MTBuilder AcademyLearn it. Test it. Build it.
Electricity & powerLesson 11 of 48
Practice65 minutes2 project connections

Capacitance and transients

Predict first-order charge and discharge behavior to choose a timing or filtering capacitor without mistaking a transient model for an ideal delay.

After this lesson, you can
  • Calculate an RC time constant, estimate transient voltages, and diagnose a capacitor polarity, leakage, or connection fault from a measured curve.
ReadPracticedBench demonstrated
01

Understand

The working idea

A capacitor stores separated charge and therefore energy in an electric field. Its defining relation is Q = CV: at a given voltage V, a larger capacitance C stores more charge Q. Current describes how quickly charge changes, so i = C dV/dt. A capacitor's voltage cannot jump instantaneously in the ideal model unless infinite current is available. This makes capacitors useful for smoothing noise, holding a reference briefly, and shaping timing.

In a resistor-capacitor circuit driven by a DC step from 0 to V_s, capacitor voltage is V_C(t) = V_s(1 − e^(−t/RC)). The time constant τ = RC has units Ω·F = s. After one τ, voltage reaches about 63% of its final value; after five τ, it is above 99% in the ideal model. During discharge from V_0 through R, V_C(t) = V_0e^(−t/RC). There is no sharp “finished” instant.

Suppose a sensor input chatters from short glitches. A 10 kΩ resistor with 10 µF gives τ = 0.10 s, which may suppress very brief events but also delays genuine changes. That latency is a build tradeoff, not free filtering. Real capacitors have tolerance, leakage, equivalent series resistance, and voltage limits. Polarized electrolytics must be oriented correctly.

A common misconception is that capacitance blocks all DC immediately. During charging, current flows; after settling in the ideal DC case, it approaches zero. Another failure is reading 100 µF as 100 F or assuming the nominal time constant is an exact measured delay. Use the curve, define a threshold, and account for component tolerance and source/load resistance. The associated RC simulation is a bounded ideal first-order model: it does not include every parasitic or instrument-loading effect.

02

Follow the reasoning

Worked example

A 47 kΩ resistor charges a 10 µF capacitor from a 5 V step. Find τ and ideal capacitor voltage after one τ and two τ.

  1. 1

    Convert values: 47 kΩ = 47,000 Ω and 10 µF = 10×10^-6 F.

  2. 2

    τ = RC = 47,000 × 10×10^-6 s = 0.47 s.

  3. 3

    At t = τ, V_C = 5(1 − e^-1) ≈ 3.16 V.

  4. 4

    At t = 2τ, V_C = 5(1 − e^-2) ≈ 4.32 V.

Result

The time constant is 0.47 s; ideal voltage is about 3.16 V at 0.47 s and 4.32 V at 0.94 s.

Sanity checkBoth voltages lie between 0 and 5 V, increase with time, and approach rather than exceed the supply.

03

Try it yourself

Independent check

If R doubles while C and the source stay unchanged, what happens to the ideal RC charging curve?
04

Move to the bench

Compare a measured low-voltage RC charge curve with the ideal time-constant prediction.

Gather
  • 3×AA battery holder
  • 47 kΩ resistor
  • 10 µF electrolytic capacitor rated above 5 V
  • multimeter
  • breadboard
  • timer
  • jumper wires

Experiment

  1. With power absent, confirm capacitor polarity and build the series resistor-capacitor circuit; calculate τ from measured or nominal values.
  2. Discharge the capacitor through the resistor, then apply the battery and record actual capacitor voltage at 0, 0.5τ, 1τ, 2τ, and 5τ.
  3. Compare readings with ideal expected values and note meter timing and component tolerance.
  4. Remove power, discharge safely, then deliberately move the resistor so the capacitor has no charging path; repower and diagnose the flat or erratic trace as an open-path fault.
  5. Restore the path and repeat one checkpoint.

Observe

  • Expected ideal values are about 39%, 63%, 86%, and 99% of final voltage at 0.5τ, 1τ, 2τ, and 5τ; actual readings must be kept distinct.
  • Expected fault clue: an open charging path prevents the smooth rise and may leave a residual voltage determined by leakage and the meter.
Transfer it

Choose R or C to target a 50 ms time constant for suppressing a brief button glitch, then state the response delay that choice introduces.

Limits and cautions
  • Use only the low-voltage battery holder and orient the electrolytic capacitor correctly.
  • Remove power and discharge through the resistor before rewiring; never short a charged capacitor directly.
05

Keep evidence

Bench note

Record what you expected, what you actually measured or observed, and one difference worth investigating. This is self-reported evidence, not a certification.

0 / 5,000A bench demonstration needs a concrete note of at least 20 characters.
Terms in this lessonBrowse the advanced glossary

Sources and further reading

  1. MIT OpenCourseWare: Circuits and Electronics