Objective and use case
What you’ll build: This experiment allows you to observe and measure the charging and discharging of a capacitor through resistors using a breadboard setup. You’ll gain hands-on experience with basic electronic components and measurement techniques.
Why it matters / Use cases
- Understanding the RC time constant in circuits helps in designing filters and timing applications.
- Measuring capacitor behavior is crucial for applications in power supply circuits and energy storage systems.
- This experiment provides foundational knowledge for students pursuing electronics or electrical engineering.
- Observing real-time voltage changes reinforces theoretical concepts of capacitance and resistance.
Expected outcome
- Measure the capacitor voltage (V_C) reaching approximately 3.3 V after one time constant (τ = R1 × C1).
- Observe the discharge curve on an oscilloscope, confirming the exponential decay of voltage over time.
- Record the time taken for the capacitor to charge to 63% of the supply voltage (approximately 3.2 V).
- Determine the discharge time to reach 36.8% of the initial voltage, validating the RC time constant.
Audience: Beginners in electronics; Level: Basic
Architecture/flow: Breadboard setup with a DC power supply, resistors, capacitor, pushbutton switch, and measurement tools (multimeter/oscilloscope).
Materials
- 1× Breadboard
- 1× DC power supply, +5 V (or USB 5 V with breakout)
- 1× R1 = 1 kΩ, 1/4 W resistor (charge path)
- 1× R2 = 1 kΩ, 1/4 W resistor (discharge path)
- 1× C1 = 100 µF, ≥16 V electrolytic capacitor
- 1× S1 = Pushbutton (normally open, NO)
- 6× Jumper wires
- 1× Multimeter (DC volts) and/or 1× Oscilloscope with probe
Wiring guide
- Place R1 so one end will go to +5 V and the other to a central node (the capacitor node).
- Connect the free end of R1 to a free row that will be the node V_C (capacitor node).
- Insert C1 so its positive lead goes to node V_C and its negative lead goes to the ground rail. Observe polarity: “+” to V_C, “−” to GND.
- Build the discharge branch: connect one end of R2 to node V_C; connect the other end of R2 to one terminal of S1; connect the other terminal of S1 to the ground rail.
- Connect the power supply +5 V to the breadboard’s +V rail and the supply ground to the GND rail.
- Abbreviations used in the schematic:
- V_C = capacitor voltage at the node (measure here with the red probe).
- REF = reference ground point (connect black probe here).
- For a multimeter: set to DC volts, red probe to the black dot labeled V_C, black probe to the black dot labeled REF.
- For an oscilloscope: CH1 probe tip to V_C, CH1 ground clip to REF; timebase around 50 ms/div to 200 ms/div to see the RC curve.
Schematic
+5 V
│
┌┴┐
│ │ S1 = Pulsador NA (carga)
│ │
└┬┘
│
┌┴┐
│ │ R1 = 10 kΩ (carga)
│ │
└┬┘
│
● V_C
├───────────────┬
│ │
│ ┌┴┐
│ │ │ S2 = Pulsador NA (descarga)
│ │ │
│ └┬┘
│ │
┌┴┐ ┌┴┐
│ │ │ │ R2 = 10 kΩ (descarga)
│ │ C1 = │ │
│ │ 100 μF └┬┘
└┬┘ │
│ │
GND GND
Measurements and tests
-
Before powering on:
- Verify C1 polarity: positive to V_C, negative to GND.
- Confirm there is no short between +V and GND with the multimeter continuity mode (power supply off).
-
Charging (R1–C1):
- Power on +5 V with S1 released (open).
- Observe V_C:
- With a multimeter: V_C will rise smoothly toward +5 V.
- With an oscilloscope: an exponential rise V_C(t) = 5 V · (1 − e^(−t/τ)).
- The time constant τ_charge = R1·C1 = 1 kΩ · 100 µF ≈ 0.10 s (100 ms).
- Check points:
- At t = τ (≈0.1 s), V_C ≈ 0.63 · 5 V ≈ 3.15 V.
- By t ≈ 5τ (≈0.5 s), V_C ≈ 99% of 5 V.
-
Discharging (R2–S1–C1):
- Press and hold S1 to connect R2 to GND and discharge the capacitor.
- Observe V_C:
- With a multimeter: V_C will fall toward 0 V.
- With an oscilloscope: an exponential decay V_C(t) = V0 · e^(−t/τ).
- The time constant τ_discharge = R2·C1 = 1 kΩ · 100 µF ≈ 0.10 s.
- Check points:
- At t = τ (≈0.1 s) after pressing S1, V_C ≈ 37% of its initial value.
- After ≈5τ (≈0.5 s), V_C is near 0 V.
-
Repeatability and symmetry:
- Release S1 to let the capacitor charge again through R1.
- Compare charge and discharge curves; with R1 = R2, the time constants should match.
-
Optional checks:
- Change R1 or R2 (e.g., to 4.7 kΩ) and verify τ scales linearly with R.
- Try a smaller capacitor (10 µF) and note the faster transitions.
Common mistakes
- Reversing the electrolytic capacitor polarity (can damage the capacitor).
- Forgetting the ground reference for the meter/scope (always connect to REF).
- Misplacing the pushbutton so its internal contacts short +V to GND; ensure S1 is only between R2 and GND.
- Using a multimeter in current mode across the capacitor node V_C (will short the circuit). Use voltage mode.
Safety notes
- Keep the supply at 5 V. Higher voltages increase inrush/discharge currents and stress components.
- Always discharge C1 (hold S1 for a second) before re-wiring.
- Do not short V_C directly to GND without a resistor; R2 limits discharge current.
Improvements
- Replace S1+R2 with an SPDT toggle to select CHARGE (to +V via R1) or DISCHARGE (to GND via R2) hands-free.
- Add an LED with a series resistor from V_C to GND to visualize the charge level; note it will slightly alter τ.
- Use a data acquisition or oscilloscope cursors to measure τ accurately and compare with R·C.
More Practical Cases on Prometeo.blog
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