Electricity Flashcards
(30 cards)
1
Q
current
I
A
- rate of flow of charge
- I = Q/t
- current (Amperes, A), charge (coulombs, C), time (seconds, s)
- current is measured with an ammeter (in series)
2
Q
potential difference
voltage (V)
A
- the energy change per coulomb of charge
- V = E/Q
- voltage (volts, V), energy (joules, J), charge (coulombs, C)
- measured with a voltmeter
- in a power supply, the energy is given to the charge
- in a component, the energy is used by the charge
3
Q
resistance
R
A
- opposition to the flow of current
- measured with an ohmeter
- depends on the length, thickness, and type of wire; as well as temperature
- R α l, Resistance is proportional to length
4
Q
potential divider
A
- a series circuit with two or more resistors which each receives a share of the supply voltage
- the voltage is split in proportion to resistance, V α R, so: V1/V2 = R1/R2
5
Q
power (electricity)
P
A
- the electrical energy transferred per second
- P = E/t P = VI P = I2R P = V2/R
6
Q
direct current
DC
A
when current flows in only one direction at all times
e.g. cell, battery
7
Q
alternating current
AC
A
when current changes direction and instantanious value with time
e.g. mains supply, a.c. lab power supplies
8
Q
mains voltage
A
230V, 50Hz (A.C.)
9
Q
r.m.s. value
A
- root mean square
- squaring the number turns negative numbers positive, and square rooting them keeps them positive
- the mean is the average value of voltage, current and power of an a.c. supply
- Vrms = Vpeak/√2
allows for comparison between DC and AC
10
Q
peak voltage
Vpeak
A
- the maximum voltage in an a.c. supply
- for an a.c. voltage wave on an oscilloscope screen, it is given by the crest of the wave (when centered)
11
Q
time-base
A
- setting on an oscilloscope which contols the time per cm or division on the horizontal axis
- can be used to find the frequency of an a.c. supply
12
Q
y-gain
A
- setting on an oscilloscope which controls the voltage per cm or division on the verticle axis
- can be used to find the peak voltage of an a.c. supply
13
Q
period
T
A
- the time taken for one wave to pass a point
- on an oscilloscope, it is given by the time-base setting multipied by the number of divisions
14
Q
frequency
f
A
- the number of waves per second
- f = 1/T f = N/t v=fλ
15
Q
electromotive force
e.m.f. (E)
A
- the number of joules/energy available to each coulomb of charge passing through the cell
- E = V + Ir
16
Q
internal resistance
r
A
- the opposition to the flow of charges through a circuits power supply
- the internal resistance obeys ohms law
17
Q
external resistance
R
A
- opposition to the flow of charges externally to the source
- aslo known as the load resistance or the load
18
Q
terminal potential difference
t.p.d.
A
- the potential difference that can be measured at the terminals of a source
- Vt.p.d = E - Ir
19
Q
lost volts
A
- it is the potential difference required for current to pass through the source
- V lost = Ir
20
Q
short circuit
A
- this happens when the load resistance is zero
- in practice the load resistance has to be made as low as possible which can result in very high currents
21
Q
open circuit
A
- this happens when the load resistance is infinite
- this means no current is flowing
- in pratice this is done by a switch or a break/fault in the circuit
22
Q
capacitance
A
- the ability of a device to store electrical charge
- the ratio of charge stored to the p.d. across the two conductors
- C = Q/V
23
Q
work done in a capacitor
A
- a negatively charged plate stores electrons; work is done each time an additional electron is added
- in a graph of Q/V, the area under the graph is = work done, and the gradient of the line = capacitance
- E = 1/2QV E = 1/2CV2 E = 1/2(Q2/C)
24
Q
intristic semiconductor
A
pure semiconductor
25
n-type semiconductor
- contains atoms with 5 valence electrons
- extra electrons are free to move which allows conduction due to free charge carriers
26
p-type semiconductors
- contains some atoms with 3 valence electrons
- these create holes which allow electrons to flow into therefore conduction occurs
27
forward bias
- current flows (n-type to negative, p-type to positive)
- electrons move through diode by moving from the conduction band of the n-type to the conduction band of the p-type
- some electrons drop from the conduction band to the valence band in the depletion layer losing energy
28
reverse bias
- current doesn’t flow (there are exemptions)
- the electrons in the n-type are attracted to the +ve end of the supply, electrons from the -ve supply combine with holes in the p-type
- this enlarges the depletion layer and therefore the p.d. across it so very little current can flow through the energy barrier
| small amounts of current that get through is called leakage current
29
LED
| how does it work
- electrons in the conduction band of the n-type semiconductor move towards the conduction band of the p-type semiconductor
- a free electron is attracted to a hole and falls (from conduction to valence band) losing energy
- this energy is emitted in the form of a light photon (colour determined by the energy lost)
| larger E => larger f => smaller wavelength
30
photodiode
| how does it work
- electrons absorb energy from photons
- electrons move from the valence band to the conduction band
- electrons move towards the n-type semiconductor producing a potential difference