Chapter 21 - Capacitance Flashcards

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1
Q

Capacitor

A

A component used to store charge

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2
Q

How does a capacitor work

A
  • Made up of 2 electrically conducting plates separated by an air gap or a dielectric material
  • When connected to a DC power source, negative charge builds on one plate, repelling electrons from the other plate to build a negative charge on the other
  • Therefore a potential difference builds up in the air gap
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3
Q

Capacitance formula

A

C (F) = Q/V

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4
Q

Capacitance definition

A

The amount of charge stored per unit potential difference

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5
Q

Charging a capacitor

A
  1. Initially there is a high current
  2. As the charge builds up on the plate, electrostatic repulsion makes it harder to deposit more electrons
  3. When the p.d. across the capacitor equals the p.d. of the supply, the current falls to 0
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6
Q

Discharging a capacitor

A
  1. If the source of emf is removed, the capacitor will start to discharge
  2. Current will flow in the opposite direction as the repulsive forces are initially high
  3. The current and potential difference will fall to 0 over time
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7
Q

Work done by a capacitor

A

W = 1/2 QV

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8
Q

Parallel circuits

A

The p.d. across each capacitor is the same

The total capacitance is the sum of each individual capacitance

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9
Q

Series circuits

A

The p.d. is shared across the capacitors
The charge of each capacitor is the came
1/C(T) = 1/C1 + 1/C2 + …

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10
Q

Capacitor uses

A

Flash photography, smoothing peaks and troughs in p.d

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11
Q

Using electricity equations for discharge

A

I = V0/R

Q = V0C

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12
Q

Discharging Exponential equations

A

x = x0 e^-t/CR

x can be I, V, Q

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13
Q

τ

A

TIme constant (CR) - the time for it to be 37% from full value- discharge to 37%, charge to 63%

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14
Q

Current equation for a capacitor

A

I = -ΔQ/Δt

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15
Q

ΔQ/Δt

A

-Q/CR

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16
Q

Charging V and Q

A
V = V0(1-e^-t/CR)
Q = Q0(1-e^-t/CR)
17
Q

Charging I

A

I = I0 x e^-t/CR