Kirchhoff's Current Law at a Series Junction (I₁ = I₂)

A fixed two-resistor series branch carries one unknown loop current. Record noisy ammeter readings I₁ and I₂ for several supply voltages; a linear fit of I₂ versus I₁ should recover unit slope — KCL at the intermediate node.

School· 24 min·Related simulator: Electricity & MagnetismKirchhoff's Laws (KCL & KVL)

Goal

Verify that in a series branch the current entering the junction equals the current leaving it (KCL): expect I₁ = I₂ within measurement error, i.e. slope ≈ 1 for I₂ plotted against I₁.

Equipment

  • Ideal DC voltage source
  • Fixed resistors R₁ = 220 Ω, R₂ = 330 Ω
  • Two ammeters in series (simulated)
  • Common ground

Theory

In steady-state DC, Kirchhoff's current law (KCL) states that the algebraic sum of currents into any node is zero. For a simple series connection of two resistors between two nodes, the single loop current is the same everywhere along the branch, so the readings on two ammeters wired in series must agree (up to instrument error).

Procedure

  1. The bench uses a fixed series pair R₁ = 220 Ω and R₂ = 330 Ω between the ideal supply and ground (topology matches the “series only” mode of the related simulator).
  2. Set the supply voltage V with the slider (try several values between about 5 V and 22 V).
  3. Press “Record measurement” to log (V, I₁, I₂) with small independent ammeter noise.
  4. Repeat for at least 6 different voltages spread across the range.
  5. Inspect the linear fit of I₂ versus I₁: the slope should be close to 1 (KCL); the intercept should be close to 0.
  6. Compare the fitted slope with the ideal 1 and write the conclusion.

Experiment

Conclusion

The fitted slope agrees with unity within tolerance, supporting KCL for this series junction. Residual mismatch comes from independent ammeter noise and a finite number of voltage points.