1008 Electric Capacitance

By the end of this you should understand the following
  1. the basic idea of capacitance
  2. how to calculate it in simple cases.
  3. how capacitors store energy
  4. how capacitors work in circuits

Capacitance

FInal application of static electricity is Capacitors
Parallel Plate system: There is another way of writing the eqn. for the parallel plates:
  • V=  4πkσd
    
  • and
    σ = Charge  = Q 
         Area     A 
  • so
    Q =   A 
    V   4πkd
    


This tells you that if you put a certain amount of charge on parallel plates, there will be a certain fixed voltage. Capacity is measured in farads (which is an enormous unit)

What is the capacity of the earth? (R = 6500 km), assuming it is a conducting sphere.

  1. 720 f
  2. .72 f
  3. 7.2x10-4 f
  4. 7.2 μf

Charge as a fluid.

It's a bit hard to visualize capacitance: it helps to think of charge as a fluid.


Dielectrics

Usually a solid material is put between the plates of a capacitor: this has the effect of reducing the field for a given charge (the dipoles get rotated).

Dielectric constant

K = Eapplied
    Eeff
This
An application of this: the proximity detector. By measuring the capacitance, (via the voltage) can decide if a dielectric object has entered.
Can even do this by regarding object as one plate of capacitor

Energy in capacitors:

We can store energy in capacitors
Work done in adding charge dQ is V dQ, but V = Q/C, so
U = ½CV²

(Same calculation as we did for P.E. stored in stretched spring).


e.g an inventor proposes to build a car where the energy is stored in a parallel plate capacitor with a area of 100m², separation d = 10μ, dielectric constant K = 10.
  1. What is the capacitance?
  2. What is the maximum voltage? (take the breakdown field to be 3x107 V m-1
  3. How much energy can be stored?
  4. Would you invest in it?

Energy Density

e.g. Assume that you are trying to store energy at the same density as in gasoline: what field E would you need? (1 litre [~10-3 m³]~ 4x107 J), ε₀ = 8.85x10-12 C²N-1m-2 or k = 9x109 N m² C-2.
  1. 105 V/m
  2. 107 V/m
  3. 109 V/m
  4. 1011 V/m

So why do you use capacitors to store energy? Energy can be released very rapidly, but non-destructively. e.g. flash for camera has all of energy released in ~ 1 ms.

An example of energy storage in capacitors. This uses a 27 mF capacitor charged to 4 kV: how much energy does this correspond to?


Capacitors in Circuits:

Finally we need to know how to combine capacitors.
We frequently need to combine capacitors with other electrical components: the symbol is obvious!

SImplest possible is just a capacitor and battery (in paractice always have an resistance). Can assume that battery just applies constant voltage.


Combinations of capacitors

Practical circuits often combine different elements, such as resistors, capacitors and inductances (and "active" elements like transistors etc). Hence we need to know how to combine them. e.g.
In parallel: we want to replace 2 capacitors by a single equivalent one: in this case that must have the same voltage across each one, so
Q₁ = V C₁, Q₂ =V C₂, Q = VC but Q₁ + Q₂ = Q 
so that
C = C₁ + C₂

this is almost obvious, if we think of C₁ and C₂ as being part of a larger cap. C.


In series: in this case the central part is isolated and neutral, so charges must be +Q and -Q as shown. Hence
V = V₁ + V₂ = Q = Q  + Q 
              C   C₁   C₂
so that
1 = 1  + 1 
C   C₁   C₂

Useful to remember that this is the opposite of the corresponding relations for resistors.


e.g suppose C₁ = 1 μf,C₂ = 2 μf, C₃ = 12 μf, what is the equivalent capacitance of the circuit?

This sets up electrostatics: we now want to go on and look at current electricity