Electricity: Physics 9702 (Cambridge International AS & A Level)

Syllabus 9.1, 9.2, 9.3 · Strand 3 Electricity and Circuits

Questions
10
Total marks
50
Tier mix
10 Core

0 of 10 questions completed

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Syllabus coverage

  • 9.1 4 questions
  • 9.2 2 questions
  • 9.3 8 questions

Electricity (syllabus ref 9.1 to 9.3) builds the quantities that describe circuits from a microscopic starting point: an electric current is a flow of quantised charge carriers, related to charge by Q=ItQ = It, and to the carriers’ motion by I=AnvqI = Anvq, where nn is the number density of charge carriers, vv their drift velocity and qq their charge. Potential difference across a component is defined as the energy transferred per unit charge, V=W/QV = W/Q, and combining current and potential difference gives electrical power, P=VI=I2R=V2/RP = VI = I^2R = V^2/R.

Resistance, R=V/IR = V/I, measures how strongly a component opposes current, and for a uniform conductor of length LL and cross-sectional area AA it can be found from the material’s resistivity, R=ρL/AR = \rho L / A. Different components have distinctive current–voltage characteristics: a metallic conductor at constant temperature gives a straight line through the origin (obeying Ohm’s law), a filament lamp curves as its resistance rises with temperature, and a semiconductor diode conducts in only one direction. Two temperature/light-sensitive resistors are also introduced: a thermistor’s resistance falls as temperature rises, and a light-dependent resistor (LDR)‘s resistance falls as light intensity rises.

Original worked examples below apply these relationships to full step-by-step circuit calculations.

Question 1

Structured AS 5 marks

A phone charger delivers a constant current of 1.50 A1.50\text{ A} to a battery for 40.040.0 minutes.

(a) State the equation relating charge QQ, current II and time tt, and use it to calculate the charge QQ delivered to the battery in this time. [2]

(b) The charge on a single electron is e=1.60×1019 Ce = 1.60\times10^{-19}\text{ C}. Calculate the number nn of electrons that flow through the charger in this time. [2]

(c) State what is meant by an electric current, in terms of the charge carriers in a conductor. [1]

Question 2

Multiple choice AS 1 mark

A student obtains the current–voltage (I–V) characteristic of an unknown electrical component at room temperature. As the potential difference VV across the component is increased steadily from zero, the current II also increases, but not in direct proportion to VV: for equal increases in VV, the increase in II becomes progressively smaller. The current never decreases and the graph never bends back on itself.

Which statement correctly explains this I–V characteristic?

Question 3

Structured AS 9 marks

A battery maintains a constant potential difference of 9.00 V9.00\text{ V} across a resistor of resistance 15.0Ω15.0\,\Omega. The circuit is switched on for 4.004.00 minutes.

(a) State what is meant by potential difference. [1]

(b) Calculate the current II in the resistor. [2]

(c) Calculate the charge QQ that flows through the resistor during the 4.004.00 minutes. [2]

(d) The charge on a single electron is e=1.60×1019 Ce = 1.60\times10^{-19}\text{ C}. Use Q=neQ = ne to calculate the number nn of electrons that flow through the resistor in this time. [2]

(e) Calculate the power PP dissipated in the resistor using P=VIP = VI, and show that this agrees with the value obtained using P=I2RP = I^2R. [2]

Question 4

Structured AS 8 marks

A wire is made from constantan, of resistivity ρ=4.90×107Ωm\rho = 4.90\times10^{-7}\,\Omega\,\text{m}. The wire has length L=2.50 mL = 2.50\text{ m} and a uniform circular cross-section of diameter 0.460 mm0.460\text{ mm}.

(a) Calculate the cross-sectional area AA of the wire, in m2\text{m}^2. [2]

(b) Calculate the resistance RR of the wire, using R=ρL/AR = \rho L / A. [2]

(c) A second wire is made from the same constantan, with the same length, but with double the diameter of the first wire. State and explain, without further detailed calculation, how the resistance of the second wire compares with the resistance found in (b). [2]

(d) The original wire (from part (b)) carries a current of 0.600 A0.600\text{ A}. Calculate the power dissipated in the wire. [2]

Question 5

Multiple choice AS 1 mark

A student measures the current II through a component for four different values of potential difference VV across it:

VV / V 1.001.00 2.002.00 3.003.00 4.004.00
II / A 0.2000.200 0.2800.280 0.3500.350 0.4000.400

Which statement correctly describes how the resistance of the component changes over this range, and what this suggests about the component?

Question 6

Structured AS 9 marks

A copper wire of uniform circular cross-section carries a current of 2.50 A2.50\text{ A}. The wire has diameter 0.60 mm0.60\text{ mm}. Copper has n=8.5×1028n = 8.5\times10^{28} free (conduction) electrons per cubic metre, and the charge on a single electron has magnitude q=1.60×1019 Cq = 1.60\times10^{-19}\text{ C}.

(a) State the equation relating current II, cross-sectional area AA, number density of charge carriers nn, drift velocity vv and charge on each carrier qq, and identify what is meant by "drift velocity". [2]

(b) Calculate the cross-sectional area AA of the wire, in m2\text{m}^2. [2]

(c) Calculate the drift velocity vv of the free electrons in the wire. [2]

(d) The current in the wire is increased to 5.00 A5.00\text{ A}, with AA, nn and qq unchanged. State and calculate the new drift velocity. [2]

(e) The drift velocity found in (c) is extremely small, yet a lamp connected to this wire lights up almost instantly when the circuit is switched on. Explain why. [1]

Question 7

Multiple choice AS 1 mark

A student connects a semiconductor diode into a circuit and measures the current II through it for a range of potential differences VV across it, first with the diode forward-biased and then with the diode reverse-biased, in each case increasing the magnitude of VV from zero.

Which statement correctly describes the resulting I–V characteristic of the diode?

Question 8

Structured AS 7 marks

A thermistor is connected across a supply that maintains a constant potential difference of 6.00 V6.00\text{ V} across it. At a temperature of 20C20\,^{\circ}\text{C}, the thermistor has resistance R1=1200ΩR_1 = 1200\,\Omega. The thermistor is then warmed to a higher temperature, at which its resistance falls to R2=300ΩR_2 = 300\,\Omega.

(a) Calculate the current I1I_1 in the thermistor at 20C20\,^{\circ}\text{C}. [2]

(b) Calculate the current I2I_2 in the thermistor at the higher temperature. [2]

(c) Using the equation I=AnvqI = Anvq, explain, in terms of the charge carriers within the semiconductor material of the thermistor, why its resistance falls as its temperature rises. [3]

Question 9

Multiple choice AS 1 mark

Two wires, X and Y, are made from the same material at the same temperature. Wire X has length LL and cross-sectional area AA. Wire Y has length 2L2L (twice as long) and cross-sectional area A/2A/2 (half as large).

How does the resistance of wire Y compare with the resistance of wire X?

Question 10

Structured AS 8 marks

An engineer is designing a heating element for a laboratory kettle, to be made from nichrome wire of resistivity ρ=1.10×106Ωm\rho = 1.10\times10^{-6}\,\Omega\,\text{m} and uniform cross-sectional area A=4.00×108 m2A = 4.00\times10^{-8}\text{ m}^2. The element must have resistance R=55.0ΩR = 55.0\,\Omega when connected to the 230 V230\text{ V} mains supply.

(a) Calculate the current II that flows in the element when it is connected to the 230 V230\text{ V} supply. [2]

(b) Calculate the length LL of nichrome wire needed to give the required resistance R=55.0ΩR = 55.0\,\Omega, using R=ρL/AR = \rho L / A. [2]

(c) Calculate the power PP dissipated by the heating element when connected to the 230 V230\text{ V} supply, using P=V2/RP = V^2/R. [2]

(d) The wire is now replaced by a nichrome wire of the same length but with half the cross-sectional area. State and explain the effect this has on the resistance and, hence, on the power dissipated at the same 230 V230\text{ V} supply. [2]