Capacitance 9702

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9702 A Level Physics, 19 Capacitance

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25 Terms

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Capacitors

Electrical devices used to store energy.

<p>Electrical devices used to store energy.</p>
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Circuit symbol for parallel plate capacitor

Here

<p>Here</p>
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Capacitors store capacitance, which is defined as

The charge stored per unit potential.
(Or ratio of charge on an object to its potential)

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Greater capacitance =

Greater charge stored on capacitor

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2 forms capacitors come in

isolated spherical conductors, parallel plate capacitors

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Isolated spherical conductors

- stores charge on its surface

- as p.d. of supply increases, the charge of the conductor also increases

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Parallel plates capacitors

- made up of two conducting metal plates connected to a voltage supply

- negative terminal of voltage supply pushes electrons onto one plate, making it negatively charged
- electrons repelled from opposite plate, making it positively charged
- thereā€™s a (dielecteric) insulator between the plates which ensures charge doesnā€™t flow freely between the plates

<p>- made up of two conducting metal plates connected to a voltage supply</p><p>- negative terminal of voltage supply pushes electrons onto one plate, making it negatively charged<br>- electrons repelled from opposite plate, making it positively charged<br>- thereā€™s a (dielecteric) insulator between the plates which ensures charge doesnā€™t flow freely between the plates</p>
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charge stored by capacitor refers to

  • magnitude of charge stored on each plate in a parallel plate capacitor/surface of a spherical conductor

  • capacitor itself doesnā€™t store charge

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capacitance formula

C = Q / V

  • C = capacitance (F)

  • Q = charge (C) ā€¦ on plates

  • V = potential difference (V) ā€¦ across capacitor

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unit of capacitance

  • Farad (F) = 1 Coulomb per Volt, 1 C V-1

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capacitance of a spherical conductor

  • charge per unit potential at surface of the sphere

    • because charge on surface of a spherical conductor can be considered as a point charge at its centre

    • Q= charge stored on surface of spherical conductor (not charge of capacitor)

  • V of an isolated point charge =

    • V = Q/ (4Ļ€Īµ0R)

    • and C=Q/V so V=Q/C

    • so V=Q/C = V = Q/ (4Ļ€Īµ0R)

    • so C= 4Ļ€Īµ0R

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combined capacitance of capacitors in a circuit depends onā€¦

whether theyā€™re connected in series or parallel

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derive formulae for capacitance of capacitors in series

  • consider 2 parallel plates capacitors C1 and C2 connected in series with a p.d. V across them

  • in a series circuit, p.d. is shared between all the components in the circuit

    • therefore, if capacitors store same charge but diff. p.d.s, the p.d. across C1 is V1 and across C2 is V2

    • total p.d. V = sum of V1 and V2

    • V = V1 + V2

    • āˆ“ V1 = Q/C1 and V2 = Q/C2

    • total p.d. => V = Q/Ctotal

    • substitute into V = V1 + V2

      • Q/Ctotal = Q/C1 + Q/C2

  • since current is same throughout all components in a series circuit, charge is same through each capacitor and cancels out

    • āˆ“ eqn. for combined capacitance in a series circuit

      • 1/Ctotal = 1/C1 + 1/C2 + 1/C3 + ā€¦

<ul><li><p>consider 2 parallel plates capacitors C<sub>1 </sub>and C<sub>2</sub> connected in series with a p.d. V across them</p></li><li><p>in a <strong>series</strong> circuit, <span style="color: rgb(255, 255, 255)"><strong>p.d. is shared </strong></span>between all the components in the circuit</p><ul><li><p>therefore, if capacitors store same charge but diff. p.d.s, the p.d. across C<sub>1 </sub>is V<sub>1</sub> and across C<sub>2</sub> is V<sub>2</sub></p></li></ul><ul><li><p>total p.d. V = sum of V<sub>1 </sub>and V<sub>2</sub></p></li><li><p>V = V<sub>1 </sub>+ V<sub>2</sub></p></li><li><p>āˆ“ V<sub>1 </sub>= Q/C<sub>1 </sub>and V<sub>2</sub> = Q/C<sub>2</sub> </p></li><li><p>total p.d. =&gt; V = Q/C<sub>total</sub></p></li><li><p>substitute into V = V<sub>1 </sub>+ V<sub>2 </sub></p><ul><li><p>Q/C<sub>total</sub> = Q/C<sub>1 </sub>+ Q/C<sub>2</sub></p></li></ul></li></ul></li><li><p>since <strong>current is same</strong> throughout all components in a <strong>series </strong>circuit, <strong>charge</strong> is same through each capacitor and cancels out</p><ul><li><p><span>āˆ“ eqn. for <strong>combined capacitance in a series circuit</strong> </span></p><ul><li><p> 1/C<sub>total </sub>= 1/C<sub>1 </sub>+ 1/C<sub>2 </sub>+ 1/C<sub>3</sub> + ā€¦</p></li></ul></li></ul></li></ul><p></p>
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capacitors in parallel

  • since current is split across each junction in a parallel circuit, the charge stored on each capacitor is different

    • therefore charge on capacitor C1 is Q1 and on C2 is Q2

  • total charge Q:

    • Qtotal = Q1 + Q2

  • therefore (by rearranging capacitance eqn.)

    • Q1=C1V and Q2=C2V

  • total charge Q is defined by total capacitance

    • Qtotal = CtotalV

  • substitute in Qtotal = Q1 + Q2

    • CtotalV = C1V + C2V

  • since p.d. is same across all components in a parallel circuit, p.d. V cancels out

    • āˆ“ combined capacitance of capacitors in parallel

    • Ctotal = C1 + C2 + C3 +ā€¦

<ul><li><p>since current is <strong>split </strong>across each junction in a parallel circuit, the <strong>charge</strong> stored on each capacitor is <strong>different </strong></p><ul><li><p>therefore charge on capacitor C<sub>1 </sub>is Q<sub>1</sub> and on C<sub>2</sub> is Q<sub>2</sub></p></li></ul></li><li><p>total charge Q:</p><ul><li><p>Q<sub>total</sub> = Q<sub>1</sub> + Q<sub>2</sub></p></li></ul></li><li><p>therefore (by rearranging capacitance eqn.) </p><ul><li><p>Q<sub>1</sub>=C<sub>1</sub>V and Q<sub>2</sub>=C<sub>2</sub>V</p></li></ul></li><li><p>total charge Q is defined by total capacitance</p><ul><li><p>Q<sub>total</sub> = C<sub>total</sub>V</p></li></ul></li><li><p>substitute in Q<sub>total</sub> = Q<sub>1 </sub>+ Q<sub>2 </sub></p><ul><li><p>C<sub>total</sub>V = C<sub>1</sub>V + C<sub>2</sub>V</p></li></ul></li><li><p>since <strong>p.d. is same<sub> </sub></strong>across all components in a <strong>parallel circuit</strong>, <strong>p.d.</strong> V <strong>cancels out</strong></p><ul><li><p><span>āˆ“</span> combined capacitance of capacitors in parallel </p></li><li><p>C<sub>total</sub> = C<sub>1 </sub>+ C<sub>2</sub> + C<sub>3</sub> +ā€¦</p></li></ul></li></ul><p></p>
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determine the electrical potential energy stored in a capacitor from a potential charge-graph

  • electrical potential energy stored in a capacitor = area under potential-charge graph

<ul><li><p>electrical potential energy stored in a capacitor = <strong>area under </strong>potential-charge graph </p></li></ul><p></p>
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how electrical potential energy is produced on a capacitor

  • when charging a capacitor, power supply transfers electrons on one plate, giving it a negative charge, and transfers electrons away from the other plate, giving it a positive charge

    • āˆ“ it does work on the electrons, which increases their electrical potential energy

  • as charge of negative plate increases, the electric repulsion between electrons increases

    • thus greater amount of work needs to be done to increase the charge on the negative plate

  • also, charge Q on the capacitor is directly proportional to its p.d. V, so the graph is a straight line passing through the origin

<ul><li><p>when charging a capacitor, power supply transfers electrons on one plate, giving it a negative charge, and transfers electrons away from the other plate, giving it a positive charge</p><ul><li><p><span>āˆ“ it does work on the electrons, which increases their <strong>electrical potential energy</strong></span></p></li></ul></li><li><p>as charge of negative plate increases, the electric repulsion between electrons increases</p><ul><li><p>thus greater amount of work needs to be done to increase the charge on the negative plate </p></li></ul></li><li><p>also, charge Q on the capacitor is directly proportional to its p.d. V, so the graph is a <strong>straight line</strong> passing through <strong>the origin</strong></p></li></ul><p></p>
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energy stored in a capacitor formula

  • electrical potential energy is equal to the area under a potential-charge graph

    • this is equal to the work done in charging the capacitor across a particular p.d.

  • āˆ“ the work done/energy stored in a capacitor is defined by

    • W = Ā½ QV

  • substitute charge as C = Q/V āˆ“ Q=VC

    • āˆ“ W = Ā½ CV2

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capacitor discharge graphs

  • capacitors are discharged through a resistor

    • electrons flow from negative plate to positive plate until there are equal numbers on each plate

  • as capacitor discharges, the current, p.d. and charge all decrease exponentially

    • so these graphs w.r.t. to time are all identical and represent exponential decay

<ul><li><p>capacitors are discharged through a resistor</p><ul><li><p>electrons flow from negative plate to positive plate until there are equal numbers on each plate</p></li></ul></li><li><p>as capacitor discharges, the <strong>current, p.d. and charge</strong> all <strong>decrease exponentially</strong></p><ul><li><p>so these graphs w.r.t. to time are all identical and represent <strong>exponential decay </strong></p></li></ul></li></ul><p></p>
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the rate at which a capacitor discharges depends uponā€¦

  • the resistance of the circuit

    • high resistance = current decreases = charge flows from capacitor plates more slowly = more time for capacitor to discharge

    • & vice versa

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time constant, (šœ), of a capacitor discharging through a resistor

  • a measure of how long it takes for the capacitor to discharge

  • defined as: the time taken for the charge, current or voltage of a discharging capacitor to decrease to 37% of its original value

  • unit seconds

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time constant šœ equation

  • šœ = RC

  • šœ = time constant (s)

  • R = resistance of resistor (Ī©)

  • C = capacitance of capacitor (F)

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find time constant from graph

  • find 0.37V0 and the corresponding time for that value = time constant

<ul><li><p>find 0.37V<sub>0</sub> and the corresponding time for that value = time constant</p></li></ul><p></p>
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capacitor discharge equation

  • x = x0e-(t/RC)

  • x = current, charge or p.d.

  • x0 = initial current, charge or p.d. before discharge

  • e = the exponential function

  • t = current time/time elapsed

  • RC = resistance (Ī©) * capacitance (C) = time constant (šœ)

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equation shows that greater time constantā€¦ and greater initial currentā€¦

  • greater time constant = greater the speed at which current/charge/p.d. falls during discharge

  • greater initial current/charge/p.d. = greater rate of discharge (capacitor will take longer to discharge)

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