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Capacitors consist of two metal plates separated by a layer of insulating material called a dielectric.


1 mF = 1 × 10-6 F
1 nF = 1 × 10-9 F

There are two types of capacitor, electrolytic and non-electrolytic.
Electrolytic capacitors hold much more charge
Electrolytic capacitors have to be connected with the correct polarity, otherwise they can explode.
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Electrolytic |
Non
electrolytic |
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Advantages:
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Advantages:
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Disadvantages:
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Disadvantages:
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In an electrolytic capacitor there has to be a current to maintain the aluminium oxide layer. This is about 1 mA. Over a period of time the charge leaks away. This is called the leakage current. Also it is important that the polarity of the capacitor is correct, otherwise the aluminium oxide layer is not made and the component will conduct. The resulting heating effect can result in the capacitor exploding.
All capacitors have a maximum working voltage. All insulators have a maximum voltage at which they will retain their insulating properties. The breakdown voltage is quoted in units of volts per metre, so it is actually an electric field. The breakdown voltage of air is 3000 V/mm, so a 5 mm gap will insulate up to 15 000 V. The actual voltage at which the breakdown occurs depends on the thickness of the material. The thinner the material, the lower the voltage that is needed before sparking will occur. If sparking occurs over a dielectric, then a hole will be burned in the dielectric and that is the end of the useful life for the capacitor.
As capacitors age, their values can change. This too can lead to poor stability in circuits.

Temperature Coefficient
Capacitors, especially electrolytic, can lose their capacitance, i.e. hold less charge, when they get hot. The decrease in capacitance can change the characteristics of the circuit so much that it will not work properly. Therefore it is essential that the temperature in which the circuit is going to operate at is taken into consideration when designing a circuit and choosing the components.

The results are like this:

From this graph we can see that:
Mica capacitors are very stable with temperature
Ceramic bead capacitors have a linear relationship.
Other types of capacitor have a temperature at which their capacitance is at a maximum. It falls away either side of the optimum.
Data Sheets
Electronic engineers need to know the specifications of the components they are going to use. They refer to data sheets in catalogues, which give them all the information that they need to make a choice. For capacitors, data sheets might include:
Tolerance
Working voltage
Temperature coefficient
Physical size
Price
|
Value
(pF) |
Tolerance
(±
%) |
Working
Voltage (V) |
Temperature
Coefficient (ppm/K) |
Size Thickness
´
diameter (mm) |
Price
(pence) |
|
4.7 |
0.25 |
100 |
0 |
2.5 ´ 5 |
13 |
|
330 |
5 |
100 |
+350 to -1000 |
2.5 ´ 5 |
13 |
|
4700 |
10 |
100 |
± 100 000 |
2.5 ´ 8 |
13 |
|
22 000 |
-20 to +80 |
63 |
± 220 000 |
2.5 ´ 10 |
13 |
Click HERE to find out more about capacitors. You won't need to know this for the AS exam, but you might be interested.
Capacitors
in Series and Parallel
Here is a circuit consisting of two capacitors in parallel. They have values C1 and C2 and are connected to a battery of voltage V.
Like
all parallel circuits the voltage across the capacitors is the same. The
total charge is the sum of the charges on the capacitors. It’s like
the currents in parallel resistors adding up. Click
HERE
for a worked example Series
Capacitors Here
is a circuit consisting of two capacitors in series.
They have values C1
and C2
and are connected to a battery of voltage V.
The
voltages add up to the battery voltage The
current (charge) is the same all the way round. ·
Since Q
= It, it is reasonable to say that the charge that has moved is the same all
the way round. If a number of
electrons of total charge of Q crowds
onto the negative plates of C2
then the same number of electrons are repelled away from the positive plates.
These crowd onto the negative plates of C1
and repel the same number away from the positive plates. Now
we know that V = Q/C and that Vtot = V1 + V2. So we can write:
1
= 1 + 1
Ctot
C1
C2 This
gives us a general relationship for any number of series capacitors:
1
= 1 + 1 + 1 + … +
1
Ctot
C1
C2
C3
Cn We
can tackle problems that involve both series and parallel capacitors in a
similar way to the way we tackle problems with combined series and parallel
arrays of resistors. Click
HERE
for a worked example. When
you tackle problems involving both series and parallel capacitors in the same
circuit, you may find it helpful to adopt the following problem solving
strategy: Work
out the single capacitor equivalent of the parallel capacitors Then
use this answer to work out the single capacitor equivalent of the series
capacitors. Summary Capacitors
in Series and Parallel
Ctot
C1 C2 Back: Home
Electronics AS
Module 2
Topic 8


http://www.s-cool.co.uk/topic_index.asp?subject_id=2
Leakage
Current
Working
Voltage
Temperature Coefficient