Crash course: Ohm's Law for electricians no jargon edition (part 4)
Crash course on Ohm's Law for electricians no jargon edition. Field-ready, no fluff.
Part 4: Ohm's Law when the math gets weird
Parts 1 through 3 covered the basics: V=IR, the wheel, voltage drop, and sizing conductors. This one handles the edge cases that trip up techs in the field. Parallel paths, mixed loads, power factor, and why your meter reads something different than the calculator says it should.
If you are troubleshooting and the numbers do not add up, one of these is usually why.
Parallel paths and why current splits
Current always takes every available path, not just the path of least resistance. That old saying is wrong and it gets people hurt. Lower resistance gets more current, but every parallel path carries some.
For two resistances in parallel: R_total = (R1 × R2) / (R1 + R2). The total is always less than the smallest branch. Put a 10 ohm and a 20 ohm in parallel, you get 6.67 ohms. That is why a ground fault through a person standing in wet soil is dangerous even if the equipment ground is intact. The human body is just another parallel path.
If you are meggering a motor and reading 2 megohms, check whether the heaters or space heater circuits are still landed. Parallel paths through auxiliary gear will pull your reading down and make a good motor look bad.
Mixed loads on a single branch
Resistive loads (heaters, incandescent, resistance elements) follow Ohm's Law cleanly. Inductive loads (motors, ballasts, transformers) and capacitive loads do not, because current and voltage are out of phase. On the same circuit, you cannot just add the amps.
For a 20A branch feeding a 1200W heater and a 1/2 HP motor at 120V, the heater pulls 10A resistive. The motor nameplate might say 9.8A. Adding them gives 19.8A, which looks fine. But motor inrush on start can hit 6x or 7x FLA for a half second. See NEC 430.22 for motor branch circuit sizing and NEC 210.19 for general branch conductor rules.
- Continuous loads: size conductors at 125 percent (NEC 210.19(A)(1))
- Single motor branch: 125 percent of FLC (NEC 430.22)
- Multiple motors plus other loads: NEC 430.24
- Largest motor gets the 125 percent bump, the rest at 100 percent
Power factor, real power, apparent power
Your clamp meter reads amps. Multiply by volts, you get VA (volt-amps), not watts. On a purely resistive load they are the same. On anything with a coil or a capacitor, they are not.
Real power (watts) = V × I × PF. Power factor is the cosine of the phase angle between voltage and current. A typical induction motor runs at 0.8 to 0.85 PF under load, worse when lightly loaded. A VFD or LED driver without correction can be lower.
This matters when you are sizing a generator or a transformer. A 10 kVA transformer does not deliver 10 kW to a 0.7 PF load. It delivers 7 kW, and the other 3 kVAR is reactive power bouncing back and forth between the source and the load, heating your conductors the whole way.
If the POCO is billing you for kVA demand and your PF is under 0.9, capacitor correction pays for itself in under two years on most industrial services. Check the bill before you quote the job.
Why your meter disagrees with the calculator
You calculated 24A on a run. The clamp reads 21A. Which is right? Usually both, and the difference tells you something.
- Voltage is not 120V. It is 117 or 122 or whatever the POCO is delivering today. Measure, do not assume.
- The load is not at nameplate. Motors pull less than FLA when underloaded. Heaters pull less when the element is aging.
- Harmonics. Non-linear loads (electronics, VFDs, LED) distort the waveform. A true-RMS meter reads correctly, an averaging meter does not. If your cheap meter reads low on a known resistive load, it is averaging.
- Neutral current on 3-phase systems with triplen harmonics can exceed phase current. NEC 310.15(E) covers this, and it is why you derate or upsize the neutral on heavy electronic loads.
Voltage drop under real conditions
The textbook formula (2 × K × I × D / CM for single phase) assumes a steady resistive load at a fixed temperature. Conductor resistance goes up about 0.4 percent per degree C above 20C. A circuit that drops 2.5 percent on a cool morning can drop 3.5 percent on a 40C afternoon in a hot attic.
NEC 210.19 Informational Note No. 4 recommends 3 percent on branch circuits, 5 percent total feeder plus branch. Those are recommendations, not code, but the AHJ in some jurisdictions treats them as enforceable. Know your local amendments.
- Long runs: upsize the conductor, not the breaker
- Motor circuits: voltage drop on starting can stall the motor even if running voltage is fine
- Use the actual circuit length, not the straight-line distance
Field checklist when numbers do not match
Before you chase ghosts, run through this. Nine times out of ten the answer is in the first three items.
- Measure actual voltage at the load, not at the panel
- Verify meter is true-RMS if the load has any electronics
- Check for parallel paths you did not account for
- Confirm power factor if it is an inductive load
- Look at conductor temperature, especially in conduit fill or attics
- Re-read the nameplate. Service factor, duty cycle, and code letter all change the math
Ohm's Law is never wrong. The inputs are wrong. Measure, do not guess, and the numbers will land.
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