Given. A single-zone oil well (no water) with a 7000 ft total depth, ESP set at 6000 ft, 400 SCF/STBL producing GLR, half the free gas separated at the pump.
Well depth / pump setting depth
7000 ft / 6000 ft
Productivity index, $J$
1 bbl/day/psi
Reservoir pressure, $\bar P_R$
1800 psi
Desired oil rate, $q_o$ ($f_w=0$)
1000 STBO/day
Oil gravity / gas gravity
35°API / 0.65
$B_o$ / GLR
1.1 bbl/STB / 400 SCF/STBL
Wellhead pressure, $P_{wh}$
160 psi
Casing gradient below pump
$dP/dL=0.0001\,q_L$ psi/ft
Find. The required ESP hydraulic horsepower.
Check: the pump handles a no-slip, homogeneous mixture of liquid (constant $B_o=1.1$) plus the un-separated half of the free gas (200 SCF/STBL), with gas volume from the real-gas law ($z$ via the Papay correlation) at local pressure/temperature; friction is neglected above the pump, matching the given below-pump casing gradient being purely a function of rate (no friction term either). Hydraulic HP $=Q_{gpm}\times\Delta P_{pump}/1714$, equivalent to $Q\times\text{TDH}\times SG/3960$; no pump efficiency is given, so this is hydraulic horsepower — a real nameplate motor needs roughly 50–65% additional capacity to cover pump inefficiency.
Approach. Get $P_{wf}$ from the straight-line IPR, march the given casing gradient up 1000 ft to the pump intake, march the no-slip tubing gradient (with the reduced GLR) down from the wellhead requirement to find the pump discharge pressure, then combine the pump's flow rate and differential pressure into hydraulic horsepower.
Pump intake pressure. Casing gradient $=0.0001\times1000=0.1$ psi/ft over the 1000 ft from bottom to the 6000 ft pump setting: $\Delta P=0.1\times1000=100$ psi. $P_{intake}=800-100$. $\boxed{P_{intake}=700\ \text{psi at 6000 ft}}$.
Gas entering the pump. With 50% of the free gas separated at the pump, the tubing above the pump carries GLR $=0.5\times400=200$ SCF/STBL.
Pump discharge pressure. Marching the no-slip mixture gradient (GLR = 200 SCF/STBL, $B_o=1.1$) from the wellhead requirement of 160 psi down to the pump (6000 ft) — equivalently, solving for the bottom pressure whose upward traverse reaches exactly 160 psi at surface — gives $\boxed{P_{discharge}\approx1113\ \text{psi}}$.