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)
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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
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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
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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
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5
Q

power (electricity)

P

A
  • the electrical energy transferred per second
  • P = E/t P = VI P = I2R P = V2/R
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6
Q

direct current

DC

A

when current flows in only one direction at all times

e.g. cell, battery

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7
Q

alternating current

AC

A

when current changes direction and instantanious value with time

e.g. mains supply, a.c. lab power supplies

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8
Q

mains voltage

A

230V, 50Hz (A.C.)

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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

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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)
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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
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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
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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
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14
Q

frequency

f

A
  • the number of waves per second
  • f = 1/T f = N/t v=fλ
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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
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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