Capacitance Flashcards

(23 cards)

1
Q

Describe the basic structure of a capacitor.

A

2x conducting metal plates separated by an insulated dielectric

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2
Q

How do capacitors store electrical energy?

A
  • Work is done to separate electric charges onto opposing plates
  • This energy is stored as electric potential energy in the field that forms between the plates
  • Hence a p.d.
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3
Q

How do capacitors differ from electrochemical cells?

A
  • They store electrostatic energy rather than chemical energy to be converted to electrical forms
  • They can store and release energy far quicker than chemical cells
  • Less energy overall can be stored
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4
Q

Describe the general trend of capacitor charging.

A
  • Initially current is very large
  • This decays exponentially
  • Until p.d. across the oppositely-charged plates rises to match that of the original power supply
  • Opposing emf and reducing current
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5
Q

Describe the process of discharging a capacitor.

A
  • They discharge though a resistor with no present power supply; no opposition to V(cap)
  • Electrons flow back from the -ve plate to the +ve one until p.d. = 0
  • Current is initially large and in the -ve direction
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6
Q

Describe the flow of electrons when charging a capacitor.

A
  • Electron are repelled from the plate closest to the +ve terminal, leaving this plate with a +ve charge
  • Electrons are deposited onto the -ve plate leaving it with a net -ve charge
  • Until p.d increases to match emf so no current flows
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7
Q

Define capacitance.

A
  • The charge stored per unit potential difference
  • This has the units Farad.
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8
Q

Give the equation used to determine capacitance.

A

Q=CV

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9
Q

How does capacitance in series differ to that in parallel?

A

In series, total capacitance is given by…
1/C1 + 1/C2 … +1/Cx = 1/Ct
… reflecting the reciprocal rule of resistors IN PARALLEL.
In parallel, total capacitance is given by C1 + C2 … Cx = Ct. This reflects the rules of resistors IN SERIES.

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10
Q

Derive total capacitance in parallel.

A

Qt = C1V1 + C2V2…
CtVt = C1V1 + C2V2 …
Ct = C1 + C2 … where V is equal across both parallel branches by K2.

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11
Q

Derive capacitance in series.

A

Vt = V1 + V2…
Qt/Ct = Q1/C1 + Q2/C2 …
Since charge Qt displaced across each capacitor is equal…
1/Ct = 1/C1 + 1/C2 …

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12
Q

Why is work done when we charge a capacitor?

A
  • Separating charges onto an opposing plate forms and intensifies an electric field between the plates
  • Work is done to overcome electric force as we remove further electrons
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13
Q

How do we graphically determine the work done by a capacitor?

A

W=1/2*QV
- This is equal to the area under a V/Q graph
- Remainder is energy dissipated

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14
Q

Derive equations to calculate work done when charging a capacitor.

A

W=1/2CV^2 = 1/2Q^2/C

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15
Q

Describe the shape of the following graphs for charging a capacitor…
- I/t
- V/t

A
  • I/V is an downwards exponential decay
  • V/t is an upwards exponential decay from -ve
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16
Q

Describe the shape of the following graphs for DIScharging a capacitor…
- I/t
- V/t

A
  • I/V is an upwards exponential decay lying within the -ve portion of the I-axis
  • V/t is a downwards exponential decay
17
Q

Explain the trends in current, voltage for charging a capacitor.

A

As we charge…
- initial current is high
- p.d increases until it matches emf
- current decreases exponentially until reaching zero at this point

18
Q

Explain the trends in current, voltage for DIScharging a capacitor.

A

As we discharge…
- initial current is high but -ve
- p.d decreases until it reaches zero
- current decreases exponentially until reaching zero at this point

19
Q

Give the equation describing charge for a DIScharging capacitor. Derive this for current and voltage.

A

Q=Q0 * e^-t/CR

I=-I0 * e^-t/CR
V=V0 * e^-t/CR

20
Q

Give the equation describing charge for a charging capacitor. Derive this for current and voltage.

A

Q=Q0 * (1 - e^-t/CR)

I=I0 * e^-t/CR
V=V0 * (1 - e^-t/CR)

21
Q

What is the time constant for the exponential capacitor equations, and how is it calculated?

A
  • Time constant = C * R
  • This is the time taken for Q on the capacitor to fall to 1/e of its’ original value.
22
Q

How do we use exponential modelling to model discharge of a capacitor?

A
  • For a small time interval…
    delta Q = (delta T / CR) * Q
  • We apply this formula iteratively
22
Q

Why is charging a capacitor an exponential process?

A
  • As the electric field of the capacitor grows, the electric potential between the plates grows
  • This acts to oppose the emf so voltage overall decreases
  • Thus rate of flow of charge and rate of change of emf, charge decreases over time - Since charge carriers flow less readily