Q + W, remains essential for calculating energy changes, heat, or work in various scenarios. In closed systems, only temperature changes affect internal energy, with isothermal processes resulting in ΔU = 0. Understanding both methods is crucial for solving thermodynamic problems effectively.
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Given that U = (3/2)PV does this mean that ΔU = Δ(3/2)PV for an ideal gas? Hence when finding the change in internal energy using a P-V diagram, can we simply apply this equation instead of using ΔU = Q+W?
 
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Yes, if you can know ##\Delta(PV)## you can know the change in internal energy. For this formula, you have to know both the initial and final pressure and volume. A more often seen version of this concept is using the other side of the ideal gas law, so that with constant N:

$$\Delta U = \frac{3}{2}Nk_T \Delta T$$

Thus, for a closed system, only a change in temperature will lead to a change in energy. Specifically, isothermal processes on ideal gases have the condition ##\Delta U =0##.

But ##\Delta U=Q+W## is the first law of Thermodynamics. It can come in very useful when you're finding either ##\Delta U## or ##Q## or ##W##. Often you will have to use this law in some form or another in many problems.
 
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