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.
A capacitor consists of two separated conductors and its capacitance C represents its "capacity to store charge". Applying a voltage difference V between these two conductors can induce charge +Q on one conductor and Q on the other conductor (so the total charge is zero, that is, the capacitor as a whole is charge neutral), such that:
Note here that Q is the charge on one conductor (not the total charge on both conductors which would be 0). If the voltage V is changing with time, so will the charge Q. If V and Q change by ΔV and ΔQ, respectively in a time interval Δt, then,
ΔQ = C • ΔV
Since ΔQ/Δt is the current (called "charging current") flowing into the positively charged conductor of the capacitor, then as shown in Equation 2:
This means the capacitance is the proportionality factor to convert the rate of voltage change (ΔV/Δt) to the current flowing into the capacitor (see Figure 1).
The capacitance can also be measured directly using a capacitance meter (for example, using the capacitance measurement mode of a multi-meter or "LCR meter"; see Figure 2).
The simplest kind of capacitor, depicted in Figures 1 and 2, consists of two parallel conducting plates, and is called a "parallel plate capacitor". Its capacitance C is given by Equation 3
where A is the area of the plate, d is the separation between the plates, and is the dielectric constant of the medium between the two plates (or "filling" the capacitor). The medium needs to be electrically insulating. For a vacuum,
This value is commonly denoted as ε0, which also describes ε of air to a good approximation. Other medium, such as oil, generally have a larger ε, which is scaled from the vacuum value ε0 quoted above by a factor larger than one. This factor is known as the "relative" dielectric constant or permittivity of the medium and commonly denoted as κ. Such a medium is also generally referred to as a "dielectric material".
Therefore, for a parallel plate capacitor:
If the charge Q is fixed, then increasing the plate-plate separation d will increase the voltage V (in proportion to d):
Capacitors can be connected in parallel or series just like resistors. The total "effective" capacitance is related to individual capacitances in a parallel or series connection similar to how electrical conductance of a parallel/series resistor connection is related to individual conductances. Thus, for two capacitors with capacitances C1 and C2, the total capacitance for a parallel connection is equal to the sum of the two capacitances. Or,
For a series connection,
These two kinds of connections are depicted in Figures 3 and 4.
Figure 1: Diagram showing a capacitor connected to a voltage source used to charge the capacitor, and an amp-meter to read the current.
Figure 2: Diagram showing a capacitance meter connected to a capacitor to directly measure its capacitance.
1. Charging a Capacitor
- 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).
- 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 connection can be made with cables with clamps or banana plugs into receiving ports on the capacitor and instruments.
- Switch the voltage source from 0 V to 1 V (in about 1 s), and observe the transient current reading on the amp-meter. Do the same for 2 V, 5 V, and 10 V (for each target voltage; this means first go back to 0 V, then switch to the target voltage in about 1 s). Note that the transient current is larger for a larger target voltage, as expected from Equation 2.
- Program the voltage source to generate a voltage ramp from 0 V to 10 V in 5 s, and record the "steady state" reading of the amp-meter during the middle of the ramp. Repeat for a ramp time of 10 s, 20 s, and 30 s. Plot the observed current versus the voltage ramp rate (in V/s).
2. Tuning the Capacitance
- Turn off the voltage source and replace it with a 300 V battery, and replace the amp-meter by a 1 MΩ resistor (the purpose of this resistor is to provide extra protection to limit the current in the circuit); also replace the commercial capacitor with a parallel plate capacitor with an adjustable separation between the plates.
- Obtain a high-impedance voltmeter (or "electrometer") and connect it to measure the voltage difference V between the two plates (the high impedance impedes the discharge of the capacitor during the experiment when the electrometer is connected). See Figure 5.
- Connect the 300 V battery to the parallel plate capacitor, wait until the electrometer reaches the steady state of 300 V (now the capacitor is fully charged by the 300 V source), and then quickly disconnect the voltage source from the plates. See Figure 6. The electrometer should still read 300 V.
- Now increase the distance d between the plates to larger values such as 15 mm, 10 mm, and 5 mm, and observe and record the corresponding voltage reading on the electrometer (V); plot V versus d.
- Increase d back to ~ 20 mm, insert a plastic slab between the two plates and observe what happens to V read by the electrometer. The reduction of V between the plates (with charge Q fixed in this case) results from the larger dielectric constant ε of the plastic (compared to air) as the medium of the capacitor (refer to Equations 1 and 3).
3. Parallel and Series Capacitances
- Obtain a capacitance meter (a "LCR meter" or a multi-meter with a capacitance measurement mode); obtain a breadboard to facilitate the electrical connections in this part of the experiment.
- Obtain two commercial "ceramic" capacitors with a capacitance of 1 µF, and use the capacitance meter to verify their capacitance, as in Figure 2.
- Connect the two capacitors in parallel, and use the capacitance meter to measure the total capacitance (between points A and B, see Figure 3).
- Connect the two capacitors in series, and use the capacitance meter to measure the total capacitance (between points A and B, see Figure 4).
Figure 3: Diagram showing two capacitors connected in parallel.
Figure 4: Diagram showing two capacitors connected in series.
Figure 5: Diagram showing the charging up of a capacitor using a voltage source, while reading the voltage with an electrometer.
Figure 6: After quickly disconnecting the voltage source in Figure 5, the voltage and charge on the capacitor should remain.
A capacitor is essential in circuits because it resists changes in voltage by storing equal and opposite charges on its conductive terminals and then supplying energy when the voltage supply drops.
A capacitor is composed of two conductive terminals, such as the two plates in a "parallel plate capacitor", separated by an insulating material or gap. When voltage is applied across a capacitor, it draws current. This causes electrons to accumulate on one plate while they are repelled on the other, thus storing equal and opposite charges on the two plates.
The ability of the component to store charge is called capacitance, and is measured in units called Farads.
This video uses a parallel plate capacitor to illustrate the concept of capacitance and its dependence on physical factors and network configuration.
When a power source is applied to a circuit, the capacitor draws "charging current" until its conductors are fully charged. The amount of charge 'Q' a capacitor can store depends on the capacitance 'C' of the component, and the magnitude of the supplied voltage 'V'.
When the voltage drops, charge from the capacitor's conductors flows to the circuit, generating current until the stored charge is depleted, thus stabilizing voltage fluctuation. Current is the rate of change in the amount of charge. Combining this with the previous equation, we can say that the current flow out of the capacitor is capacitance times the rate of change in voltage.
The value of C is constant for a given capacitor, and can be obtained by using this equation, which shows that C is directly proportional to A -- the plate surface area, d -- the gap distance, and epsilon -- the dielectric constant or "permittivity" of the insulating material between the plates.
Dielectric constant is a measure of the extent to which the material becomes polarized in an electric field.
Thus, given the relationship between epsilon and C, and C and Q; at a given voltage, higher the permittivity, higher will be the capacitor's charge storage capacity.
Vacuum has a dielectric constant of 8.85x10-12 Farads per meter, denoted ε0. Other media generally have greater permittivity values, which are scaled to ε0 and termed the "relative" permittivity of the medium. For example, the relative permittivity of air is approximately one, polymers range from 2 to 4, and distilled water is 80.
Now that physical properties effecting capacitance have been explained, let's take a look at how to measure capacitance in individual or networked capacitive elements.
To start, gather the following materials: a commercial capacitor with capacitance close to 470 micro farad, a programmable voltage source, and an amp-meter or multi-meter that can measure current.
Next, with the voltage source set to 0 V, connect its positive terminal to the amp-meter. Then connect the other port of the amp-meter to the capacitor, using cables with clamps or banana plugs. This enables the measurement of output current from the capacitor. Following that connect the negative port of the voltage source to the other terminal of the capacitor.
Then, switch the voltage source from 0 to 1 V and observe the transient current reading on the amp-meter. Next adjust the voltage back to 0 before increasing to 2 V, 5 V and finally 10 V. For each target voltage allow one second of rest at 0 V between changes to different target voltages. Observe the transient current as the voltage changes.
As predicted by the equation the transient current is expected to be larger for a larger target voltage.
Lastly, program the voltage source to generate a voltage ramp from 0 V to 10V over 5 seconds, and record the "steady state" amp-meter reading mid-ramp. Next, repeat for ramp times of 10 s, 20 s, and 30 s.
Now obtain a parallel plate capacitor with adjustable separation between the plates, and use a 300V battery as the voltage source. Replace the amp-meter with a 1 mega-ohm resistor. This resistor provides an extra protection limiting the current flow in the circuit.
Second, connect a high-impedance voltmeter, or electrometer, between the two plates in order to measure the voltage difference.
Next, connect the battery to the capacitor, and wait until the electrometer also reaches the steady state of 300 V, indicating the capacitor is fully charged. Then quickly disconnect the battery from the plates. The electrometer should still read 300 V.
Repeat the measurement after decreasing the distance between the plates to 15, 10, and 5 mm.
Finally, with a capacitor plate distance of 20 mm, insert a plastic slab between the two plates and observe what happens to the electrometer voltage reading.
For the commercial capacitor, the plot of measured current versus voltage ramp rate reveals a linear relationship between the two parameters.
This complies with the relationship predicated by this equation, which we derived earlier in the video. As per the equation, the slope of the line is equal to the capacitance.
For the parallel plate capacitor with fixed charge, the plot of voltage between the plates versus distance between the plates is linear. This again supports the theoretical relationships. We know that capacitance and plate distance are inversely proportional. We also know that when conductor charge is fixed, capacitance and voltage are also inversely proportional. Combining these two equations reveals that voltage and plate distance are directly proportional to each other when the charge is fixed.
This equation also predicts that with a fixed charge, the larger dielectric constant of the gap medium, the lower would be the voltage between the plates. This was confirmed when the air in the gap was replaced by plastic and we saw a drop in the voltmeter reading.
Capacitors are used in a large variety of engineering and scientific applications to store charge and selectively discharge electricity.
Capacitors are essential for electrical signal processing. For example, biologists used a two-choice test to evaluate how mice recognize and respond to different ultrasonic vocalizations. First, sound files are recorded from live mice and trimmed using high pass filters to select for frequency.
High-pass filter circuits use capacitors to block low frequency oscillations, as the conduction between capacitor plates generally increases at higher frequencies and decreases at low frequencies. Then, variable frequency sounds are simultaneously played in two separate locations, allowing mice to migrate towards the preferred vocalization.
While mains supplies are AC with fluctuating current, many electronic devices, such as computers, require DC power. Capacitors are used within AC power adapters to filter electrical signals and stabilize the DC supply, providing a smooth, uninterrupted source.
You've just watched JoVE's introduction to capacitors. You should now understand the concept of capacitance, how to measure this physical parameter, and how properties like plate-to-plate distance or gap material effect the capacitance value. As always, thanks for watching!
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).
For a parallel plate capacitor with fixed charge Q, a plot of the voltage V between the plates versus the distance d between the plates should also be linear, as depicted in Figure 8. This verifies Equation 4, which is a consequence of the capacitance C of the parallel plate capacitor being inversely proportional to the distance d (Equation 3) and the voltage V being inversely proportional to the capacitance C (because the charge Q is fixed, Equation 1).
For two capacitors, each having 1 μF of capacitance, their parallel connection should give a total capacitance of 2 µF, and their series connection should measure a total capacitance of 0.5 µF, consistent with Equations 5 and 6 on the rules of combining capacitances in parallel or in series.
Figure 7: An exemplary linear plot between current and voltage ramp rate.
Figure 8: An exemplary linear plot between inter-plate voltage and distance.
Applications 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 or in series.
Capacitors are commonly used in many circuit applications. They can be used to store charges and energy. They are essential for electrical signal processing. For example, taking the derivative of an electrical signal, so called the "differentiator", as the capacitor current, is directly proportional to the derivative of a time dependent voltage applied to the capacitor. They are also used in filters (the conduction between the two conductors making up a capacitor generally increases at higher frequency although it is very low at low frequency).
The author of the experiment acknowledges the assistance of Gary Hudson for material preparation and Chuanhsun Li for demonstrating the steps in the video.