Virtual engineering lab

RL Time-Constant Measurement

Measure current build-up in a series RL circuit and compare the sampled 63.2% crossing with the analytic time constant τ = L/R.

Electrical Engineering / InstrumentationintroductoryValidated educational model
Learning mode

Guided laboratory

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Integrated virtual bench

RL transient bench

Ideal instruments
Source

Bench power supply

Output voltage
Current limit
Mode check
CV expected
DMM

Resistance check

COM + VΩ · circuit unpowered

Confirm the modeled series resistance before applying the source.

Oscilloscope

Transient response

Adjust experiment parameters to preview the ideal response, then run the experiment for validation.

Device under test

Series R–L network

RLsourcereturn
Analytic τ
63.2% measurement
Current-limit margin
Measurements

Instrument readings

Analytic time constant
RL time constant calculated from L/R.
Scope-measured time constant
Interpolated 63.2% crossing from the sampled current waveform.
Final current
Ideal steady-state current VS/R.
Initial inductor voltage
Ideal inductor voltage immediately after the source step.
DMM resistance check
Independent resistance reading before energizing the circuit.
Current-limit margin
Bench-supply current limit minus steady-state current.
Result visualization

Transient measurement check

Compare the analytic first-order time constant with the oscilloscope-style 63.2% crossing and verify the source current-limit margin.

Analytic τ
Measured τ
Final current
Current-limit margin

Independent check: I(τ) = 0.6321(VS/R) and τ = L/R.

Theory

Equations and model

First-order inductor current rise

An ideal inductor initially opposes a sudden current change. In a series RL circuit the current rises exponentially toward VS/R.

τ = L/RI(t) = (VS/R)(1 − e^(−tR/L))I(τ) = 0.6321 VS/R

Oscilloscope current measurement

A scope measures voltage, so the lab uses the voltage across the known series resistor as a current-sense signal.

VR(t) = I(t)RI(t) = VR(t)/R
Validation

Independent checks

RL time-constant checkNot run

Compares the sampled 63.2% current crossing with τ = L/R.

Expected
Simulated
Error
Tolerance
0.25%

Run the experiment to perform this check.

Engineering interpretation

Run the experiment to generate an engineering interpretation.

Assumptions and limitations
Assumptions
  • Ideal resistor and inductor.
  • Ideal DC step source provided the current limit is not reached.
  • Inductor winding resistance is represented only by the explicit series resistor.
  • No magnetic saturation, parasitic capacitance, or source/wiring inductance.
Limitations
  • Current-limited RL response is detected and rejected instead of being solved in Phase 1.6.
  • Core loss, saturation, winding resistance, noise, and measurement non-idealities arrive in later work.
Local experiment export

Save your measurements and setup

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Phase 1.9
Settings JSON
Current parameter values for reproducibility and later project handoff.
Measurements CSV
Completed instrument readings with labels, units, and descriptions.
Plot PNG
The current canvas-based scope, transient, sweep, or statistics visualization when available.
Summary
Markdown report with objectives, setup, measurements, validation, interpretation, assumptions, and graded guided concept-check results.

Ready to export the current local experiment state.

Learning objectives

What this experiment should establish

  • Predict an RL time constant from inductance and series resistance.
  • Relate resistor voltage to circuit current for oscilloscope measurement.
  • Verify that the bench-supply current limit exceeds the steady-state RL current.
  • Compare measured and analytic time constants.
Check your understanding

Questions to answer from the experiment

  1. Why is the ideal inductor current still zero at the instant immediately after the voltage step?
  2. What happens to the RL time constant if series resistance doubles?
  3. Why is voltage across the series resistor a useful way to observe current with an oscilloscope?
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