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Capacitance

Overview

Source: Yong P. Chen, PhD, Department of Physics & Astronomy, College of Science, Purdue University, West Lafayette, IN

This experiment will use commercial capacitors and a parallel plate capacitor to demonstrate the concept of capacitance. A capacitor stores opposite charges on two conductors, for example two opposite metal plates, leading to a potential difference (voltage drop) between the two conductors. The amount of charge on each conductor is proportional to this voltage drop, with the capacitance as the proportionality factor. If the voltage is changing with time, the current flowing into the capacitor will be proportional to the rate of that change, and again the capacitance is the proportionality factor.

The capacitance of the parallel plate capacitor is the product of the dielectric constant with the distance between the plates divided by the area of the plate. This experiment will demonstrate the proportionality with distance by first depositing some charge onto the capacitor and then using a high-impedance voltmeter (electrometer) to monitor the voltage between the plates as the distance is increased. The voltage change will also be monitored with a dielectric material, such as a plastic plate inserted into the space between the metal plates.

A capacitance meter will be used to directly measure the capacitance, as well as to measure parallel and series connections of commercially-available capacitors and to study how the total capacitance is related to individual capacitances.

Procedure

1. Charging a Capacitor

  1. Obtain a commercial capacitor with capacitance C = 470 µF (or some similar value), a programmable voltage source, and an amp-meter (or multi-meter that can measure current).
  2. With the voltage source set to 0 V, connect the "+" terminal of the voltage source to one terminal of the capacitor, with the amp-meter in between, and connect the "−" terminal of the voltage source to the other terminal, as in Figure 1. The connect

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Results

For a capacitor, a plot of current I versus ramp rate ΔV/Δt is linear, as shown in Figure 7. Since the current is the rate of the change in the charge Q on one conductor terminal, this also reflects the linear relationship between charge Q and voltage V for a capacitor (Equation 1). The slope of the line is equal to the capacitance of the capacitor (Equation 2).

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Application and Summary

In this experiment, the charging of a capacitor was demonstrated, where the current is the product of the capacitance and the rate of change of voltage. By observing how the voltage varies given a fixed charge, we have demonstrated how the capacitance of a parallel plate capacitor varies with the separation and with the medium between the plates.

The capacitance meter can also be used to directly measure the capacitance, and determine the total capacitance for capacitors connected in parallel

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Tags
CapacitanceCapacitorVoltageChargesConductive TerminalsInsulating MaterialParallel Plate CapacitorCurrentElectronsFaradsCharge StoragePower SourceNetwork ConfigurationCharging CurrentPhysical FactorsMagnitude Of VoltageVoltage FluctuationCurrent Flow

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0:06

Overview

1:03

Principles of Capacitance

3:11

Charging the Capacitor

4:47

Tuning the capacitance

5:56

Data Analysis and Results

7:12

Applications

8:30

Summary

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