Capacitance and Dielectrics
- Storing Charge
- Connect two conducting plates to battery (source of potential difference)
- Charge will move
Equilibrium
- DV plates =D Vbattery
- Plate connected to negative terminal
- Plate connected to positive terminal
- Capacitor
- stores charge
- stores energy
- The larger the voltage the more charge can
be stored
- Capacitance
- ratio of stored charge to applied voltage
- C=Q/V
- units
- C/V = Farad = F (in honor of Michael Faraday)
- Capacitance is independent of Q and V, depends on geometry of
the capacitor
- Parallel Plate Capacitor
- Area (A), separation of plates (d)
- Qualitative Estimate for Capacitance
- depends on area
- separation of plates
- closer together - more charge
- permittivity of free space
- Quantitative Value for Capacitance
- The electric field between the plates is uniform and can be
determined as follows
- the electric field due to the positive plate
away from positive plate
- the electric field due to the negative plate
toward negative plate or in
same direction as that due to the positive plate
- the total electric field
- the electric potential
- C = Q/V
- Other Shapes
- Examples
- Circuits
- Battery -

- Capacitor -

- Combining Capacitors
- replace combination by a single equivalent capacitance
- battery will contribute a given amount of charge
- *circuit - every point on wire is at same potential
- Parallel
- each capacitor is connected to the same two points
- potential difference across each capacitor is the same
- Finding the equivalent capacitance

- V1 = V2 = Vb
- Q1 + Q2 = Qt
- Qt = CeqV
- C1 V + C2 V = CeqV
- C1 + C2 = Ceq
- Capacitance increases
- Series
- capacitors are connected end to end
- each capacitor stores same charge (ideal)
- Finding the equivalent capacitance
- Q1 = Q2 = Qt
- V1 + V2 = Vt
- Qt = CeqV
- Q/C1 + Q/C2 = Q/Ceq
- 1/C1 + 1/C2 = 1/Ceq
- Combination
- find series and parallel combinations
- replace with equivalent capacitance
- continue until the circuit has been reduced to one equivalent
capacitance
- Examples
- Storing Energy
- stored energy = to work done to obtain configuration
- start with neutral plate
- no potential difference across plate
- bring in small amount of charge (DQ)
- now potential difference exists across plates
bring in more charge
- DW = DQV
- W = area under line
- W = 1/2QV = 1/2CV2 =
1/2
Q2/2C
- work done to bring in infinitesimally small bit of charge
- total work
- The energy stored is equal to the work done while obtaining the
arrangement,
- an electric field exists between the plates, and we could think about
the energy stored in terms of the electric field.

- (A d) is just the volume between the plates, energy density
- Examples