Alternating current

AC Voltage Drop Calculator

Single-phase and three-phase drop with the reactance term included, not just resistance. Set the power factor and the raceway and the calculator combines AC resistance and inductive reactance the way NEC Chapter 9 Table 9 says to.

Voltage drop calculator

Electrical system
V
Load given as
A

Conductor

Size system
Material

Run

One-way is the distance from the source to the load. Round-trip is the total conductor length there and back. The formulas already account for the return path, so choose the one you actually measured.

%
Advanced options

Identical conductors run in parallel. Leave blank for one.

°C

Reference data is at 75 °C.

1 for a purely resistive load. Motors and electronics typically run 0.7 to 0.95.

Stranded conductors read about 2% higher resistance than solid at the same size.

1.39% is inside the 3% limit you set. About 1.39% of the 480 V supply is lost in the conductors under these conditions, leaving 473.34 V at the load. That is 6.66 V dropped across the run, line to line.

Your voltage drop appears here

Enter a supply voltage, a load current and a cable length. The result updates as you type.

Voltage dropWithin limit

1.39%

6.66 V lost against a3% limit

Supply
480.00V
At the load
473.34V
Lost as heat
1,275.8W

1.39% is inside the 3% limit you set. About 1.39% of the 480 V supply is lost in the conductors under these conditions, leaving 473.34 V at the load. That is 6.66 V dropped across the run, line to line.

Source480.00 V
At load473.34 V
3% limit
Voltage falls from 480.00 volts at the source to 473.34 volts at the load, a drop of 1.39 percent against a limit of 3 percent.
Working, assumptions and sources
Conductor resistance
0.03274 Ω
Conductor reactance
0.03152 Ω
Impedance per 1000 ft
0.07329 Ω

Calculation details

  1. Effective impedance per 1000 ft

    Z_e = R × cos θ + X_L × sin θZ_e = 0.054 × 0.85 + 0.052 × 0.5268

    Result: 0.07329 Ω per 1000 ft

    R and X_L are for 250 kcmil copper in steel conduit, from NEC Chapter 9 Table 9. θ is the power factor angle.

  2. Voltage drop

    V_drop = √3 × I × Z_e × LV_drop = 1.732 × 150 A × 0.07329 Ω/1000 ft × 0.3500 (1000 ft)

    Result: 6.66 V

    A balanced three-phase circuit has no return conductor carrying full load current. The line-to-line drop is √3 times the drop along one conductor over the one-way length.

  3. Voltage drop percentage

    %V_drop = (V_drop ÷ V_source) × 100%V_drop = (6.66 V ÷ 480 V) × 100

    Result: 1.39%

  4. Voltage at the load

    V_load = V_source − V_dropV_load = 480 V − 6.66 V

    Result: 473.34 V

  5. Power lost in the conductors

    P_loss = I² × R_path × number of current-carrying pathsP_loss = 150² × 0.0189 Ω × 3

    Result: 1,275.8 W

    Only resistance dissipates power. Reactance stores and returns energy each cycle rather than turning it into heat.

Assumptions and sources

  • AC resistance and reactance are for three single conductors in steel conduit, 60 Hz, Class B stranded.
  • Balanced three-phase load. The result is the line-to-line voltage drop.

Resistance and reactance: NEC Chapter 9, Table 9 (AC values at 75 °C, 60 Hz)

Formula

Resistance is only half of it.

Single-phase AC
V_drop = 2 × I × Z_e × L
Balanced three-phase AC
V_drop = √3 × I × Z_e × L
Effective impedance
Z_e = R × cos θ + X_L × sin θ
R
AC resistance of the conductor · Ω / 1000 ft
X_L
Inductive reactance at 60 Hz · Ω / 1000 ft
θ
Power factor angle, arccos(PF)
cos θ
The power factor itself

Power factor

What ignoring reactance costs you.

250 kcmil copper in steel conduit: AC resistance 0.052 Ω and reactance 0.052 Ω per 1000 ft. The last column is how much a resistance-only estimate understates the drop.

Effective impedance against power factor for 250 kcmil copper in steel conduit
Power factorEffective ZResistance onlyUnderstated by
1.000.054 Ω0.054 Ω
0.950.06754 Ω0.054 Ω25.1%
0.900.07127 Ω0.054 Ω32.0%
0.850.07329 Ω0.054 Ω35.7%
0.800.0744 Ω0.054 Ω37.8%
0.700.07494 Ω0.054 Ω38.8%

Computed as Z_e = R cos θ + X_L sin θ from NEC Chapter 9, Table 9 values for 250 kcmil uncoated copper in steel conduit at 75 °C, 60 Hz.

A 350 ft feeder at 0.8 power factor calculated on resistance alone would come out roughly a third low. That is the difference between a run that passes a 3% target on paper and one that fails when it is commissioned. To calculate voltage drop for DC and AC circuits from one place, the main calculator handles all three system types.

Questions

Common questions.

When does conductor reactance actually matter?

When power factor is below about 0.9, when the conductors are large, or when they run in steel conduit, and most of all when all three are true at once. At unity power factor reactance contributes nothing to the drop. At 0.8 power factor on 250 kcmil copper in steel conduit, effective impedance is about 60% higher than the resistance-only figure, so a resistance-only calculation would tell you a run passes when it does not. On small conductors at good power factor the difference is a fraction of a percent and not worth chasing.

What is effective impedance and why is it not √(R² + X²)?

Effective impedance is Z_e = R × cos θ + X_L × sin θ, the projection of the conductor impedance onto the load-current direction. The magnitude √(R² + X²) would be right if you wanted the total impedance of the conductor, but voltage drop is about the component of that impedance in phase with the current. NEC Chapter 9 Table 9 states this formula in its notes and publishes an effective-Z column at 0.85 power factor computed with it.

Why does steel conduit increase voltage drop?

Steel is ferromagnetic, so it concentrates the magnetic field around the conductors. That raises inductive reactance, roughly 25% higher than in PVC, and adds eddy-current and hysteresis losses that show up as higher AC resistance. On 250 kcmil copper the reactance goes from 0.041 Ω per 1000 ft in PVC to 0.052 in steel. At poor power factor that difference is worth several percent of the total drop.

Does the three-phase result mean line-to-line or line-to-neutral?

Line-to-line. The √3 multiplier produces the drop between two phase conductors, which is what you compare against a line-to-line supply voltage like 480 V or 400 V. If you need the line-to-neutral drop on a balanced system, divide the result by √3, or equivalently calculate with the line-to-neutral voltage and a multiplier of 1. Mixing the two is a common way to get an answer that is out by 73%.

What frequency do these reactance values assume?

60 Hz. Inductive reactance is proportional to frequency, so at 50 Hz the reactance values are about 17% lower: multiply them by 50/60. Resistance is essentially unchanged at these frequencies for the conductor sizes involved. For anything above power frequency, skin effect becomes significant and this data no longer applies.