ESP Motor and Cable Sizing - Horsepower, Amperage, and Voltage Drop

Overview

The motor and cable are the power delivery system for an ESP installation. The motor must provide sufficient horsepower to drive the pump at the required brake horsepower, and the cable must deliver adequate voltage and current from the surface to the motor without excessive losses.

Undersized motors lead to overloading, overheating, and premature failure. Undersized cables cause excessive voltage drop, reduced motor performance, and wasted energy. Both components must be sized together as part of an integrated electrical system design.


Motor Horsepower Requirements

Required Motor HP

The motor must deliver at least the brake horsepower demanded by the pump:

HPrequired=BHPpumpηmotor+HPprotectorHP_{required} = \frac{BHP_{pump}}{\eta_{motor}} + HP_{protector}

Where:

  • BHPpumpBHP_{pump} = brake horsepower required by the pump
  • ηmotor\eta_{motor} = motor efficiency (typically 0.80 to 0.92)
  • HPprotectorHP_{protector} = power consumed by the seal/protector section (typically 2-10 HP)

In most practical designs, the protector losses are small relative to the pump BHP and are accounted for in the motor selection margin.

Brake Horsepower from Pump

The pump BHP depends on the number of stages, flow rate, and fluid properties:

BHPpump=Nstages×BHPstage(Q)×SGfBHP_{pump} = N_{stages} \times BHP_{stage}(Q) \times SG_f

Where BHPstage(Q)BHP_{stage}(Q) is the power consumption per stage at the operating rate (from the manufacturer's curve), and SGfSG_f is the fluid specific gravity.

Alternatively, from hydraulic horsepower and efficiency:

BHPpump=Q×TDH×SGf3960×ηpumpBHP_{pump} = \frac{Q \times TDH \times SG_f}{3960 \times \eta_{pump}}

Motor Selection

Motors are available in discrete nameplate HP ratings. The selected motor must satisfy:

HPnameplateHPrequiredHP_{nameplate} \geq HP_{required}

Standard ESP motor sizes (HP): 15, 20, 25, 30, 40, 50, 60, 75, 100, 125, 150, 200, 250, 300, 400, 500, 600, 750, 1000.


Motor Load Factor

Definition

The load factor is the ratio of actual shaft load to the motor's nameplate rating:

LF=BHPpumpHPnameplateLF = \frac{BHP_{pump}}{HP_{nameplate}}

Load Factor Guidelines

Load Factor Status Consequence
< 0.70 Underloaded Reduced motor efficiency, higher unit cost
0.70 - 0.90 Optimal Good efficiency and reliability
0.90 - 1.00 Fully loaded Maximum efficiency, minimal margin
1.00 - 1.10 Overloaded (service factor) Acceptable short-term, reduced life
> 1.10 Severely overloaded Not recommended, rapid overheating

Most ESP motors have a service factor of 1.0 to 1.15, meaning they can sustain 100-115% of nameplate HP under certain conditions. However, operating above nameplate reduces motor life due to increased winding temperature.

Temperature and Load

Motor winding temperature rise is approximately proportional to the square of the load:

ΔTLF2\Delta T \propto LF^2

A motor at 110% load generates approximately 21% more heat than at 100% load, significantly reducing insulation life.


Motor Amperage

Nameplate Current

ESP motors are rated at a specific voltage and amperage at full load. The relationship between power, voltage, and current for a three-phase motor:

HP=3×Vmotor×Imotor×PF×ηmotor746HP = \frac{\sqrt{3} \times V_{motor} \times I_{motor} \times PF \times \eta_{motor}}{746}

Where:

  • VmotorV_{motor} = motor terminal voltage (V)
  • ImotorI_{motor} = motor current (A)
  • PFPF = power factor (typically 0.80 to 0.85 for ESP motors)
  • ηmotor\eta_{motor} = motor efficiency (decimal)
  • 746 = watts per horsepower

Rearranging for motor current at any load:

Imotor=746×HPactual3×Vmotor×PF×ηmotorI_{motor} = \frac{746 \times HP_{actual}}{\sqrt{3} \times V_{motor} \times PF \times \eta_{motor}}

Current at Partial Load

At partial load, motor current does not decrease linearly with HP because magnetizing current remains roughly constant:

IpartialIno-load+(Ifull-loadIno-load)×LFI_{partial} \approx I_{no\text{-}load} + (I_{full\text{-}load} - I_{no\text{-}load}) \times LF

Where Ino-loadI_{no\text{-}load} is typically 30-50% of Ifull-loadI_{full\text{-}load} for ESP motors.

Typical Motor Parameters

Motor HP Voltage (V) Current (A) Motor OD (in)
30 460 40 3.75
75 750 62 4.56
100 1,000 62 4.56
200 1,500 83 5.43
400 2,400 103 5.43
750 3,300 141 7.38

Note: These are representative values. Actual parameters vary by manufacturer and motor series.


Motor Temperature Considerations

Heat Dissipation

The ESP motor is cooled by the well fluid flowing past the motor housing. The minimum fluid velocity past the motor for adequate cooling:

vfluid1.0 ft/s (typical minimum)v_{fluid} \geq 1.0 \text{ ft/s (typical minimum)}

The annular velocity between the motor and casing:

vannular=QtotalAannular=Qtotalπ4(Dcasing2Dmotor2)v_{annular} = \frac{Q_{total}}{A_{annular}} = \frac{Q_{total}}{\frac{\pi}{4}(D_{casing}^2 - D_{motor}^2)}

Where all dimensions are in consistent units.

Temperature Rating

Motor Class Maximum Winding Temperature Typical Application
Standard 280 F (138 C) Wells with BHT < 200 F
High-temp 350 F (177 C) Wells with BHT 200-300 F
Ultra high-temp 400 F (204 C) HPHT wells

The motor winding temperature equals the ambient well temperature plus the temperature rise from internal losses:

Twinding=Tambient+ΔTriseT_{winding} = T_{ambient} + \Delta T_{rise}TwindingTratingT_{winding} \leq T_{rating}

Cable Voltage Drop

Importance

The cable delivers three-phase power from the surface to the downhole motor. Due to the cable's electrical resistance, voltage is lost along the cable length. If the voltage reaching the motor terminals is too low, the motor cannot develop rated torque and will overheat.

Voltage Drop Calculation

For a three-phase cable, the voltage drop per 1,000 ft of cable:

ΔV1000=3×Imotor×Rcable\Delta V_{1000} = \sqrt{3} \times I_{motor} \times R_{cable}

Where:

  • ΔV1000\Delta V_{1000} = voltage drop per 1,000 ft (V/1000 ft)
  • ImotorI_{motor} = motor current (A)
  • RcableR_{cable} = cable resistance per 1,000 ft per conductor (ohm/1000 ft)

The total voltage drop along the full cable length:

ΔVtotal=ΔV1000×Lcable1000\Delta V_{total} = \Delta V_{1000} \times \frac{L_{cable}}{1000}

Where LcableL_{cable} is the cable length in feet (typically equal to or slightly greater than the pump setting depth).

Temperature Effect on Resistance

Cable resistance increases with temperature. The resistance at downhole temperature:

RT=R77×[1+α(T77)]R_T = R_{77} \times [1 + \alpha (T - 77)]

Where:

  • R77R_{77} = resistance at 77 F (published catalog value, ohm/1000 ft)
  • α\alpha = temperature coefficient of resistance (0.00214 per F for copper)
  • TT = average cable temperature (F)

The average cable temperature is typically estimated as:

Tavg=Tsurface+Tbottomhole2T_{avg} = \frac{T_{surface} + T_{bottomhole}}{2}

Cable Resistance by Size

AWG Size Conductor Area (kcmil) R77R_{77} (ohm/1000 ft) Max Ampacity (A)
1 83.7 0.139 115
2 66.4 0.175 95
4 41.7 0.278 70
6 26.3 0.442 55

Note: Resistance values are per conductor. Ampacity ratings are approximate and depend on cable construction, insulation type, and installation conditions.


Cable Size Selection

Selection Criteria

Cable size must satisfy two independent requirements:

  1. Ampacity: The cable must carry the motor current without exceeding its thermal rating
  2. Voltage drop: The voltage drop must be within acceptable limits

Ampacity Requirement

I_{cable\text{-}rating} \geq I_{motor} \times 1.10 \quad \text{(10% margin)}

Voltage Drop Requirement

The voltage drop should not exceed a percentage of the motor nameplate voltage:

ΔVtotalΔVmax\Delta V_{total} \leq \Delta V_{max}

Common criteria:

Criterion Maximum Voltage Drop
Conservative 3% of motor nameplate voltage
Standard 5% of motor nameplate voltage
Aggressive 8% of motor nameplate voltage
Rule of thumb 30 V per 1,000 ft of cable

Minimum Cable Size

The minimum cable size is the larger (lower AWG number) of:

  1. The size that satisfies the ampacity requirement
  2. The size that satisfies the voltage drop requirement
AWGmin=min(AWGampacity,AWGvdrop)AWG_{min} = \min(AWG_{ampacity}, AWG_{vdrop})

Where lower AWG numbers indicate larger cables.

Selection Workflow

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Power Loss in Cable

Cable Power Loss

The electrical power dissipated as heat in the cable:

Ploss=3×Imotor2×RT×Lcable1000P_{loss} = 3 \times I_{motor}^2 \times R_T \times \frac{L_{cable}}{1000}

Where:

  • PlossP_{loss} = power loss in cable (watts)
  • ImotorI_{motor} = motor current per phase (A)
  • RTR_T = resistance at temperature per conductor per 1,000 ft (ohm/1000 ft)
  • LcableL_{cable} = cable length (ft)
  • Factor of 3 accounts for three conductors

Converting to horsepower:

HPloss=Ploss746HP_{loss} = \frac{P_{loss}}{746}

Cable Loss as Percentage of Total Power

%loss=PlossPtotal×100=3I2RTL/10003×Vsurface×I×PF×100\%_{loss} = \frac{P_{loss}}{P_{total}} \times 100 = \frac{3 I^2 R_T L / 1000}{\sqrt{3} \times V_{surface} \times I \times PF} \times 100

Typical Cable Losses

Cable AWG Motor Amps Cable Length (ft) Power Loss (HP) Loss %
2 60 6,000 8.0 3.2%
2 60 10,000 13.3 5.3%
1 80 8,000 14.2 3.8%
4 40 5,000 4.5 3.6%
4 40 12,000 10.7 8.6%

Note: Values calculated at 77 F. At higher temperatures, losses increase due to higher resistance.


Surface Electrical System

Required Surface Voltage

The surface transformer or VSD must supply sufficient voltage to overcome the cable drop and deliver rated voltage to the motor:

Vsurface=Vmotor+ΔVtotalV_{surface} = V_{motor} + \Delta V_{total}

VSD Considerations

When a Variable Speed Drive (VSD) is used:

  • Voltage scales with frequency: Voutf/fbaseV_{out} \propto f / f_{base}
  • At reduced speed, motor voltage and current change
  • Cable voltage drop changes with current

The VSD output voltage at any frequency:

VVSD=Vbase×ffbase+ΔVcable(If)V_{VSD} = V_{base} \times \frac{f}{f_{base}} + \Delta V_{cable}(I_f)

Where ff is the operating frequency and fbasef_{base} is the base frequency (typically 60 Hz).

System Efficiency

The overall electrical efficiency from surface to pump shaft:

ηsystem=ηVSD×ηcable×ηmotor\eta_{system} = \eta_{VSD} \times \eta_{cable} \times \eta_{motor}

Where:

ηcable=1Pcable-lossPinput\eta_{cable} = 1 - \frac{P_{cable\text{-}loss}}{P_{input}}
Component Typical Efficiency
VSD 95 - 97%
Cable 92 - 98% (depends on length and size)
Motor 80 - 92%
Overall electrical 70 - 87%

Design Example

Given Data

Parameter Value
Pump BHP 150 HP
Motor selected 200 HP, 1,500 V, 83 A
Cable length 8,000 ft
Surface temperature 80 F
Bottomhole temperature 220 F
Cable type #2 AWG copper, round

Calculations

Load Factor:

LF=150200=0.75(optimal range)LF = \frac{150}{200} = 0.75 \quad \text{(optimal range)}

Average Cable Temperature:

Tavg=80+2202=150 FT_{avg} = \frac{80 + 220}{2} = 150 \text{ F}

Cable Resistance at Temperature:

R150=0.175×[1+0.00214×(15077)]=0.175×1.156=0.202 ohm/1000 ftR_{150} = 0.175 \times [1 + 0.00214 \times (150 - 77)] = 0.175 \times 1.156 = 0.202 \text{ ohm/1000 ft}

Voltage Drop:

ΔV=3×83×0.202×8,0001,000=232 V\Delta V = \sqrt{3} \times 83 \times 0.202 \times \frac{8{,}000}{1{,}000} = 232 \text{ V}

Voltage Drop Percentage:

%=2321,500×100=15.5%\% = \frac{232}{1{,}500} \times 100 = 15.5\%

This exceeds the 5% criterion. The designer should either:

  • Increase cable size to #1 AWG (reduces resistance)
  • Select a higher-voltage motor (reduces current for same HP)

With #1 AWG Cable:

R150=0.139×1.156=0.161 ohm/1000 ftR_{150} = 0.139 \times 1.156 = 0.161 \text{ ohm/1000 ft}ΔV=3×83×0.161×8=185 V(12.3%)\Delta V = \sqrt{3} \times 83 \times 0.161 \times 8 = 185 \text{ V} \quad (12.3\%)

Still high. A higher voltage motor (e.g., 2,400 V, 52 A) would yield:

ΔV=3×52×0.161×8=116 V(4.8%)\Delta V = \sqrt{3} \times 52 \times 0.161 \times 8 = 116 \text{ V} \quad (4.8\%)

This meets the 5% criterion with #1 AWG cable.

Cable Power Loss (final design, 2,400 V motor, #1 AWG):

Ploss=3×522×0.161×8=10,461 W=14.0 HPP_{loss} = 3 \times 52^2 \times 0.161 \times 8 = 10{,}461 \text{ W} = 14.0 \text{ HP}

References

  1. Takacs, G. (2009). Electrical Submersible Pumps Manual: Design, Operations, and Maintenance. Gulf Professional Publishing.

  2. Baker Hughes. (2021). ESP Cable Engineering Handbook. Baker Hughes Technical Publications.

  3. IEEE Standard 1580. (2010). Recommended Practice for Marine Cable for Use on Shipboard and Fixed or Floating Platforms. IEEE.

  4. Brown, K.E. (1984). The Technology of Artificial Lift Methods, Vol. 2b. PennWell Books.

  5. Neely, A.B. and Patterson, M.M. (1984). "Soft Starting the Submersible Pump." SPE-12484-MS, Formation Damage Control Symposium, Bakersfield, California.

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