Capacitors

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Last updated 8:32 PM on 4/11/26
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32 Terms

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Capacitor

  • Consists of 2 metal plates which are seperated by an insulating layer (known as a dielectric)

  • It stores charge by building up a surplus of electrons on one plate and a deficit on the other

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What can a dielectric (insulating layers) be made of?

  • Air

  • Plastic

  • Paper

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How do capacitors store charge?

  • When a capacitor is uncharged it contains equal amounts of electrons on both plates

  • When a capacitor is connected to a battery some of those electrons are moved from one plate to another

  • The electrons will be attracted to the positive terminal of the battery and then repelled by the negative terminal

  • The capacitor is now charged

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Rules of a capacitor

  • Can only be charged by a DC supply

  • The capacitor cannot be charged to a higher voltage then the power supply

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Capacitors vs batteries

  • Stores energy as electrical potential energy (due to electrons being pushed together) - battery = chemical energy

  • Capacitors store very small amounts of charge which can be released very quickly as a high current

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Application of capacitors

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Capacitance

The amount of charged stored per unit potential difference

<p>The amount of charged stored per unit potential difference</p>
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Capacitance graph

  • This assumes that current stays constant which is not true

<ul><li><p>This assumes that current stays constant which is not true</p></li></ul><p></p>
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Why does current not stay constant when charging a capacitor?

  • There aren’t fixed spaces on a capacitor for electrons

  • Instead as you pack the electrons closer together the force of repulsion between them increases

  • Evenutally the force of repulsion is equal to the EMF (electromotive force) for the battery and so the current stops

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How to keep current constant when charging a capacitor

  • Use a variable resistor

  • Set the resistance high to slow the flow of electrons in and gradually reduce

<ul><li><p>Use a variable resistor</p></li><li><p>Set the resistance high to slow the flow of electrons in and gradually reduce</p></li></ul><p></p>
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How is energy stored in a capacitor

  • Capacitor energy is stored as electrical potential energy

  • It’s achieved by forcing electrons closer together on one plate

  • The more electrons that squeeze onto the plate, the smaller the distance between them, so these electrons will try to space out equally

  • This increases the force between them (Coulomb’s law)

  • Which takes energy to push the electrons onto the plate - the moment the power supply is taken away, they will burst back out

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Relationship between energy stored and potential difference (voltage)

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How does the energy stored in a capcitor compare to the energy stored in a battery

  • Batteries produce a steady voltage

  • In a capacitor half the energy gets lost as heat when moving electrons from one plate to the other

<ul><li><p>Batteries produce a steady voltage</p></li><li><p>In a capacitor half the energy gets lost as heat when moving electrons from one plate to the other</p></li></ul><p></p>
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Dielectric

  • The insulating layer between the two metal plates

  • It prevents electrons from jumping from one plate to another

  • Between the two parallel plates, a uniform electric field is generated

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Relationship between permittivity and charge to generate an electric field

  • Greater permittivity requices greater charge

  • Directly proportional

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Permittivity

How hard it is to generate an electric field in a material

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Relative permittivity (Dielectric Constant)

  • The ratio of the permittivity of a material compared to the permittivity of free space (a vacuum)

  • Different dielectrics have different relative permittivity’s

<ul><li><p>The ratio of the permittivity of a material compared to the permittivity of free space (a vacuum)</p></li><li><p>Different dielectrics have different relative permittivity’s</p></li></ul><p></p>
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Breakdown voltage

Refers to how strong the electrical field needs to be to allow electrons to ‘punch’ through the dielectric

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Polar Molecules

  • Permittivity can be explained by the motion of polar molecules inside a dielectric

  • Polar molecules have a positive and negative end

  • As the capacitor charges, one plate becomes positive and the other negative

  • The positive ends will be attracted to the negative plate, and the negative ends to the positive plate

  • Molecules are aligned anti-parallel to the field

  • This means the charges on the field and molecules are the opposite way round

<ul><li><p>Permittivity can be explained by the motion of polar molecules inside a dielectric</p></li><li><p>Polar molecules have a positive and negative end</p></li><li><p>As the capacitor charges, one plate becomes positive and the other negative</p></li><li><p>The positive ends will be attracted to the negative plate, and the negative ends to the positive plate</p></li><li><p>Molecules are aligned anti-parallel to the field</p></li><li><p>This means the charges on the field and molecules are the opposite way round</p></li></ul><p></p>
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How relative permittivity affects capacitance

  • Each polar molecule has its own electric field

  • In this alignment, it opposes the field between the plates

  • Permittivity (larger) is directly proportional to the opposing field (larger) - thereby creating a weaker overall electric field

  • This makes it easier to continue transferring electrons from one plate to the other

  • Therefore reducing the potential difference (Joules per coulomb) needed to transfer a given charge (electrons)

  • So capacitance increases

<ul><li><p>Each polar molecule has its own electric field</p></li><li><p>In this alignment, it opposes the field between the plates</p></li><li><p>Permittivity (larger) is directly proportional to the opposing field (larger) - thereby creating a weaker overall electric field</p></li><li><p>This makes it easier to continue transferring electrons from one plate to the other</p></li><li><p>Therefore reducing the potential difference (Joules per coulomb) needed to transfer a given charge (electrons)</p></li><li><p>So capacitance increases</p></li></ul><p></p>
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Three factors that affect capcitance

  • Area overlap (More area = More space to store electrons, C A)

  • Permittivity of dielectric (Higher permittivity = makes it easier to transfer electrons C ε1 [ε0 x εr])

  • Distance between plates (When distance is small the force between the plates is greater, allowing you hold more electrons in place, C 1/d

<ul><li><p>Area overlap (More area = More space to store electrons, C <span style="font-size: medium;">∝ </span>A)</p></li><li><p>Permittivity of dielectric (Higher permittivity = makes it easier to transfer electrons C <span style="font-size: medium;">∝ </span><span>ε1 [ε0 x εr]</span>)</p></li><li><p>Distance between plates (When distance is small the force between the plates is greater, allowing you hold more electrons in place, C <span style="font-size: medium;">∝ </span>1/d</p></li></ul><p></p>
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Capacitors in parallel

  • When capacitors are placed in parallel you are increasing the area that electrons can be stored on

  • Effectively creating one larger capacitor

  • Which leads to an increase in capcitance, as C A

  • C total = C1 + C2 + …

<ul><li><p>When capacitors are placed in parallel you are increasing the area that electrons can be stored on</p></li><li><p>Effectively creating one larger capacitor </p></li><li><p>Which leads to an increase in capcitance, as C <span style="font-size: medium;">∝ </span>A</p></li><li><p>C total = C1 + C2 + …</p></li></ul><p></p>
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Capacitors in series

  • When capacitors are placed in series you are effectively increasing the distance between the plates

  • Which leads to a decrease in capacitance as C 1/d

  • 1/C total = 1/C1 + 1/C2 + …

<ul><li><p>When capacitors are placed in series you are effectively increasing the distance between the plates</p></li><li><p>Which leads to a decrease in capacitance as C <span style="font-size: medium;">∝ </span>1/d</p></li><li><p>1/C total = 1/C1 + 1/C2 + …</p></li></ul><p></p>
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Capacitor charging graphs

  • Current flowing into an uncharged capacitor starts off high and then falls exponentially

  • The charge will build up quickly on an uncharged capacitor while current is high and then build up slower as current slows

  • The voltage will do the same as charge as tjeu are dorectly proportional. It cannot go above the emf of the battery

<ul><li><p>Current flowing into an uncharged capacitor starts off high and then falls exponentially</p></li><li><p>The charge will build up quickly on an uncharged capacitor while current is high and then build up slower as current slows</p></li><li><p>The voltage will do the same as charge as tjeu are dorectly proportional. It cannot go above the emf of the battery</p></li></ul><p></p>
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How the voltage across the resistor varies in a charging circuit

  • In a charging circuit, the capacitor and resistor will share the voltage produced by the battery

  • But as the voltage across the capacitor increases, the resistor will get a decreasing share

  • Until eventually the capacitor has a voltage to the emf, and the resistor will get none

<ul><li><p>In a charging circuit, the capacitor and resistor will share the voltage produced by the battery</p></li><li><p>But as the voltage across the capacitor increases, the resistor will get a decreasing share</p></li><li><p>Until eventually the capacitor has a voltage to the emf, and the resistor will get none</p></li></ul><p></p>
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Analogy for a discharging capacitor

  • Use of coulomb’s law

  • When a capacitor is charged, the electrons are close together

  • Coulombs tells us that the smaller the distance the greater the force

  • As the capacitor discharges and electrons leave the plate, the distance between them increases, which reduces the force

<ul><li><p>Use of coulomb’s law</p></li><li><p>When a capacitor is charged, the electrons are close together</p></li><li><p>Coulombs tells us that the smaller the distance the greater the force</p></li><li><p>As the capacitor discharges and electrons leave the plate, the distance between them increases, which reduces the force</p></li></ul><p></p>
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Capacitor discharging graphs

  • Initial current from a charged capacitor will start high and then reduce exponentially over time

  • The charge reduce quickly when current it high and then reduce more slowly as the current slows

  • The voltage will do the same as charge as they are directly proportional

<ul><li><p>Initial current from a charged capacitor will start high and then reduce exponentially over time</p></li><li><p>The charge reduce quickly when current it high and then reduce more slowly as the current slows</p></li><li><p>The voltage will do the same as charge as they are directly proportional</p></li></ul><p></p>
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How voltage across the resistor varies in a discharging circuit

  • In a discharging circuit the capacitor is the only power supply

  • The resistor is the only other component

  • So whatever voltage the capacitor is producing gets completely used by the resistor

  • The voltage on both will be the same magnitude

  • The reason why the voltage across the resistor is labelled as a negative is because it is flowing the opposite way to when the circuit was charging

<ul><li><p>In a discharging circuit the capacitor is the only power supply</p></li><li><p>The resistor is the only other component</p></li><li><p>So whatever voltage the capacitor is producing gets completely used by the resistor</p></li><li><p>The voltage on both will be the same magnitude</p></li><li><p>The reason why the voltage across the resistor is labelled as a negative is because it is flowing the opposite way to when the circuit was charging</p></li></ul><p></p>
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Exponential decay equation for capacitors

  • The graph is an exponential decay. This means we can predict the charge left at any point in time

  • It also follows the half-life rule - this means the charge always takes the same amount of time to halve

<ul><li><p>The graph is an exponential decay. This means we can predict the charge left at any point in time</p></li><li><p>It also follows the half-life rule - this means the charge always takes the same amount of time to halve</p></li></ul><p></p>
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Discharging equations

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Charging equations

  • The current graph is exponential decay whilst the others aren’t

<ul><li><p>The current graph is exponential decay whilst the others aren’t</p></li></ul><p></p>
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What happens when a capacitor discharges into another capacitor

Following the circuit diagram:

  • When the switch is at position 1, then capacitor C1 is charged by the battery:

  • This will cause capacitor C1 to become fully charged and have a voltage of the emf

  • This will happen almost instantly as the wires are the only thing providing resistance

  • C2 will not charge as it is part of a broken circuit

  • When connected to position 2 then the fully charged C1 discharges into C2, charging it,

  • C1 is now the only power cupply, it will discharge into C2, and charge it up

  • Eventually C1’s and C2’s voltage will become the same

  • The current will then stop flowing

  • Remember that C1 and C2 are not the same capacitance, so the charge won’t be equal

<p>Following the circuit diagram:</p><ul><li><p><strong>When the switch is at position 1, then capacitor C<sub>1</sub> is charged by the battery:</strong></p></li><li><p>This will cause capacitor C<sub>1</sub> to become fully charged and have a voltage of the emf</p></li><li><p>This will happen almost instantly as the wires are the only thing providing resistance</p></li><li><p>C<sub>2</sub> will not charge as it is part of a broken circuit</p></li><li><p><strong>When connected to position 2 then the fully charged C<sub>1</sub> discharges into C<sub>2</sub>, charging it,</strong></p></li><li><p>C<sub>1</sub> is now the only power cupply, it will discharge into C<sub>2</sub>, and charge it up</p></li><li><p>Eventually C<sub>1</sub>’s and C<sub>2</sub>’s voltage will become the same</p></li><li><p>The current will then stop flowing</p></li><li><p>Remember that C<sub>1</sub> and C<sub>2</sub> are not the same capacitance, so the charge won’t be equal</p></li></ul><p></p>