For an ideal gas, we have \begin{align} pV = Nk_B T \end{align} Considering a monatomic ideal gas specifically, the internal energy is \begin{align} U = \frac{3}{2}Nk_BT \end{align} so that \begin{align} pV = \frac{2}{3}U\quad\quad\quad \tag{1} \end{align} If we interpret the term $pV$ as "the energy a gas has due to being confined to volume $V$ at pressure $p$", then $(1)$ seems to suggest something along the lines of \begin{align} \text{"two-thirds of the internal energy of a gas is due to its being confined to volume $V$"} \tag{2} \end{align} This interpretation seems suspect to me since $\frac{3}{2}Nk_BT$ is simply the kinetic energy of the gas, and I would expect a gas to have this same internal energy regardless of whether we confine it to a finite volume or not.
My questions are as follows. Is $(2)$ a correct interpretation of the relation $(1)$? And if not, how should we interpret $(1)$?