Physic Labs

Electricity and magnetism

Series and parallel circuits

Measure current and voltage in two-resistor series then parallel circuits. Verify Rs=R1+R2R_s=R_1+R_2, 1/Rp=1/R1+1/R21/R_p=1/R_1+1/R_2, and Kirchhoff's current/voltage rules.

Middle school

⚠ Real circuits: use only low-voltage supplies, connect a voltmeter in parallel and an ammeter in series — a wrongly placed ammeter can short the circuit.

Equipment

  • Two-resistor circuit model with the «Switch to parallel» button
  • Source-voltage, R₁, and R₂ sliders
  • Virtual ammeter/voltmeter and branch readouts

Procedure

  1. Explore the series circuit

    Set U = 9 V, R₁ = 3 Ω, R₂ = 6 Ω. Read the current through each resistor — identical, I=U/(R1+R2)=0.6I=U/(R_1+R_2)=0.6 A — and the voltage across each: U1=1.8U_1=1.8 V, U2=3.6U_2=3.6 V, summing to 9 V (Kirchhoff's loop rule).

  2. Switch to parallel

    Press «Switch to parallel», keeping U, R₁, R₂. Both branches see the same 9 V; read branch currents I1=U/R1=3I_1=U/R_1=3 A, I2=1.5I_2=1.5 A; the total I=I1+I2=4.5I=I_1+I_2=4.5 A (Kirchhoff's junction rule). Equivalent resistance Rp=U/I=2R_p=U/I=2 Ω — matching 1/Rp=1/3+1/61/R_p=1/3+1/6.

  3. Compare power and brightness

    In panel 2, watch the charge carriers in the branches and compare their «crowding» — a picture of current. Compute P=UIP=UI for each configuration: parallel dissipates much more power than series because Rp<RsR_p<R_s — which is why home lamps are wired in parallel.

  4. Predict with chosen values

    Pick any U, R₁, R₂; compute Is=U/(R1+R2)I_s=U/(R_1+R_2) and Ip=U/R1+U/R2I_p=U/R_1+U/R_2 beforehand, then toggle the mode to check. Try the limit R₂ → 1 Ω in parallel: that branch «dominates» the current — the small resistor rules in parallel, the large one in series.

Simulation

Experiment history

The resistor-combination rules are direct consequences of the two Kirchhoff laws that Gustav Kirchhoff, aged 21, stated in 1845 in a paper on branched circuits — only 18 years after Ohm's still-controversial law. Kirchhoff founded general circuit analysis before electronics even existed. Its first spectacular application was transatlantic telegraphy in the 1850s–60s, where Kirchhoff and Thomson (Lord Kelvin) analyzed currents on submarine cables. Today the junction/loop rules are the language of every circuit analysis — from phone boards to national power grids — and a textbook example of charge and energy conservation.

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