chapter 21 - capacitance Flashcards

1
Q

capacitor

A

stores charge
- 2 conducting plates
- separated. by an insulator - dielectric

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2
Q

electrolytic capacitor

A
  • dielectric is an electrolyte
  • only works when connected right way round
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3
Q

capacitance

A

charge stored per unit pd
C = Q/V
measured in Farads

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4
Q

parallel plate capacitor

A

C = Aε/d
as A increases more charge can build up on the plate so C increases
as d decreases plates exert a greater force so more electrons move so charge increases C increases

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5
Q

dielectric

A

between plates of a capacitor
- molecules become polarised in an electric field
- align with the field
- attract more electrons onto the plate increasing charge increasing C

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6
Q

permitivity ε

A

is larger with a dielectric

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7
Q

capacitor in series

A

1/Ct = 1/C1 + 1/C2 ….

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8
Q

capacitor in parallel

A

Ct = C1 + C2….

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9
Q

energy stored in a capacitor

A

= 1/2QV
= 1/2CV^2
= 1/2 Q^2/C
less than E = QV as other half of energy lost through heat so not stored

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10
Q

discharging a capacitor

A

initially there is a voltage across the plates
V decreases as Q moves from the plates Q = CV
initially I when charge is moving from plates as Q = It when no pd no moving charge so no I

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11
Q

discharging equations

A

Q = Q0 e^-t/RC
V = V0 e^-t/RC
I = I0 e^-t/RC

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12
Q

time constant

A

RC
time taken for the pd to decrease to 1/e of its initial value

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13
Q

discharging when t = RC

A

Q = Q0/e
V = V0/e
I = I0/e
1/e = 0.37

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14
Q

discharging graphs

A

all downwards curve start fast then slows
can ln and plot
ln against t
eg lnQ = lnQ0 - t/RC
grad = -1/RC

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15
Q

charging a capacitor

A

starts with 0 charge so 0 pd
electrons repelled from neg terminal and attracted from pos
charge builds up on plates increasing pd
but as I = V/R it starts at max I
as pd builds up harder to force charge on the plates so rate of flow of charge is lower until I = 0 and pd = emf

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16
Q

charging equations

A

Q = Q0 (1-e^-t/RC)
V = V0 (1-e^-t/RC)
I = I0 w^-t/RC

17
Q

charging when t = RC

A

Q = (1- 1/e) Q0
V = (1- 1/e) V0
I = 1/e I0

1- 1/e = 0.63

18
Q

charging graphs

A

V and Q upward curves start fast then slow
I same as discharging
V across resistor same as I ( emf - V)

19
Q

capacitor uses

A
  • releasing energy quickly eg flash
  • can store energy
  • can smooth voltage
20
Q

rectifier

A

4 diodes in a diamond
only allows +ve current to flow - makes ac source become dc
but instead of not allowing neg current just makes it become positive

21
Q

capacitor use in a rectifier

A

can be used to smooth current
when V starts to decrease the capacitor is charged so holds some charge and V - keeping it flowing between the humps
making to become almost a constant direct voltage
reduce bumps by increasing RC