Labo Élec

electrical lab simulator

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Reminder sheet

Resistor networks

Bastaya

In series, resistances add up and the current is shared; in parallel, conductances add up and the voltage is shared. Every network reduces to these two rules.

In series the same current flows through every resistor: resistances add up and the voltage is shared in proportion to each (voltage divider).

In parallel all branches are at the same voltage: currents add up and the equivalent resistance is smaller than the smallest branch. A mixed network is reduced step by step. The two wires of a line are in series with the load: they cause a voltage drop 2·R_l·I.

Formulas

Whatever the network

Ohm's law on each resistorUn = Rn · In
In = UnRn
Rn = UnIn
QuantitySymbolUnit
Voltage across resistor nUnV
Resistor nRnΩ
Current through itInA

Every resistor obeys Ohm's law with its own voltage and current, in series as in parallel.

Equivalent resistanceRéq = UI
QuantitySymbolUnit
Equivalent resistanceRéqΩ
Voltage across the networkUV
Total currentIA

Req is the single resistor that, at the same voltage U, would carry the same current I.

Power in each resistorPn = Un · In
Pn = Rn · I
Pn = URn
QuantitySymbolUnit
Power dissipated by resistor nPnW
Power balanceP = P₁ + P₂ + ...
P = U · I
QuantitySymbolUnit
Total powerPW

Powers always add up, in series, in parallel or in a mixed network.

In series

Equivalent resistanceRéq = R₁ + R₂ + ...
QuantitySymbolUnit
Equivalent resistanceRéqΩ
Common and split quantitiesI = I₁ = I₂ = ...
U = U₁ + U₂ + ...
QuantitySymbolUnit
Current (common)IA
Total voltage (split)UV

In series the current I is common to every resistor; the voltage U is split between them.

Voltage across each resistorU = Réq · I
U₁ = R₁ · I
Un = Rn · I
QuantitySymbolUnit
Voltage across resistor nUnV
Resistor nRnΩ
CurrentIA
CurrentI = URéq
I₁ = U₁R₁
In = UnRn
QuantitySymbolUnit
CurrentIA
Total voltageUV
Equivalent resistanceRéqΩ
Each resistanceRéq = UI
R₁ = U₁I
Rn = UnI
QuantitySymbolUnit
Resistor nRnΩ
Voltage across resistor nUnV
CurrentIA
Voltage dividerU₁ = U · R₁R₁ + R₂
QuantitySymbolUnit
Voltage on R₁U₁V
Total voltageUV

In parallel

Equivalent resistance1Réq = 1R₁ + 1R₂ + ...
QuantitySymbolUnit
Equivalent resistanceRéqΩ

Two resistors: Req = R₁·R₂ / (R₁ + R₂).

Common and split quantitiesU = U₁ = U₂ = ...
I = I₁ + I₂ + ...
QuantitySymbolUnit
Voltage (common)UV
Total current (split)IA

In parallel the voltage U is common to every branch; the current I is split between them.

Current in each branchI = URéq
I₁ = UR₁
In = URn
QuantitySymbolUnit
Current in branch nInA
Voltage (common)UV
Resistance of branch nRnΩ

The branch with the smallest resistance carries the largest current.

VoltageU = Réq · I
U = R₁ · I₁ = R₂ · I₂ = ... = Rn · In
QuantitySymbolUnit
Voltage (common)UV
Total currentIA
Equivalent resistanceRéqΩ
Resistance of each branchRéq = UI
R₁ = UI₁
Rn = UIn
QuantitySymbolUnit
Resistance of branch nRnΩ
Voltage (common)UV
Current in branch nInA
Current dividerI₁ = I · R₂R₁ + R₂
QuantitySymbolUnit
Current in R₁I₁A
Total currentIA

Two branches: the current splits inversely to the resistances (I₁ gets R₂'s share).

n identical resistorsRéq = Rn
QuantitySymbolUnit
Equivalent resistanceRéqΩ
Resistance of each branchRΩ
Number of resistorsn

Mixed network

Step-by-step reductionR₂₃ = R₂ · R₃R₂ + R₃
Réq = R₁ + R₂₃
QuantitySymbolUnit
Equivalent resistance of R₂ ∥ R₃R₂₃Ω
Total equivalent resistanceRéqΩ

Example: R₁ in series with R₂ ∥ R₃. Replace each series or parallel group by its equivalent resistance until a single resistor remains.

Other case: parallel then seriesR₂₃ = R₂ + R₃
Réq = R₁ · R₂₃R₁ + R₂₃
QuantitySymbolUnit
Equivalent resistance of R₂ + R₃R₂₃Ω
Total equivalent resistanceRéqΩ

R₁ in parallel with the R₂ + R₃ branch: reduce the series branch first, then the parallel.

Total currentI = URéq
QuantitySymbolUnit
Current delivered by the generatorIA
Generator voltageUV
Back down to each resistorU₁ = R₁ · I
U₂₃ = R₂₃ · I
I₂ = U₂₃R₂
I₃ = U₂₃R₃
QuantitySymbolUnit
Voltage on R₁U₁V
Voltage shared by R₂ and R₃U₂₃V
Current in R₂I₂A

Walk back the other way: a series group gets the common current (U = R · I), a parallel group gets the common voltage (I = U / R). Check: U₁ + U₂₃ = U and I₂ + I₃ = I.

Power line

Line voltage dropΔU = 2 · Rl · I
QuantitySymbolUnit
Voltage dropΔUV
Resistance of one wireRlΩ
CurrentIA

Worked example

R₁ = 100 Ω is in series with the group R₂ = 220 Ω ∥ R₃ = 330 Ω, all under U = 12 V. Find the equivalent resistance, the total current, then the voltage and current of each resistor.

Parallel first: R₂₃ = 220 × 330 / (220 + 330) = 132 Ω. Then series: Req = 100 + 132 = 232 Ω.

I = U / Req = 12 / 232 = 51.7 mA.

U₁ = R₁ · I = 100 × 0.0517 = 5.17 V; U₂₃ = 132 × 0.0517 = 6.83 V (check: 5.17 + 6.83 = 12 V).

I₂ = U₂₃ / R₂ = 6.83 / 220 = 31.0 mA; I₃ = 6.83 / 330 = 20.7 mA (check: 31.0 + 20.7 = 51.7 mA).

Common mistakes

  • Adding parallel resistors as if they were in series: in parallel, the reciprocals add up, and Req is smaller than the smallest branch.
  • Forgetting to invert back: 1/Req = 0.00758 is not the answer, Req = 1 / 0.00758 = 132 Ω.
  • Applying the voltage divider to parallel resistors: they share the same voltage, it is the current that splits.

IEC symbols

Resistor

Mini circuit

Frequently asked questions

Why is the equivalent resistance smaller in parallel?
Each branch offers an extra path to the current: under the same voltage the total current is larger, so U/I is smaller. Two equal resistors in parallel are worth half of one.
Are the lamps of a house in series or in parallel?
In parallel: each receives the 230 V of the mains and works independently of the others. In series, switching one lamp off would switch off all the others, and each would receive only a fraction of the voltage.

71 exercises in this topic

Simulated time00:00:00
Q = I·t-
W = P·t-

Workbench

Circuit diagram CEI 60617

How does it work?

The perfboard: each big hole is a circuit node. You push a single leg of a component (resistor, lamp...) into it. The 4 small holes around it are connected to it: that is where chips and leads plug in.

  1. Drag a component onto the board: it snaps onto the grid. R rotates it.
  2. To join neighbouring big holes, click Jumper chip in the palette (or C) then drag on the board: a line of chips is laid at once. Bridged holes become a single node.
  3. For long links and for the power supply (placed next to the board), drag a lead from one big hole to another (or to a terminal).
  4. As soon as a loop is closed, the circuit is solved in real time (Ohm + Kirchhoff) and the diagram follows.
  5. Zoom with the wheel (or + / , two-finger pinch); drag the background to pan, 0 fits the board. The + buttons around the board add a row or a column.

Del delete · R rotate · C chip brush · Esc cancel · wheel zoom · drag the background to pan

Confirmer

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