Labo Élec

electrical lab simulator

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Formulas

All formulas

Basics & units

Usual prefixesk = 10³
m = 10⁻³
µ = 10⁻⁶
n = 10⁻⁹
QuantitySymbolUnit
VoltageUV
CurrentIA
ResistanceRΩ
PowerPW
EnergyWJ
Ampere-hour and kilowatt-hour1 Ah = 3 600 C
1 kWh = 3,6 × 10⁶ J
QuantitySymbolUnit
Quantity of electricityQC
EnergyWJ

Electrostatics

Coulomb's lawF = k · q · q'
QuantitySymbolUnit
ForceFN
ChargeqC
Distancedm
Constant (9 × 10⁹)kN·m²/C²
Field between two platesE = Ue
QuantitySymbolUnit
Electric fieldEV/m
VoltageUV
Plate spacingem
Force on a chargeF = q · E
QuantitySymbolUnit
ForceFN
ChargeqC
Electric fieldEV/m

Voltage & current

Quantity of electricityQ = I · t
QuantitySymbolUnit
Quantity of electricityQC
CurrentIA
Timets
Current densityJ = IS
QuantitySymbolUnit
Current densityJA/mm²
CurrentIA
Cross-sectionSmm²
Cross-section of a round wireS = π ·4
QuantitySymbolUnit
Cross-sectionSmm²
Diameterdmm

Ohm's law & resistance

Ohm's lawU = R · I
QuantitySymbolUnit
VoltageUV
ResistanceRΩ
CurrentIA
Pouillet's lawR = ρ · lS
QuantitySymbolUnit
ResistanceRΩ
ResistivityρΩ·m
Lengthlm
Cross-sectionS

Copper ρ ≈ 1.7 × 10⁻⁸ Ω·m; aluminium 2.8 × 10⁻⁸; iron 1.0 × 10⁻⁷.

Temperature effectR = R₀ · (1 + α · Δθ)
QuantitySymbolUnit
Resistance at 20 °CR₀Ω
Temperature coefficientα/°C
Temperature changeΔθ°C

Power, energy, efficiency

Electrical powerP = U · I
QuantitySymbolUnit
PowerPW
VoltageUV
CurrentIA
Joule heatingP = R · I² = R
QuantitySymbolUnit
PowerPW
ResistanceRΩ
CurrentIA
EnergyW = P · t
QuantitySymbolUnit
EnergyWJ
PowerPW
Timets

In kWh: power in kW × time in hours.

Efficiencyη = PuPa
QuantitySymbolUnit
Efficiencyη-
Useful powerPuW
Absorbed powerPaW

Resistor networks

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

Real generators & loads

Real generatorU = E − r · I
QuantitySymbolUnit
EMFEV
Internal resistancerΩ
Terminal voltageUV
Active loadU = E' + r' · I
QuantitySymbolUnit
Back-EMFE'V
Internal resistancer'Ω
Generalised Ohm's lawI = ΣE − ΣE'ΣR
QuantitySymbolUnit
CurrentIA
Sum of loop resistancesΣRΩ
CharacteristicU = f(I) : droite de pente −r, ordonnée à l'origine E

Kirchhoff's laws

Junction ruleΣ I entrants = Σ I sortants
QuantitySymbolUnit
CurrentIA
Loop ruleΣ E − Σ R · I = 0
QuantitySymbolUnit
EMFEV
Voltage dropR·IV

Capacitors

CapacitanceQ = C · U
QuantitySymbolUnit
ChargeQC
CapacitanceCF
VoltageUV
Stored energyW = ½ · C ·
QuantitySymbolUnit
EnergyWJ
Combinationsparallèle : Céq = C₁ + C₂
série : 1Céq = 1C₁ + 1C₂
QuantitySymbolUnit
Equivalent capacitanceCéqF
RC time constantτ = R · C
QuantitySymbolUnit
Time constantτs
ResistanceRΩ
CapacitanceCF

3-digit marking: two digits then number of zeros, in pF (104 = 100 000 pF = 100 nF).

Magnetism & electromagnetism

Magnetic fluxΦ = B · S
QuantitySymbolUnit
FluxΦWb
Magnetic flux densityBT
AreaS
Field of a long coilB = µ₀ · N · Il
QuantitySymbolUnit
Vacuum permeability (4π × 10⁻⁷)µ₀T·m/A
Number of turnsN-
Lengthlm
Laplace forceF = B · I · l
QuantitySymbolUnit
ForceFN
CurrentIA
Conductor lengthlm

Induction & self-induction

Faraday's lawE = −N · ΔΦΔt
QuantitySymbolUnit
Induced EMFEV
Number of turnsN-
FluxΦWb
Timets
Cut fluxE = B · l · v
QuantitySymbolUnit
Magnetic flux densityBT
Lengthlm
Speedvm/s
Self-inductionE = −L · ΔIΔt
QuantitySymbolUnit
InductanceLH
CurrentIA
Energy of a coilW = ½ · L ·
QuantitySymbolUnit
EnergyWJ
RL time constantτ = LR
QuantitySymbolUnit
Time constantτs

Alternating current

Sinusoidal quantityu(t) = Umax · sin(ω · t + φ)
QuantitySymbolUnit
Peak valueUmaxV
Angular frequencyωrad/s
Initial phaseφrad
Angular frequency, frequency, periodω = 2 · π · f
f = 1T
QuantitySymbolUnit
FrequencyfHz
PeriodTs
RMS valueUeff = Umax√2
QuantitySymbolUnit
RMS valueUeffV
Peak valueUmaxV

RLC circuits

ReactancesXL = L · ω
XC = 1C · ω
QuantitySymbolUnit
ReactanceXΩ
InductanceLH
CapacitanceCF
Angular frequencyωrad/s
Series impedanceZ = √(R² + (XL − XC)²)
QuantitySymbolUnit
ImpedanceZΩ
ResistanceRΩ
Ohm's law in ACU = Z · I
QuantitySymbolUnit
RMS voltageUV
RMS currentIA
Phase shifttan φ = XL − XCR
cos φ = RZ
QuantitySymbolUnit
Phase shiftφrad

AC power

The three powersS = U · I
P = U · I · cos φ
Q = U · I · sin φ
QuantitySymbolUnit
Apparent powerSVA
Active powerPW
Reactive powerQvar
Power triangleS² = P² + Q²
cos φ = PS
QuantitySymbolUnit
Power factorcos φ-
Power factor correctionC = P · (tan φ₁ − tan φ₂)· ω
QuantitySymbolUnit
Capacitance to addCF
Phase shifts before / afterφ₁, φ₂rad

Measurement & instruments

Reading a dialvaleur = divisions luesdivisions totales × calibre
Ammeter shuntRs = rA · iI − i
QuantitySymbolUnit
Shunt resistanceRsΩ
Ammeter resistancerAΩ
Full-scale currentiA
Total current to measureIA
Series multiplier (voltmeter)Radd = Ui − rV
QuantitySymbolUnit
Series multiplierRaddΩ
Voltmeter resistancerVΩ
Volt-ammeter methodR = UI
QuantitySymbolUnit
Measured resistanceRΩ

Downstream: the voltmeter is across R alone (error from the current shunted by V); upstream: the voltmeter spans A (error from the drop in A).

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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