As we know One V/A is equal to 1 Ω (1 V/A = 1 Ω).
To convert Volt/Ampere to Ohm, multiply your V/A figure by 1.
Example : convert 25 V/A to Ω:
25 V/A = 25 × 1 Ω = Ω
To convert Ohm to Volt/Ampere, divide your Ω figure by 1.
Example : convert 25 Ω to V/A:
25 Ω = 25 ÷ 1 V/A = V/A
As we know One Ω is equal to 1 V/A (1 Ω = 1 V/A).
To convert Ohm to Volt/Ampere, multiply your Ω figure by 1.
Example : convert 45 Ω to V/A:
45 Ω = 45 × 1 V/A = V/A
To convert Volt/Ampere to Ohm, divide your V/A figure by 1.
Example : convert 45 V/A to Ω:
45 V/A = 45 ÷ 1 Ω = Ω
| V/A to Ω | 1 V/A = 1 Ω |
| V/A to MΩ | 1 V/A = 0.000001 MΩ |
| V/A to μΩ | 1 V/A = 1000000 μΩ |
| V/A to mΩ | 1 V/A = 1000 mΩ |
| V/A to kΩ | 1 V/A = 0.001 kΩ |
| V/A to 1/S | 1 V/A = 1 1/S |
| V/A to abΩ | 1 V/A = 1e+9 abΩ |
| V/A to EMU of resistance | 1 V/A = 1e+9 EMU of resistance |
| V/A to stΩ | 1 V/A = 1.11265e-12 stΩ |
| V/A to ESU of resistance | 1 V/A = 1.11265e-12 ESU of resistance |
| V/A to Quantized Hall resistance | 1 V/A = 0.000038740461 Quantized Hall resistance |
| V/A to Planck impedance | 1 V/A = 0.03335641 Planck impedance |
| V/A to EΩ | 1 V/A = 1e-18 EΩ |
| V/A to PΩ | 1 V/A = 1e-15 PΩ |
| V/A to TΩ | 1 V/A = 1e-12 TΩ |
| V/A to GΩ | 1 V/A = 1e-9 GΩ |
| V/A to hΩ | 1 V/A = 0.01 hΩ |
| V/A to daΩ | 1 V/A = 0.1 daΩ |
| V/A to dΩ | 1 V/A = 10 dΩ |
| V/A to cΩ | 1 V/A = 100 cΩ |
| V/A to nΩ | 1 V/A = 1e+9 nΩ |
| V/A to pΩ | 1 V/A = 1e+12 pΩ |
| V/A to fΩ | 1 V/A = 1e+15 fΩ |
| V/A to aΩ | 1 V/A = 1e+18 aΩ |
| V/A to kV/A | 1 V/A = 0.001 kV/A |
| V/A to mV/A | 1 V/A = 1000 mV/A |
| V/A to μV/A | 1 V/A = 1000000 μV/A |
| V/A to MV/A | 1 V/A = 0.000001 MV/A |
| V/A to V/kA | 1 V/A = 1000 V/kA |
| V/A to V/mA | 1 V/A = 0.001 V/mA |
| V/A to V/μA | 1 V/A = 0.000001 V/μA |
| V/A to V/MA | 1 V/A = 1000000 V/MA |
| Created @ o.vg | Free Unit Converters |
Ω. Since one V/A equals 1 Ω, 9 V/A in Ω will be Ω.
There are 1 Ω in one V/A. In turn, one Ω is equal to 1 V/A.
1 Ω is approximately equal to 1 V/A.
The Volt/Ampere value of 8 Ω is V/A. (i.e.,) 8 x 1 = V/A.
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