# Plate Capacitor: Voltage, Capacitance and Eletric Force

**Level 2**requires school mathematics. Suitable for pupils.

## Table of contents

## Video - Plate Capacitor explained simply in 7 minutes!

Subscribe on YouTube## Basic setup

A plate capacitor usually consists of two round or rectangular conductive plates (also called **Electrodes**). These have an *area* \(A\) and are located at a *distance* \(d\) from each other. Both the area and the distance between the plates are two important parameters that geometrically characterize a plate capacitor.

So far there are only two plates. Only when you put positive and negative electric charges on the two plates, the whole setup becomes a **plate capacitor**. Charge one plate with *positive* charge and the opposite plate with the same amount of *negative* charge. So the total charge on one plate is \(+Q\) and on the other plate \(-Q\) . The amount \(Q\) is the same on both plates.

The positive and negative electric charges on the separated plates now attract each other. If they were free, they would simply move towards each other. But since the plates are spaced at a fixed distance \(d\) from each other, they cannot do that.

From this you probably already recognize the first possible application of a plate capacitor. If you connect the two charged plates with a conducting wire and a small lamp, an electric current flows from one plate to the other and causes the lamp to light up until there is no more difference in charge on the plates. So with a capacitor you can *store electric energy*. But you can do much more with it, for example create a *frequency filter*, which is built into the charging cable of your smartphone and is there to protect the microelectronics from external electromagnetic interference. But that is by far not all.

**Dielectric medium**:

A plate capacitor can be filled with a non-conductive material (called dielectric). For example, the dielectric could be the air, vacuum, water, wood, ceramic, or other non-conductor. This dielectric is characterized by the *relative permittivity* \(\varepsilon_{\text r}\). The dielectric should not be conductive at all, because otherwise the charges would pass through the dielectric to the other plate, thus equalizing the charge difference (this is not the purpose of a capacitor). The dielectric is useful for manipulating the physical properties of the capacitor, such as its capacitance.

Dielectric | Relative Permittivity \(\varepsilon_{\text r}\) |
---|---|

Vacuum | 1 |

Air | 1.0006 |

Water | 80 |

Glas | 6 bis 8 |

## Voltage between the plates

When a small charge \(q\), for example a *free-moving positive charge* (let's call it test charge) is placed next to the *positive* plate, the positive plate will repel the positive test charge and the negative plate will attract it. The test charge experiences an electric force \(F\) inside the plate capacitor, which accelerates the small charge straight toward the *negative* plate. The charge continues to accelerate until it arrives at the opposite negative plate.

Before the test charge hits the negative plate, it has gained *velocity* \(v\) due to acceleration and thus has also gained *kinetic energy* \(W\). This kinetic energy gained by the test charge moving from one charged plate to the other is characterized by the **voltage** \(U\) between the plates. Voltage \(U\) between two plates is the energy \(W\) gained by a small test charge as it moves from one plate to the other, divided by the charge \(q\). Voltage \(U\) is therefore energy per charge.

The voltage \(U\) between the plates and thus also the gained energy \(W\) of the test charge can be manipulated by charging the plates even more. This is done by increasing the charge \(Q\) on both plates. This increases the electric force \(F\) on the test charge. The test charge would then accelerate even more and thus reach a greater velocity \(v\) at the end, so gain a larger kinetic energy \(W\). If you double the electric charge \(Q\), then the voltage \(U\) also doubles. Thus, a test charge \(q\) would then gain twice as much energy \(W\) after traversing the voltage \(U\).

## Electric potential in plate capacitor

Electric potential \(\varphi(x) \) is the the current potential energy of a charge at position \( x \), per charge. You get the potential \(\varphi\) between the electrodes by solving the one-dimensional Laplace equation. The result is a potential \(\varphi\) that depends linearly on the spatial coordinate \(x\):

**Potential between the electrodes**

The potential difference corresponds here to the voltage between the electrodes:

**Formula: Voltage as potential difference**

If you then plot the electric potential \(\varphi\) behind and between the electrodes in a diagram (\(\varphi\), \(x\)), you get a constant potential \(\varphi_1\) in the range \(x \le 0\), that is up to the first electrode. Also behind the second electrode, that is for \(x \ge d\), the potential is constant \(\varphi_2\). Between the electrodes, that is in the region between \(x=0\) and \(x=d\), the potential increases linearly from one electrode to the other.

## Electric field and force inside a plate capacitor

No matter where you place the test charge \(q\) inside the plate capacitor, it will always move straight ahead to the other plate everywhere and experience the same force \(F\). A force field, that is the entirety of all force vectors in space, is *homogeneous* here. Homogeneous means that it does not matter where you place the test charge. The test charge experiences the same electric force everywhere in the plate capacitor.

You can calculate the force on a test charge. The force \(F\) is - without deriving the formula here:

**Electric force on a charge in a plate capacitor**

If you divide the force 3

by the test charge \(q\), then you obtain **electric field** \(E := \frac{F}{q} \):

**Formula: Electric field between capacitor plates**

The typical unit of electric field \( E \) is \( \frac{\mathrm V}{\mathrm m} \) (volts per meter) or alternatively \( \frac{\mathrm N}{\mathrm C}\) (newtons per coulomb).

The electric field is therefore nothing else than force per charge. The electric field in a plate capacitor depends only on the voltage \(U\) and on the plate distance \(d\). The larger the voltage and the smaller the distance, the larger the electric field.

Since the force field is homogeneous, the electric field in the plate capacitor is also homogeneous. Instead of drawing the vector arrows, the electric field is often illustrated with *field lines*. In the case of a plate capacitor, the field lines are straight parallel lines running from one plate to the other. Such straight lines characterize a homogeneous E-field. A test charge then moves on such a straight line.

By definition, the electric field lines run away from the positive plate and towards the negative plate. Consequently, the field lines exit the positively charged plate from both sides. And the field lines enter the negatively charged plate on both sides.

The field lines of the negative and positive plates point in opposite directions behind the plates and thus cancel each other out.

The field lines between the electrodes, on the other hand, point in the same direction, which is why the electric field between the electrodes is amplified.

If you plot the electric field behind and between the electrodes in a coordinate system (\(E\), \(x\)), then the E-field up to the first plate at \(x=0\) is zero. The E-field behind the second plate, which is at \(x=d\), is also zero. Between the electrodes, that is in the region between \(x=0\) and \(x=d\), the E-field has a constant value \(U/d\).

## Capacitance of a plate capacitor

Charge \(Q\) and voltage \(U\) are proportional to each other, where the constant of proportionality \(C\) is the so-called **capacitance**:

**Capacitance definition**

Unit of the capacitance \( C \) is \( \frac{\mathrm{As}}{\mathrm V} \) (Ampere-second per volt) or abbreviated \( \mathrm{F} \) (Farad).

Capacitance is an important characteristic quantity of a capacitor, which depends mainly on its geometry, that is on the **distance** \(d\) between the plates and on the **plate area** \(A\). The capacitance also depends on the material, called dielectric, with which the space between the plates is filled. Here we assume that between the plates there is a vacuum or at least only air. You can calculate the capacitance of a plate capacitor as follows:

**Formula: Plate capacitor capacitance**

Here, \(\varepsilon_0\) is the **electric field constant**, which provides the correct unit of capacitance. This is a natural constant with the value: \(\varepsilon_0 = 8.854 \cdot 10^{-12} \, \frac{\text{As}}{\text{Vm}} \).

If another dielectric is used between the electrodes instead of vacuum (\(\varepsilon_{\text r} = 1 \)), such as ceramic, then the capacitance of the capacitor changed by this can be taken into account by the **relative permittivity** \(\varepsilon_{\text r}\). The capacitance changes by the factor \(\varepsilon_{\text r}\):

**Plate capacitor capacitance with dielectric**

## Electrical energy in the field of the plate capacitor

If you integrate the voltage over the charge, you get the energy \(W_{\text{e}}\), which is necessary to bring the charge \(Q\) to the electrodes:

**Formula: Electrical energy - plate capacitor**

Equation 9

can also be expressed using the volume \(V\) enclosed by the E-field between the electrodes:

**Electrical energy using capacitors volume**

The equation 10

can be interpreted in such a way that the electrical energy of the plate capacitor is not somehow in the electrodes, but *stored in the electric field* between the electrodes (because for the energy only the volume enclosed by the field is relevant).