CAPACITORS 90523. NCEA Level 3 Physics. CAPACITORS. Electric field strength Capacitors Capacitance & Charge Energy in capacitors Capacitors in series and parallel RC Circuits Charging a capacitor Discharging a capacitor Time constant. ELECTRIC FIELD STRENGTH. What is it?.
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NCEA Level 3
What is it?
ANS: Is the force that an electric charge experiences within a specific space (field).
Symbol : E Units: Newtons per Coulomb (NC-1)
E = F/q
Remember from level 2 that electric fields act either inward or outwards dependent on the charge:
Field lines represented with an arrow hence are vectors.
Field lines are stronger when closer together.
If parallel plates are charged then a uniform electric field is then established:
- - - - - - - - - - - - - - - - - - - -
+ + + + + + + + + + + + + + + + + +
The field strength is the same wherever the charge happens to be e.g. A; B or C.
At the edges “D” the field strength is weaker as the field lines are longer, the plates being further apart.
If a charge is moved from the negative plate to the positive then potential energy (EP)is produced or a potential difference set up ‘V’. This is also dependent on the distance ‘d’ between the plates thus two equations can be produced:
EP = qV
E = V/d
What is it?
ANS: It is an electrical component that can store electrical charge and release it some time later.
Symbol : C Units: Farad (F)
Everyday capacitors are measured in either F (10-6); nF (10-9);pF (10-12).
1. Storing energy as in flash photography
2. Time delays in electronic circuits
3. As filters in electronic circuits
4. In tuning circuits
Often made like a swiss roll by rolling metal plates with a insulator (dielectric)in between and wires attached to each plate.
The Parallel Plate Capacitor
TWO OPPOSITELY CHARGED CONDUCTORS SEPARATED BY AN INSULATOR - WHICH MAY BE AIR
The battery causes the flow of electrons to accumulate on one plate and attracts an equal number of electrons fro the other plate, leaving the plates oppositely charged.
E = electric field strength
A capacitor is made of two thin metal sheets separated by a distance of 1.0mm. It is connected to a 12V battery. Calculate the electric field strength between the plates.
E = V/d
= 12 / 1.0 x 10-3
This is the amount of charge a capacitor can store when connected across a potential difference of 1 volt. Obviously the larger the capacitor the more charge it can contain.
The capacitance (C) of a capacitor which stores a charge, ‘Q’ coulombs on each plate when connected across a supply of volts, ‘V’, is given by:
C = Q/V
Capacitors have a finite voltage at which they work at. If the voltage is exceeded then the dielectric will melt and the plates suddenly come into contact. Short circuit, capacitor explodes!!
Gradient = C
Hence C = Q/V
Remember that the capacitance, C, is defined as
“the charge required to raise the potential by one volt”
Page 141 – 142
How much charge is stored on the plates of a 100F capacitor connected to a 12V battery?
Q = C x V
= 100x10-6 x 12
= 1.2x10-3 C
Constant = absolute permittivity of free space (o)
0 = 8.84x10-12 Fm-1
C = (oA)
C = constant x A/d
A student wishes to make a capacitor of 1.0F using parallel plates 1.0mm apart in air.
Find the area of the plates.
C = (O x A) / d
A = (C x d) / O
= (1.0 x 1.0x10-3) / 8.84x10-12
= 1.13x108 m2
= 1.1x108 m2
Different materials insulate at differing amounts thus changing the capacitance, called dielectric effect. The dielectric constant (r) gives the proportion by which ‘C’ increases when dielectric placed between the plates.
Area of Plate overlap = A
Medium relative permittivity = r
d = plate separation
0 = the permittivity of free space = 8.86. X 10-12 F m-1
For air or a vacuum, r = 1
The dielectric constant does not a have a unit as it is the ratio between two capacitance values:
r = Cdielectric
Examples of dielectric constants include:
Page 144 – 145
A parallel plate capacitor with air between its plates has capacitance 1.1nF. A sheet of polystyrene is placed between the plates. Calculate the new capacitance.
Cd = r x Ca
= 2.5 x 1.1nF
Factors affecting the capacitance of a pair of parallel plates.
Page 143 RUTTER.
CHARGING A CAPACITOR:
An RC circuit is one that contains a resistor, ‘R’ and a capacitor, ‘C’.
When a capacitor begins to charge there is a massive flow of charge to the negative plate. This then decreases with time as repulsion from that plate pushes electron away.
When the capacitor is empty there is zero charge stored. As electrons rush in there is a huge build up of energy. This begins to level out as repulsion denies entry of any further charge.
From this two graphs can be drawn for the charging of a capacitor with relation to what happens to current ‘I’ and voltage ‘V’.
Current starts at maximum Imax and then decreases to zero as the negative plate fills up with negative charge. Repulsion pushes against the force of the battery
Voltage starts at zero and rapidly increases until it begins to reach maximum. Now repulsion prevents any further charge entering so the energy remains constant.
When a capacitor discharges the voltage and current graphs are the same. They start at a maximum and follow the inverse curves down towards zero, although it is worth noting that they don’t reach zero.
Explain what is happening in each of these graphs and why they are the same.
EXERCISES: Page 146 – 147 RUTTER
Time constant is the measure of time it takes for a capacitor to reach 63% of the total amount of voltage or current that it can store/release depending on whether it is charging/discharging. The larger , the slower the process.
It is given the term tau, ‘’ and is measured in seconds, ‘s’. The formula for time constant is:
R = resistance (Ω)
C = capacitance (F)
As the voltage never reaches max or zero, then the total time taken can’t be measured hence that is why 63% of the time is used. (Same for current)
EXERCISES: Page 148 – 149 RUTTER
A 100F capacitor connected to a 10V battery is used with a 2.0MΩ resistor to automatically shut off a calculator. The capacitor, initially charged to 10V, discharges through the resistor whenever the buttons are not being pushed. The calculator will turn off when the capacitor voltage falls to 3.7V.
What time will this take?
The capacitor voltage falls by 10 – 3.7 = 6.3V, which is 63% of the initial voltage and so will take one time constant.
= 100x10-6 x 2.0x106
The time constant for a capacitor-resistor series circuit
Page 232-233 S & C.
As charge, Q, is packed onto the plates work needs to be done. Repulsive forces want to push the electrons away from the negative plate towards the positive. The battery supplies the push, energy, to pack these electrons. The push, pd, the battery has the greater the capacitance, C. Thus energy provided by the cell must equal:
E = Q x V
For a capacitor V vs Q is a straight line graph
Area under graph =
½ x Q x V
Area under graph
= energy change
= Q x V
Energy stored in capacitor
Energy provided by cell
As capacitance is the amount of stored charged then the energy inside a capacitor then two formulae can be produced.
EP = ½CV2
EP = ½QV
[Substituting Q = CV into EP]
EP = ½Q2/C
[Substituting V = Q/C into EP = ½QV]
Page 150 – 151
a. The energy stored in the charged capacitor is:
EP = ½CV2
= 0.5 x 1100x10-6 x 9.02
b. The energy provided by the battery is twice the energy stored in the capacitor energy from the battery
= 2 x 0.04455
c. The flow of charge while the capacitor is charging will cause energy to be changed to heat in the resistance of the circuit.
Charge on each capacitor is the same.
V = V1 + V2
For two or more capacitors:
Voltage across each capacitor same as, V, of cell.
Q = Q1 + Q2
For two or more capacitors:
1 = 1 + 1 ………….
Cp = C1 + C2 ……….
Cs C1 C2
EXERCISES: Page 152 – 153 RUTTER
Calculate the equivalent capacitance of the network shown.
For the two capacitors in parallel:
Cp = 4F + 2F
So the network is equivalent to 6F and 12F capacitors connected in series.
1/Cp = 1/C1 + 1/C2
= 1/12 + 1/6
Cp = 12/3 = 4F
This network of capacitors is equivalent to a single capacitor of 4F
EXERCISES FROM RUTTER