Given. A closed (no-influx), undersaturated (single liquid phase) reservoir producing entirely by rock-and-fluid expansion.
Given data
$V_p$
$1\times10^9$ res bbl
$q$
10,000 STB/day
Time produced
6 years
$p_i$
5,000 psi
$c_t$
$1\times10^{-5}$ psi$^{-1}$
$B_o$
1.4 res bbl/STB
Find. The current average reservoir pressure $\bar p$.
Approach. For a closed, undersaturated liquid reservoir, cumulative reservoir-barrel withdrawal is balanced entirely by rock+fluid expansion, giving a direct depletion material balance.
Compressibility-drive material balance. For an undersaturated, volumetric reservoir, $$N_pB_o=c_tV_p\,\Delta p\ \Rightarrow\ \Delta p=\frac{N_pB_o}{c_tV_p}$$
$$\Delta p=\frac{(21.9\times10^6)(1.4)}{(1\times10^{-5})(1\times10^9)}$$
$$\boxed{\Delta p\approx 3{,}066\text{ psi}}$$
Current average reservoir pressure.
$$\bar p=p_i-\Delta p=5{,}000-3{,}066$$
$$\boxed{\bar p\approx 1{,}934\text{ psi}}$$
This large pressure drop for a comparatively modest withdrawal (about 2.2% of the pore volume, in STB terms) illustrates why undersaturated (single-liquid-phase) reservoirs are so pressure-sensitive: with no free gas or aquifer to buffer voidage, every barrel withdrawn must come from a very small total-compressibility expansion.