Part 1 · Electrical Foundations · Chapter 03 Complete 9 min read

Ohm's Law in Practice

V = I × R. The three forms, the triangle, and how techs actually use it in the field to validate readings.

What you'll take away

  • State Ohm's Law and rearrange it to solve for any of its three variables
  • Use Ohm's Law to validate whether a meter reading makes physical sense
  • Apply the power form (P = V × I) to sizing and load estimation

There is exactly one equation you cannot get through HVAC controls work without internalizing. Every meter reading, every component spec, every calculation of whether something is operating normally traces back to it. The equation is embarrassingly simple:

V = I × R

Voltage equals current times resistance. It’s the law that ties together the three variables introduced in the previous chapter. And because it’s algebraic, any two of the variables determine the third — if you know two, you can calculate the one you don’t have a meter for.

The triangle

A mnemonic worth committing to memory, because you’ll catch yourself using it mentally for the rest of your career:

        V
      ─────
      I │ R

Cover the variable you want to find. The remaining two show how to calculate it. Cover V — I times R gives voltage. Cover I — V divided by R gives current. Cover R — V divided by I gives resistance. Three forms of the same law.

The three forms of Ohm's Law

reference
V = I × R Solve for voltage Given current and resistance
I = V / R Solve for current Given voltage and resistance
R = V / I Solve for resistance Given voltage and current

Most HVAC applications lean hardest on the first two forms. You rarely calculate resistance from a voltage and current reading; you measure resistance directly with a DMM on ohms. But predicting current from a known voltage and a coil’s rated resistance — that’s a move you’ll make constantly.

Using Ohm’s Law to validate readings

The single most common reason a service tech discovers a bad meter reading is that the number doesn’t fit Ohm’s Law. Consider: a 24 VAC gas valve coil is spec’d at 60 ohms resistance. What current should it draw when energized?

I = V / R = 24 / 60 = 0.4 amps, or 400 mA.

Now suppose you clamp around the coil lead with a milliamp-capable meter and measure 90 mA instead of 400 mA. Ohm’s Law says that’s impossible unless one of three things is wrong: the voltage across the coil is lower than 24V, the coil’s resistance is higher than 60 Ω (partial winding open), or the meter is lying. You now have a testable hypothesis rather than a mystery.

This validation move is the real power of Ohm’s Law on the job. You don’t use it to compute your readings; you use it to catch readings that don’t add up.

Voltage drop as a direct application

One of the most useful Ohm’s Law applications in the field is voltage drop across a closed switch or contact. In a perfect world, a closed switch has zero resistance, so any current flowing through it produces zero voltage drop. In reality, contacts develop surface resistance from oxidation, pitting, and corrosion. Even a few tenths of an ohm can produce a measurable voltage drop under load.

A closed high-limit switch that should read zero voltage drop across its terminals but actually reads 2.5 V drop, with the downstream load pulling 0.5 A, reveals contact resistance: R = V / I = 2.5 / 0.5 = 5 ohms of unwanted resistance. That’s a switch on its way to failure — visible to a voltage drop test but invisible to a simple continuity check. The voltage drop test is Ohm’s Law in diagnostic form.

The power form — Watts from volts and amps

Electrical power (in watts) is the rate of energy delivery. For any DC circuit or simple AC resistive circuit, the formula is:

P = V × I — power equals voltage times current.

This matters in HVAC work for sizing and for load estimation. A 24 VAC zone valve pulling 0.5 A draws P = 24 × 0.5 = 12 VA. Add up the VA of every load on the 24V circuit, compare it to the transformer’s rating (usually 40 VA or 75 VA on residential), and you know whether the transformer is properly sized.

Common 24V loads — VA draw

reference
Gas valve coil (main) ~5–10 VA Varies by valve size
Zone valve motor ~6–8 VA running, 40 VA startup Startup load can stack
Ignition module ~5–10 VA during trial Spike during HSI warmup on some
Thermostat (modern digital) ~1–3 VA C-wire powered
Contactor coil (AC/HP) ~4–10 VA Per contactor energized
Aquastat relay internal ~3–5 VA Plus any switched loads
Typical 40 VA transformer budget All loads combined < 35 VA Leave headroom for startup spikes

AC versus DC in the formula

One nuance worth flagging early: Ohm’s Law as stated (V = I × R) applies exactly to DC circuits, and to AC circuits containing only resistive loads. When you introduce AC circuits with inductive loads — motors, transformers, solenoid coils — there’s additional complexity from a property called inductance, and the relationship between voltage and current involves phase shifts that simple resistance doesn’t capture.

For practical HVAC service work, you can mostly ignore this nuance. The DMM on AC voltage reads the effective (RMS) voltage, the clamp meter reads the effective current, and the simple relationship is close enough for diagnostic sanity-checking on most circuits. When dealing with motor starting characteristics or capacitor-run circuits specifically, the AC power math gets more involved, and the Components chapter on capacitors will pick up that thread.

Worked example — a 24V control sanity check

Ohm’s Law analysis. At 20 VAC instead of 24, every 24V load in the system is being under-driven. A zone valve coil spec’d at 30 Ω normally draws I = 24/30 = 0.8 A. At 20 V, it draws I = 20/30 = 0.67 A — about 16% less current and therefore about 16% less force in the solenoid. That’s enough to prevent some valves from opening reliably.

On a pressure switch, the applied voltage has to overcome the contact mechanism’s spring. If the module’s switching output drops proportionally and can’t push the switch firmly enough to register closure, the pressure switch will appear to “fault” even though mechanically it’s working fine against actual draft.

Diagnostic resolution: the transformer’s primary voltage was normal (121 VAC), but the secondary was reading low under load — meaning the transformer itself was loaded beyond its capacity or partially failed. Checked the 24V load totals: three zone valves plus pressure switch plus gas valve coil plus inducer relay coil plus aquastat — about 42 VA of steady load on a 40 VA transformer, not counting startup spikes. Upgraded to a 75 VA transformer. 24V at R-C came to a steady 26 VAC under full load. No more pressure-switch faults.

Ohm’s Law diagnosed this call. No meter reading looked obviously wrong in isolation; the diagnosis was in how the numbers combined.

Quick reference

Ohm's Law at a glance

reference
V = I × R Voltage Current times resistance
I = V / R Current Voltage over resistance
R = V / I Resistance Voltage over current
P = V × I Power (watts or VA) Volts times amps
Validate readings Does V = I × R hold? If not, something's wrong
AC/DC note Exact for DC, close enough for non-inductive AC Motors / capacitor circuits have phase effects

Check your understanding

0 / 3

01A solenoid coil is rated 24 VAC / 40 Ω. What current does it draw when energized normally?

02You measure 2.5 V dropped across a closed high-limit switch that's passing 0.5 A during operation. What's the contact resistance?

03A 40 VA transformer is powering a combined 24V control load of 42 VA steady state, with brief startup spikes of 55 VA. What's the most likely symptom?

Before you close the chapter

You should now be able to state Ohm’s Law in all three forms, apply it to validate whether a meter reading makes physical sense, and extend it to power calculations using P = V × I for load sizing. The next chapter distinguishes AC from DC — the two kinds of electricity you’ll find in any HVAC system — and when each one matters.