Capacitors Flashcards
What do capacitors do? What is its effect?
- Capacitors build up charge on plates
- They are components of electrical circuits that temporarily store electric charge
- They can introduce a time delay into the circuit
- Or storing electrical energy for a short period of time
- They are used extensively in electrical and electronic timing circuits, in power circuits, for smoothing electrical signals and as part of the signal receiving circuits found in radios
How can you increase capacitance ? What is permittivity?
- You can increase capacitance using dielectrics
1. Permittivity is a measure of how difficult it is to generate an electric field in a certain material
2. The relative permittivity is the ratio of the permittivity of a material to the permittivity of free space
3. Relative permittivity is sometimes also called the dielectric constant
How do you work out relative permittivity?
Er = E1 / E0
- where Er is the relative permittivity of material 1, E1 is the permittivity of material 1 in Fm^-1, E0 is the permittivity of free space
What happens when no charge is applied?
- Imagine a dielectric is made up of lots of polar molecules - they have a positive need and a negative end
- When no charge is stored by the capacitor, there is no electric field - so these molecules point in a bunch of random directions
What happens when a charge is applied?
- When a charge is applied to a capacitor, an electric field is generated
- The negative ends of the molecules are attracted to the positively charged plate and vice versus
- This causes all of the molecules to rotate and align themselves with the electric field
- The molecules each have their own electric field, which in this alignment now opposes the applied electric field of the capacitor the larger the permittivity, the large this opposing field is
- This reduced the overall electric field, which reduces the potential difference needed to charge the capacitor, so the capacitance increases
How do you calculate the capacitance of a capacitor using the dimensions of the capacitor and permittivity of the dielectric?
C = AE0Er / d
-Where A is the area of the plates (m^2), E0 is the permittivity of free space (Fm^-1), Er is the relative permittivity of the dielectric and d is the separation of the plates (m)
How do capacitors store energy?
- When charge builds up on the plates of a capacitor, electrical energy is stored by the capacitor,
- You can find the energy stored in the capacitor from the areas under a graph of charge stored against potential difference across the capacitor
- The potential difference across the capacitor is directly proportional to the charge stored on it, so the graph will be a straight line though the origin
- The greater the capacitance, the more energy is stored by the capacitor for a given potential difference
How do you work out energy stored in a capacitor?
E = 1/2 Q.V.
- Where E is the energy stored (J), Q is the charge on the capacitor (C) and V is the potential difference (V)
- The gradient of a Q-V graph effectively gives the capacitance
What are the three expressions for the energy stored by a capacitor?
- E = 1/2 Q.V.
- E = 1/2 CV^2
- E = 1/2 x Q^2 / C
How can you investigate what happens when you charge a capacitor?
- Set up the test circuit shown in the circuit diagram (Diagram)
- Close the switch to connect the uncharged capacitor to the dc power supply
- Let the capacitor charge whilst the data logger records both the potential difference (from the voltmeter) and the current (from the ammeter) over time
- When the current through the ammeter is zero, the capacitor is fully charged
How can you plot graphs of current, potential difference and charge against time?
- Diagrams
- Once a capacitor begins charging
1. As soon as the Switch closed, current starts to flow. The electrons flow onto the plate connected to the negative terminal of the dc power supply, so a negative charge builds up
2. This build-up of negative charge repels electrons off the plate connected to the positive terminal, making the plate positive. These electrons are attracted to the positive terminal of the power supply
3. An equal but opposite charge builds up on each plate, causing a potential difference between the plates. Remember that no charge can flow between the plates because they are sprayed by an insulator (a vacuum, gap or dielectric)
4. As charge builds upon the plates, electrostatic repulsion makes it harder and harder for more electrons to be deposited. When the pd across the capacitor is equal to the of across the power supply, the current falls to zero
How do you discharge a capacitor?
- To discharge a capacitor remove the power supply and close the switch
1. Remove the power supply from the test circuit and close the switch to complete the circuit
2. Let the capacitor discharge whilst the data logger records potential difference and current over time
3. When the current through the ammeter And the potential difference across the plates are zero, the capacitor is fully discharged
Describe the plots of current, pd and charge against time with discharging
- DIAGRAMS
1. The current flows in the opposite direction form the charging current
2. As the potential difference decreases, the current decreases as well
3. When a capacitor is discharging, the amount of charge on and potential difference between the plates falls exponentially with time. That means it always takes the same length of time for the charge or potential difference to halve, no matter what value it starts at - like radioactive decay
4. The same is true for the amount of current flowing around the circuit
What does the time taken to charge or discharge depend on?
- The time it takes to charge or discharge a capacitor depends on:
1. The capacitance of the capacitor (C). This affects the amount of charge that can be transferred at a given potential difference
2. The resistance of the circuit (R). This affects the current in the circuit
How can you calculate the charge, pd and current as a capacitor charges?
- When a capacitor is charging, the growth rate of the amount of charge on and potential difference across the plates shows exponential decay (so over time they increase more and more slowly)
- The charge on the plates at a given time after a capacitor begins charging is given by the equation:
- Q = Q0 (1-e^-t/RC), where Q0 is the charge of the capacitor when it is fully charged (C), t is the time since charging began (s), R is the resistance (ohms) and C is the capacitance (F) - The potential difference between the plates at a given time is given by V=V0 (1-e^t/RC)
- The charging current is different however as it decreases exponentially - the formula to calculate the charging current at a given time is: I=I0e^-t/RC
How do you work out the charge, pd and current as a capacitor discharges?
- Because the amount of charge left on the plates falls exponentially with time as a capacitor discharges, it always takes the same length of time for the charge to halve, no matter how much charge you start with
- The charge left on the plates at a given time after a capacitor begins discharging from being fully charged is given by the equation: Q=Q0e^-t/RC
- As the potential difference and current also decrease exponentially as a capacitor discharges, the formulas for calculating current or potential difference at a certain time are similar: I-I0e^-t/RC and V=V0e^-t/RC
- The formula for discharging current is the same as for the charging current: it just travels in the opposite direction of the charging current
What is the time constant?
tau = RC
- If t=RC is put into the discharging equations above Q=Q0e^-1, V=V0e^-1, I=I0e^-1, so when t=tau, Q/Q0 = 1/e = 1/2.718 = 0.37
1. Tau is the time constant, is the time taken for the charge, potential difference or current of a discharging capacitor to fall to 37% of its value when fully charged
2. It is also the time taken for the charge or potential difference of a charging capacitor to rise to 63% of its value when fully charged
3. So the larger the resistance in series with the capacitor, the longer it takes to charge or discharge
4. In practice, the time taken for a capacitor to charge or fully discharge is taken to be about 5RC
How can you find the time constant from log-linear graphs?
- Instead of using tau=RC, you can create log-linear graphs from data to find the time constant. here charge is sued, but this works for potential difference and current as well
1. Stating from the equation for Q on a discharging capacitor, take the natural log of both sides and rearrange so that Q=Q0e^-tc becomes ln(Q) = (-1/RC)t + ln(Q0)
2. The equation is now in the from of y=mx + c and this means that if you plotted a graph of ln(Q) against time, t, you would get a straight line
3. The gradient of this line would be -1/RC or -1/tau and the y-intercept would be ln(Q0)
4. To get the time constant from the graph, you divide -1 by the gradient of the the line - For this you need to use the log rule: ln(A x B) = ln(A) + ln(B) and ln(e^A) = A