How do you calculate resistors in parallel?
Add the reciprocals and take the reciprocal of the sum: 1/R = 1/R1 + 1/R2 + … For two resistors that simplifies to R1 × R2 ÷ (R1 + R2), so 10 kΩ in parallel with 4.7 kΩ is 3.197 kΩ.
Add up to eight resistors in parallel or in series with this parallel resistor calculator and see how the current or voltage divides between them. Or enter an existing resistor and a lower target to get the value to add in parallel, rounded to E24 and E96.
Optional: shows the current and power in each resistor.
Parallel resistance
3.197 kΩ
If every part has the same tolerance (say ±1 %), the combination is within the same percentage, in parallel or in series.
How the current divides
| Part | Resistor | Share of current |
|---|---|---|
| R1 | 10 kΩ | 32 % |
| R2 | 4.7 kΩ | 68 % |
Use 1/R = 1/R1 + 1/R2 + … + 1/Rn. For two resistors this is R1 × R2 ÷ (R1 + R2): 10 kΩ in parallel with 4.7 kΩ gives 10 × 4.7 ÷ 14.7 = 3.197 kΩ. The total is always below the smallest resistor. In series, simply add the values.
Resistors in series share one current, so their resistances add. Resistors in parallel share one voltage, so their conductances (1/R) add.
Two resistors in parallel, and the resistor Rx that brings an existing R down to a target Rt:
With a voltage V across a parallel network, each branch carries Ik = V ÷ Rk and dissipates V² ÷ Rk. With V across a series string, the current is V ÷ R and each resistor drops Vk = V × Rk ÷ R.
1/R = 1/1 + 1/2 + 1/2 = 2 S, so R = 500 mΩ. The source supplies 3 ÷ 0.5 = 6 A: 3 A through the 1 Ω resistor and 1.5 A through each 2 Ω. The 1 Ω part dissipates 9 W and each 2 Ω part 4.5 W, 18 W in all.
R = 4 × 20 + 10 = 90 Ω, so I = 9 ÷ 90 = 100 mA. Each 20 Ω resistor drops 2 V and dissipates 200 mW; the 10 Ω drops 1 V.
Rx = 1000 × 800 ÷ (1000 − 800) = 4 kΩ. The nearest E24 value, 3.9 kΩ, gives 795.9 Ω (-0.51 %); the nearest E96 value, 4.02 kΩ, gives 800.8 Ω (+0.10 %), well inside a 1 % part’s tolerance.
R1 × R2 ÷ (R1 + R2) for common resistor values. The diagonal is half the value.
| R1 \ R2 | 100 Ω | 220 Ω | 470 Ω | 1 kΩ | 2.2 kΩ | 4.7 kΩ | 10 kΩ |
|---|---|---|---|---|---|---|---|
| 100 Ω | 50 Ω | 68.8 Ω | 82.5 Ω | 90.9 Ω | 95.7 Ω | 97.9 Ω | 99 Ω |
| 220 Ω | 68.8 Ω | 110 Ω | 150 Ω | 180 Ω | 200 Ω | 210 Ω | 215 Ω |
| 470 Ω | 82.5 Ω | 150 Ω | 235 Ω | 320 Ω | 387 Ω | 427 Ω | 449 Ω |
| 1 kΩ | 90.9 Ω | 180 Ω | 320 Ω | 500 Ω | 688 Ω | 825 Ω | 909 Ω |
| 2.2 kΩ | 95.7 Ω | 200 Ω | 387 Ω | 688 Ω | 1.1 kΩ | 1.5 kΩ | 1.8 kΩ |
| 4.7 kΩ | 97.9 Ω | 210 Ω | 427 Ω | 825 Ω | 1.5 kΩ | 2.35 kΩ | 3.2 kΩ |
| 10 kΩ | 99 Ω | 215 Ω | 449 Ω | 909 Ω | 1.8 kΩ | 3.2 kΩ | 5 kΩ |
The exact value to add across a 10 kΩ resistor for each target, the nearest E24 part and the result it gives.
| Target | Exact partner | Nearest E24 | Result | Error |
|---|---|---|---|---|
| 9.1 kΩ | 101.1 kΩ | 100 kΩ | 9.091 kΩ | -0.10 % |
| 8.2 kΩ | 45.56 kΩ | 47 kΩ | 8.246 kΩ | +0.56 % |
| 7.5 kΩ | 30 kΩ | 30 kΩ | 7.5 kΩ | +0.00 % |
| 6.8 kΩ | 21.25 kΩ | 22 kΩ | 6.875 kΩ | +1.10 % |
| 5.6 kΩ | 12.73 kΩ | 13 kΩ | 5.652 kΩ | +0.93 % |
| 4.7 kΩ | 8.868 kΩ | 9.1 kΩ | 4.764 kΩ | +1.37 % |
| 3.3 kΩ | 4.925 kΩ | 5.1 kΩ | 3.377 kΩ | +2.35 % |
| 2.2 kΩ | 2.821 kΩ | 2.7 kΩ | 2.126 kΩ | -3.36 % |
| 1 kΩ | 1.111 kΩ | 1.1 kΩ | 991 Ω | -0.90 % |
Combining two resistors is the usual way to reach a value that is not in the series you stock, or to share power: two equal resistors in parallel each carry half the current and half the power, so the pair handles twice what one part could. Tolerances do not get worse: the combination of ±1 % parts is still within ±1 %. Mind the layout, though: in a low-value current-sense network the copper between parallel parts adds resistance of its own, so place them symmetrically and take the sense connections from the resistor pads. Finally, a resistor more than about 100 times larger than the one it is across changes the total by under 1 %, less than the tolerance of either part, so it is rarely worth adding.
Add the reciprocals and take the reciprocal of the sum: 1/R = 1/R1 + 1/R2 + … For two resistors that simplifies to R1 × R2 ÷ (R1 + R2), so 10 kΩ in parallel with 4.7 kΩ is 3.197 kΩ.
5 kΩ. Any number n of equal resistors in parallel gives R ÷ n, so four 100 Ω resistors in parallel make 25 Ω.
Up to eight, in parallel or in series. Enter the voltage across them and it also works as a parallel circuit calculator, with the current and power in each branch.
Not in one pass: each run is all parallel or all series. For a mixed network, work out the total resistance in stages, reducing one parallel or series group at a time.
Yes. Every resistor you add in parallel gives the current another path, so the total is always below the smallest one. Adding a much larger resistor lowers it only slightly.
Rx = R × Rt ÷ (R − Rt), where R is the existing resistor and Rt the target. To bring 1 kΩ down to 800 Ω you need 4 kΩ; the nearest E96 value, 4.02 kΩ, gives 800.8 Ω.
In inverse proportion to resistance, because each has the same voltage across it: I = V ÷ R for each branch. In OpenStax's example, 3 V across 1 Ω, 2 Ω and 2 Ω drives 3 A, 1.5 A and 1.5 A.
If every part has the same tolerance, the combination has that tolerance too, in the worst case: two ±1 % resistors in parallel or in series make a ±1 % result. Random errors partly cancel, so the typical error is smaller.
Each dissipates V² ÷ R, so equal resistors share it equally and two equal 1/4 W parts in parallel can carry 1/2 W between them. With unequal values the smaller resistor takes more of the power, so check each part on its own.
Add them: R = R1 + R2 + … The same current flows through each, and the voltage divides in proportion to resistance. Four 20 Ω and one 10 Ω in series make 90 Ω. The Series tab above works as a series resistor calculator for up to eight parts.
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