Unit 4 — Electrical Fundamentals
Section 1 — Introduction to Electricity
1.6 — Calculating & Measuring
Calculating circuit values before you pick up a meter, and measuring them
correctly once you do, are two sides of the same skill. This lesson walks
through series, parallel, and combination circuit calculations and then
covers the safe, accurate use of the multimeter and clamp meter for voltage,
current, resistance, and power measurements in HVAC/R systems.
1.6.1 — Series Circuit Calculations
In a series circuit, components are connected end-to-end so that the same
current flows through every element. The supply voltage is divided across
the resistances in proportion to their values (voltage divider principle).
Series Circuit Rules
- Total resistance: RT = R1 + R2 + R3 + …
- Current: I = VS ÷ RT — current is the same at every point in the loop
- Voltage drops: V1 = I × R1, V2 = I × R2, …
- Kirchhoff’s Voltage Law: VS = V1 + V2 + V3 + … (all drops add up to supply)
- If one element opens: the entire circuit is broken — all current stops
A 30 V control circuit contains two resistors in series: R1 = 10 Ω and
R2 = 20 Ω. Find total resistance, current, and voltage across each resistor.
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Total resistance:
RT = R1 + R2 = 10 + 20 = 30 Ω
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Circuit current:
I = VS ÷ RT = 30 V ÷ 30 Ω = 1 A
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Voltage across R1:
V1 = I × R1 = 1 A × 10 Ω = 10 V
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Voltage across R2:
V2 = I × R2 = 1 A × 20 Ω = 20 V
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Verify (KVL):
V1 + V2 = 10 + 20 = 30 V = VS ✓
Notice that R2 (the larger resistor) drops twice the voltage of R1.
This is the voltage-divider principle, which explains why a high-resistance open contact
in a series control circuit will have the full supply voltage measured across it.
💡
Series circuits and safety chains
HVAC/R control circuits wire all safety devices (high-pressure switch, low-pressure switch, overload relay) in series so that any single safety opening will de-energise the contactor coil. This is a deliberate application of series circuit behaviour: if one element opens, the entire load is switched off.
1.6.2 — Parallel Circuit Calculations
In a parallel circuit, all components share the same voltage (connected between
the same two nodes) and each branch carries its own independent current.
Adding more branches decreases total resistance and increases total current draw.
Parallel Circuit Rules
- Voltage: V is the same across every parallel branch
- Branch currents: In = V ÷ Rn — calculated independently for each branch
- Total current: IT = I1 + I2 + I3 + …
- Total resistance (reciprocal formula): 1/RT = 1/R1 + 1/R2 + …
- Two resistors shortcut: RT = (R1 × R2) ÷ (R1 + R2)
- If one element opens: only that branch stops conducting — other branches continue
A 24 V supply feeds two parallel heater elements: R1 = 12 Ω and
R2 = 6 Ω. Find equivalent resistance, branch currents, and total current.
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Equivalent resistance (product-over-sum):
RT = (12 × 6) ÷ (12 + 6) = 72 ÷ 18 = 4 Ω
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Branch 1 current:
I1 = V ÷ R1 = 24 ÷ 12 = 2 A
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Branch 2 current:
I2 = V ÷ R2 = 24 ÷ 6 = 4 A
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Total current:
IT = I1 + I2 = 2 + 4 = 6 A
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Verify (Ohm’s Law on total):
IT = V ÷ RT = 24 ÷ 4 = 6 A ✓
RT (4 Ω) is less than either individual branch — always the case
in a parallel circuit. The smaller-resistance branch (R2) draws more current,
which must be considered when sizing the supply conductor and protection device.
💡
Parallel loads in HVAC/R
Most HVAC/R power loads (compressor, condenser fan, evaporator fans, heaters) are wired in parallel across the supply voltage so each operates at rated voltage regardless of the others. Adding a load increases total current on the supply conductors — always check ampacity when adding equipment to an existing circuit.
1.6.3 — Combination Circuit Calculations
A combination (or series-parallel) circuit contains both series and parallel
sections. The strategy is to reduce the parallel sections to a single equivalent
resistance first, then treat the result as a simple series circuit.
Step-by-Step Reduction Method
- Identify all series and parallel groups in the circuit from the schematic. Redraw if necessary to make the structure clear.
- Reduce each parallel group to a single equivalent resistance using the reciprocal formula (or product-over-sum for two resistors).
- Redraw the circuit as a series string of resistances: the original series elements plus the equivalent resistances from Step 2.
- Calculate total resistance by adding all series values: RT = Rseries + Req(parallel) + …
- Calculate total current: IT = VS ÷ RT
- Calculate voltage drops across each series element (V = IT × R). The voltage across a parallel group equals the voltage drop calculated for its equivalent resistance.
- Calculate branch currents in each parallel group: Ibranch = Vgroup ÷ Rbranch
- Verify using KVL (voltage drops sum to supply) and KCL (branch currents sum to IT at each node).
A 120 V circuit has R1 = 10 Ω in series with a parallel combination
of R2 = 30 Ω and R3 = 15 Ω.
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Reduce the parallel group (R2 ∥ R3):
Req = (30 × 15) ÷ (30 + 15) = 450 ÷ 45 = 10 Ω
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Redraw as series: R1 + Req
RT = 10 + 10 = 20 Ω
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Total current:
IT = 120 ÷ 20 = 6 A
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Voltage across R1:
V1 = 6 A × 10 Ω = 60 V
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Voltage across the parallel group:
Vparallel = 6 A × 10 Ω = 60 V
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Branch currents:
I2 = 60 ÷ 30 = 2 A | I3 = 60 ÷ 15 = 4 A
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Verify KCL: I2 + I3 = 2 + 4 = 6 A = IT ✓
Verify KVL: V1 + Vparallel = 60 + 60 = 120 V = VS ✓
⚠️
Check the reduction order
Always reduce parallel groups before combining series elements. Attempting to combine resistors in the wrong order produces incorrect results. If the circuit is complex, redraw it at each step to avoid errors.