18.4· 42 questions · 348 marks · 418 min · 2006–2025· Structured questions
Every Cambridge A Level Physics Paper 4 question on electric field of a point charge, laid out as 61 A4 pages with the mark scheme below. Nothing is left out. Free to read, no account.
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59 / 61Answers below. Sit the paper first if you are practising.
Pastlit
Physics 9702 · Electric field of a point charge — Paper 4
A Level · topical answer key — answer key (teacher use)
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9| Question | Answer | Marks | From |
|---|---|---|---|
| 1 | see sheet | 9 | 9702/41 May/June 2006 |
| 2 | see sheet | 11 | 9702/41 May/June 2007 |
| 3 | see sheet | 5 | 9702/41 May/June 2012 |
| 4 | see sheet | 5 | 9702/43 May/June 2012 |
| 5 | see sheet | 6 | 9702/43 May/June 2014 |
| 6 | see sheet | 8 | 9702/41 Oct/Nov 2014 |
| 7 | see sheet | 8 | 9702/42 Oct/Nov 2014 |
| 8 | see sheet | 6 | 9702/41 May/June 2015 |
| 9 | see sheet | 6 | 9702/41 May/June 2016 |
| 10 | see sheet | 6 | 9702/43 May/June 2016 |
| 11 | see sheet | 8 | 9702/42 Oct/Nov 2016 |
| 12 | see sheet | 10 | 9702/43 Oct/Nov 2016 |
| 13 | see sheet | 9 | 9702/42 Feb/March 2017 |
| 14 | see sheet | 7 | 9702/41 May/June 2017 |
| 15 | see sheet | 9 | 9702/42 May/June 2017 |
| 16 | see sheet | 7 | 9702/42 Oct/Nov 2017 |
| 17 | see sheet | 5 | 9702/41 May/June 2018 |
| 18 | see sheet | 5 | 9702/43 May/June 2018 |
| 19 | see sheet | 8 | 9702/42 Feb/March 2019 |
| 20 | see sheet | 8 | 9702/41 May/June 2019 |
| 21 | see sheet | 9 | 9702/42 May/June 2019 |
| 22 | see sheet | 8 | 9702/43 May/June 2019 |
| 23 | see sheet | 10 | 9702/41 Oct/Nov 2019 |
| 24 | see sheet | 10 | 9702/43 Oct/Nov 2019 |
| 25 | see sheet | 8 | 9702/42 Feb/March 2020 |
| 26 | see sheet | 7 | 9702/41 May/June 2020 |
| 27 | see sheet | 10 | 9702/42 May/June 2020 |
| 28 | see sheet | 7 | 9702/43 May/June 2020 |
| 29 | see sheet | 9 | 9702/41 Oct/Nov 2020 |
| 30 | see sheet | 11 | 9702/42 Oct/Nov 2020 |
| 31 | see sheet | 9 | 9702/43 Oct/Nov 2020 |
| 32 | see sheet | 7 | 9702/42 Feb/March 2021 |
| 33 | see sheet | 8 | 9702/41 May/June 2021 |
| 34 | see sheet | 8 | 9702/43 May/June 2021 |
| 35 | see sheet | 10 | 9702/42 Oct/Nov 2022 |
| 36 | see sheet | 10 | 9702/41 Oct/Nov 2024 |
| 37 | see sheet | 10 | 9702/42 Oct/Nov 2024 |
| 38 | see sheet | 10 | 9702/43 Oct/Nov 2024 |
| 39 | see sheet | 11 | 9702/41 May/June 2025 |
| 40 | see sheet | 11 | 9702/43 May/June 2025 |
| 41 | see sheet | 10 | 9702/44 May/June 2025 |
| 42 | see sheet | 9 | 9702/44 Oct/Nov 2025 |
5 An isolated conducting sphere of radius r is placed in air. It is given a charge +Q. This charge may be assumed to act as a point charge situated at the centre of the sphere. (a) (i) Define electric field strength. … … [1] (ii) State a formula for the electric field strength E at the surface of the sphere. Also, state the meaning of any other symbols used. … … … [2] (b) The maximum field strength at the surface of the sphere before electrical breakdown (sparking) occurs is 2.0 ×106 V m–1. The sphere has a radius r of 0.35 m. Calculate the maximum values of (i) the charge that can be stored on the sphere, charge = ………...……………… C [2] (ii) the potential at the surface of the sphere. potential = ………...……………… V [2] Use (c) Suggest the effect of the electric field on a single atom near the sphere’s surface as electrical breakdown of the air occurs. … … … [2]
9 marks
Mark scheme: 5 (a) (i) force per unit positive charge (ratio idea essential) B1 [1] (ii) E = Q / 4πε0r2 M1 ε0 being the permittivity of free space A1 [2] (b) (i) 2.0 × 106 = Q / (4π × 8.85 × 10-12 × 0.352) C1 Q = 2.7 × 10-5 C A1 [2] (ii) V = (2.7 × 10-5) / (4π × 8.85 × 10-12 × 0.35) C1 = 7.0 × 105 V A1 [2] (c) electrons are stripped off the atoms B1 electrons and positive ions move in opposite directions, (giving rise to a current) B1 [2]
3 Two charged points A and B are separated by a distance of 6.0 cm, as shown in Fig. 3.1. 6.0 cm A B d Fig. 3.1 The variation with distance d from A of the electric field strength E along the line AB is shown in Fig. 3.2. 20 E / kV m–1 15 10 5 0 0 2 4 6 d /cm position position of A of B Fig. 3.2 An electron is emitted with negligible speed from A and travels along AB. (a) State the relation between electric field strength E and potential V. … … [2] Examiner’s Use (b) The area below the line of the graph of Fig. 3.2 represents the potential difference between A and B. Use Fig. 3.2 to determine the potential difference between A and B. potential difference = …………………………. V [4] (c) Use your answer to (b) to calculate the speed of the electron as it reaches point B. speed = …………………………. m s–1 [2] (d) (i) Use Fig. 3.2 to determine the value of d at which the electron has maximum acceleration. d = …………………… cm [1] (ii) Without any further calculation, describe the variation with distance d of the acceleration of the electron. … … … [2]
11 marks
Mark scheme: 3 (a) field strength = potential gradient M1 correct sign OR directions discussed A1 [2] (b) area is 21.2 cm2 ± 0.4 cm2 C2 (if outside ± 0.4 cm2 but within ± 0.8 cm2, allow 1 mark) 1.0 cm2 represents (1.0 × 10–2 × 2.5 × 103 =) 25 V C1 potential difference = 530 V A1 [4] (c) ½mv2 = qV ½ × 9.1 × 10–31 × v2 = 1.6 × 10–19 × 530 C1 v = 1.37 × 107 ms–1 A1 [2] (d) (i) d = 0 B1 [1] (ii) acceleration decreases then increases B1 some quantitative analysis (e.g. minimum at 4.0 cm) B1 [2] (any suggestion that acceleration becomes zero or that there is a deceleration scores 0/2) GCE A/AS LEVEL – May/June 2007 9702 04 √ √
5 (a) Define electric field strength. For Examiner’s … Use … [1] (b) An isolated metal sphere is to be used to store charge at high potential. The charge stored may be assumed to be a point charge at the centre of the sphere. The sphere has a radius of 25 cm. Electrical breakdown (a spark) occurs in the air surrounding the sphere when the electric field strength at the surface of the sphere exceeds 1.8 × 104 V cm–1. (i) Show that the maximum charge that can be stored on the sphere is 12.5 μC. [2] (ii) Calculate the potential of the sphere for this maximum charge. potential = … V [2]
5 marks
Mark scheme: 5 (a) force per unit positive charge acting on a stationary charge B1 [1] (b) (i) E = Q / 4πε0r2 C1 Q = 1.8 × 104 × 102 × 4π × 8.85 × 10–12 × (25 × 10–2)2 M1 Q = 1.25 × 10–5 C = 12.5 µC A0 [2] (ii) V = Q / 4πε0r = (1.25 × 10–5) / (4π × 8.85 × 10–12 × 25 × 10–2) C1 = 4.5 × 105 V A1 [2] (Do not allow use of V = Er unless explained) GCE AS/A LEVEL – May/June 2012 9702 41
5 (a) Define electric field strength. For Examiner’s … Use … [1] (b) An isolated metal sphere is to be used to store charge at high potential. The charge stored may be assumed to be a point charge at the centre of the sphere. The sphere has a radius of 25 cm. Electrical breakdown (a spark) occurs in the air surrounding the sphere when the electric field strength at the surface of the sphere exceeds 1.8 × 104 V cm–1. (i) Show that the maximum charge that can be stored on the sphere is 12.5 μC. [2] (ii) Calculate the potential of the sphere for this maximum charge. potential = … V [2]
5 marks
Mark scheme: 5 (a) force per unit positive charge acting on a stationary charge B1 [1] (b) (i) E = Q / 4πε0r2 C1 Q = 1.8 × 104 × 102 × 4π × 8.85 × 10–12 × (25 × 10–2)2 M1 Q = 1.25 × 10–5 C = 12.5 µC A0 [2] (ii) V = Q / 4πε0r = (1.25 × 10–5) / (4π × 8.85 × 10–12 × 25 × 10–2) C1 = 4.5 × 105 V A1 [2] (Do not allow use of V = Er unless explained) GCE AS/A LEVEL – May/June 2012 9702 43
5 An isolated solid metal sphere of radius r is given a positive charge. The distance from the centre of the sphere is x. (a) The electric potential at the surface of the sphere is V0. On the axes of Fig. 5.1, sketch a graph to show the variation with distance x of the electric potential due to the charged sphere, for values of x from x = 0 to x = 4r. 1.00 V0 0.75 V0 potential 0.50 V0 0.25 V0 0 0 r 2r 3r 4r distance x Fig. 5.1 [3] (b) The electric field strength at the surface of the sphere is E0. On the axes of Fig. 5.2, sketch a graph to show the variation with distance x of the electric field strength due to the charged sphere, for values of x from x = 0 to x = 4r. 1.00 E0 0.75 E0 field strength 0.50 E0 0.25 E0 0 0 r 2r 3r 4r distance x Fig. 5.2 [3]
6 marks
Mark scheme: 5 (a) graph: straight line at constant potential = V0 from x = 0 to x = r B1 curve with decreasing gradient M1 passing through (2r, 0.50V0) and (4r, 0.25V0) A1 [3] (b) graph: straight line at E = 0 from x = 0 to x = r B1 curve with decreasing gradient from (r, E0) M1 passing through (2r, ¼E0) A1 [3] (for 3rd mark line must be drawn to x = 4r and must not touch x-axis)
5 (a) Define electric potential at a point. … … … [2] (b) An isolated solid metal sphere is positively charged. The variation of the potential V with distance x from the centre of the sphere is shown in Fig. 5.1. 200 160 V / V 120 80 40 0 0 2 4 6 8 10 x / cm Fig. 5.1 Use Fig. 5.1 to suggest (i) why the radius of the sphere cannot be greater than 1.0 cm, … … [1] (ii) that the charge on the sphere behaves as if it were a point charge. [3] (c) Assuming that the charge on the sphere does behave as a point charge, use data from Fig. 5.1 to determine the charge on the sphere. charge = … C [2]
8 marks
Mark scheme: 5 (a) work done in moving unit positive charge M1 from infinity (to the point) A1 [2] (b) (i) inside the sphere, the potential would be constant B1 [1] (ii) for point charge, Vx is constant B1 co-ordinates clear and determines two values of Vx at least 4 cm apart M1 conclusion made clear A1 [3] (c) q = 4πε0Vx q = 4π × 8.85 × 10–12 × 180 × 1.0 × 10–2 M1 = 2.0 × 10–10 C A1 [2]
5 (a) Define electric potential at a point. … … … [2] (b) An isolated solid metal sphere is positively charged. The variation of the potential V with distance x from the centre of the sphere is shown in Fig. 5.1. 200 160 V / V 120 80 40 0 0 2 4 6 8 10 x / cm Fig. 5.1 Use Fig. 5.1 to suggest (i) why the radius of the sphere cannot be greater than 1.0 cm, … … [1] (ii) that the charge on the sphere behaves as if it were a point charge. [3] (c) Assuming that the charge on the sphere does behave as a point charge, use data from Fig. 5.1 to determine the charge on the sphere. charge = … C [2]
8 marks
Mark scheme: 5 (a) work done in moving unit positive charge M1 from infinity (to the point) A1 [2] (b) (i) inside the sphere, the potential would be constant B1 [1] (ii) for point charge, Vx is constant B1 co-ordinates clear and determines two values of Vx at least 4 cm apart M1 conclusion made clear A1 [3] (c) q = 4πε0Vx q = 4π × 8.85 × 10–12 × 180 × 1.0 × 10–2 M1 = 2.0 × 10–10 C A1 [2]
5 A charged metal sphere is isolated in space. Measurements of the electric potential V are made for different distances x from the centre of the sphere. The variation with distance x of the potential V is shown in Fig. 5.1. 4.0 3.0 V / 103 V 2.0 1.0 0 0 2.0 4.0 6.0 8.0 10.0 x / cm Fig. 5.1 (a) Use Fig. 5.1 to determine the electric field strength, in N C−1, at a point where x = 4.0 cm. Explain your working. electric field strength = … N C−1 [3] (b) The charge on the sphere is 8.0 × 10−9 C. (i) Use Fig. 5.1 to state the electric potential at the surface of the sphere. potential = … V [1] (ii) The sphere acts as a capacitor. Determine the capacitance of the sphere. capacitance = … F [2]
6 marks
Mark scheme: 5 (a) (magnitude of electric field strength is the potential gradient B1 use of gradient at x = 4.0 cm M1 gradient = 4.5 × 104 N C–1 (allow ± 0.3 × 10 4) A1 or Q Q V V = and E = 2 leading to E = (B1) 4πε 0 x 4 πε 0 x x E = 1.8 × 103 / 0.04 (M1) = 4.5 × 104 N C–1 (A1) [3] (b) (i) 3.6 × 103 V A1 [1] (ii) capacitance = Q / V C1 = (8.0 × 10–9) / (3.6 × 103) = 2.2 × 10–12 F A1 [2]
6 A solid metal sphere of radius R is isolated in space. The sphere is positively charged so that the electric potential at its surface is VS. The electric field strength at the surface is ES. (a) On the axes of Fig. 6.1, show the variation of the electric potential with distance x from the centre of the sphere for values of x from x = 0 to x = 3R. 1.0 Vs 0.8 Vs potential 0.6 Vs 0.4 Vs 0.2 Vs 0 0 R 2R 3R distance x Fig. 6.1 [3] (b) On the axes of Fig. 6.2, show the variation of the electric field strength with distance x from the centre of the sphere for values of x from x = 0 to x = 3R. 1.0 Es 0.8 Es field strength 0.6 Es 0.4 Es 0.2 Es 0 0 R 2R 3R distance x Fig. 6.2 [3] [Total: 6]
6 marks
Mark scheme: 6 (a) sketch: from x = 0 to x = R, potential is constant at VS B1 smooth curve through (R, VS) and (2R, 0.5VS) B1 smooth curve continues to (3R, 0.33VS) B1 [3] (b) sketch: from x = 0 to x = R, field strength is zero B1 smooth curve through (R, E) and (2R, 0.25E) B1 smooth curve continues to (3R, 0.11E) B1 [3]
6 A solid metal sphere of radius R is isolated in space. The sphere is positively charged so that the electric potential at its surface is VS. The electric field strength at the surface is ES. (a) On the axes of Fig. 6.1, show the variation of the electric potential with distance x from the centre of the sphere for values of x from x = 0 to x = 3R. 1.0 Vs 0.8 Vs potential 0.6 Vs 0.4 Vs 0.2 Vs 0 0 R 2R 3R distance x Fig. 6.1 [3] (b) On the axes of Fig. 6.2, show the variation of the electric field strength with distance x from the centre of the sphere for values of x from x = 0 to x = 3R. 1.0 Es 0.8 Es field strength 0.6 Es 0.4 Es 0.2 Es 0 0 R 2R 3R distance x Fig. 6.2 [3] [Total: 6]
6 marks
Mark scheme: 6 (a) sketch: from x = 0 to x = R, potential is constant at VS B1 smooth curve through (R, VS) and (2R, 0.5VS) B1 smooth curve continues to (3R, 0.33VS) B1 [3] (b) sketch: from x = 0 to x = R, field strength is zero B1 smooth curve through (R, E) and (2R, 0.25E) B1 smooth curve continues to (3R, 0.11E) B1 [3]
6 Two solid metal spheres A and B, each of radius 1.5 cm, are situated in a vacuum. Their centres are separated by a distance of 20.0 cm, as shown in Fig. 6.1. 1.5 cm 1.5 cm 20.0 cm P sphere A sphere B x Fig. 6.1 (not to scale) Both spheres are positively charged. Point P lies on the line joining the centres of the two spheres, at a distance x from the centre of sphere A. The variation with distance x of the electric field strength E at point P is shown in Fig. 6.2. 50 40 30 E / N C–1 20 10 0 0 2 4 6 8 10 12 14 16 18 20 –10 x / cm –20 –30 –40 –50 Fig. 6.2 (a) Use Fig. 6.2 to determine the ratio magnitude of charge on sphere A . magnitude of charge on sphere B Explain your working. ratio = … [3] (b) The variation with distance x of the electric potential V at point P is shown in Fig. 6.3. 0.8 0.7 0.6 V / V 0.5 0.4 0.3 0.2 0.1 0 0 2 4 6 8 10 12 14 16 18 20 x / cm Fig. 6.3 An α-particle is initially at rest on the surface of sphere A. The α-particle moves along the line joining the centres of the two spheres. Determine, for the α-particle as it moves between the two spheres, (i) its maximum speed, maximum speed = … m s–1 [3] (ii) its speed on reaching the surface of sphere B. speed = … m s–1 [2] [Total: 8]
8 marks
Mark scheme: 6 (a) E = 0 or EA = (–)EB (at x = 11 cm) B1 QA / x2 = QB / (20 – x)2 = 112 / 92 C1 QA / QB or ratio = 1.5 A1 [3] or E ∝ Q because r same or E = Q / 4πε0r2 and r same (B1) QA / QB = 48 / 32 (C1) QA / QB or ratio = 1.5 (A1) (b) (i) for max. speed, ∆V = (0.76 – 0.18) V or ∆V = 0.58 V C1 q∆V = ½mv2 2 × (1.60 × 10–19) × 0.58 = ½ × 4 × 1.66 × 10–27 × v2 C1 v2 = 5.59 × 107 v = 7.5 × 103 m s–1 A1 [3] (ii) ∆V = 0.22 V C1 2 × (1.60 × 10–19) × 0.22 = ½ × 4 × 1.66 × 10–27 × v2 v2 = 2.12 × 107 v = 4.6 × 103 m s–1 A1 [2]
5 Two small solid metal spheres A and B have equal radii and are in a vacuum. Their centres are 15 cm apart. Sphere A has charge +3.0 pC and sphere B has charge +12 pC. The arrangement is illustrated in Fig. 5.1. sphere A sphere B P charge + 3.0 pC charge + 12 pC 5.0 cm 15 cm Fig. 5.1 Point P lies on the line joining the centres of the spheres and is a distance of 5.0 cm from the centre of sphere A. (a) Suggest why the electric field strength in both spheres is zero. … … … [2] (b) Show that the electric field strength is zero at point P. Explain your working. [3] (c) Calculate the electric potential at point P. electric potential = … V [2] (d) A silver-107 nucleus (10747 Ag) has speed v when it is a long distance from point P. Use your answer in (c) to calculate the minimum value of speed v such that the nucleus can reach point P. speed = … m s−1 [3] [Total: 10]
10 marks
Mark scheme: 5 (a) in an electric field, charges (in a conductor) would move B1 no movement of charge so zero field strength or charge moves until F = 0 / E = 0 B1 [2] or charges in metal do not move (B1) no (resultant) force on charges so no (electric) field (B1) (b) at P, EA = (3.0 × 10–12) / [4πε0(5.0 × 10–2)2] (= 10.79 N C–1) M1 at P, EB = (12 × 10–12) / [4πε0(10 × 10–2)2] (= 10.79 N C–1) M1 or (3.0 × 10–12) / [4πε0(5.0 × 10–2)2] – (12 × 10–12) / [4πε0(10 × 10–2)2] = 0 or (3.0 × 10–12) / [4πε0(5.0 × 10–2)2] = (12 × 10–12) / [4πε0(10 × 10–2)2] (M2) fields due to charged spheres are (equal and) opposite in direction, so E = 0 A1 [3] (c) potential = 8.99 × 109 {(3.0 × 10–12) / (5.0 × 10–2) + (12 × 10–12) / (10 × 10–2)} C1 = 1.62 V A1 [2] (d) ½mv2 = qV EK = ½ × 107 × 1.66 × 10–27 × v 2 C1 qV = 47 × 1.60 × 10–19 × 1.62 C1 v 2 = 1.37 × 108 v = 1.2 × 104 m s–1 A1 [3]
6 (a) State one similarity and one difference between the electric field lines and the gravitational field lines around an isolated positively charged metal sphere. similarity … … difference … … [2] (b) A positive point charge +Q is positioned at a fixed point X and an identical positive point charge is positioned at a fixed point Y, as shown in Fig. 6.1. X A B Y +Q +Q 2.5 cm 2.5 cm 10.0 cm Fig. 6.1 The charges are separated in a vacuum by a distance of 10.0 cm. Points A and B are on the line XY. Point A is a distance of 2.5 cm from X and point B is a distance of 2.5 cm from Y. The electric field strength at point A is 4.1 × 10–5 V m–1. (i) Calculate charge +Q. +Q = … C [3] (ii) On Fig. 6.2, sketch the variation of the electric field strength E with distance d from A to B, along the line AB. 5 E / 10–5 V m–1 4 3 2 1 0 0 1 2 3 4 5 d / cm –1 –2 –3 –4 –5 Fig. 6.2 [2] (iii) A small positive charge is placed at A. The electric field causes this charge to move from rest along the line AB. Describe the acceleration of the charge as it moves from A to B. … … … … [2] [Total: 9]
9 marks
Mark scheme: 6(a) similarity: lines are radial / greater separation of lines with increased distance from the sphere B1 difference: gravitational lines directed towards sphere and electric lines directed away from sphere B1 6(b)(i) E = Q / 4πε0r 2 or E = kQ / r 2 with k defined / substituted in C1 4.1 × 10–5 = [Q / (4π × 8.85 ×10–12 × 0.0252)] – [Q / (4π × 8.85 × 10–12 × 0.0752)] C1 Q = 3.2 × 10–18 C A1 6(b)(ii) smooth curve with gradient decreasing starting at (0, 4.1 × 10–5) to d-axis at (2.5, 0) B1 smooth curve with gradient increasing from (2.5, 0) ending at (5, – 4.1 × 10–5) B1 6(b)(iii) acceleration decreases (to zero at mid-point) B1 then acceleration increases in the opposite direction / increasing negative acceleration B1
5 An α-particle is travelling in a vacuum towards the centre of a gold nucleus, as illustrated in Fig. 5.1. gold nucleus α-particle × 10–13 J charge 79e energy 7.7 Fig. 5.1 The gold nucleus has charge 79e. The gold nucleus and the α-particle may be assumed to behave as point charges. At a large distance from the gold nucleus, the α-particle has energy 7.7 × 10–13 J. (a) The α-particle does not collide with the gold nucleus. Show that the radius of the gold nucleus must be less than 4.7 × 10–14 m. [3] (b) Determine the acceleration of the α-particle for a separation of 4.7 × 10–14 m between the centres of the gold nucleus and of the α-particle. acceleration = … m s–2 [3] (c) In an α-particle scattering experiment, the beam of α-particles is incident on a very thin gold foil. Suggest why the gold foil must be very thin. … … [1] [Total: 7]
7 marks
Mark scheme: 5(a) or 7.7 × 10–13 = Qq / 4πε0r C1 7.7 × 10–13 = 8.99 × 109 × 79 × 2 × (1.60 × 10–19)2/ r M1 r = 4.7 × 10–14 m r is closest distance of approach so radius less than this A1 5(b) force = Qq / 4πε0r 2 = 4u × a C1 8.99 × 109 × 79 × 2 × (1.60 × 10–19)2/ (4.7 × 10–14)2 = 4 × 1.66 × 10–27 × a C1 a = 2.5 × 1027 m s–2 A1 5(c) so that single interactions between nucleus and α-particle can be studied or so that multiple deflections with nucleus do not occur B1
6 (a) State Coulomb’s law. … … … [2] (b) Two charged metal spheres A and B are situated in a vacuum, as illustrated in Fig. 6.1. 6.0 cm sphere A sphere B P x Fig. 6.1 The shortest distance between the surfaces of the spheres is 6.0 cm. A movable point P lies along the line joining the centres of the two spheres, a distance x from the surface of sphere A. The variation with distance x of the electric field strength E at point P is shown in Fig. 6.2. 10 E / 103 V m–1 5 0 0 1 2 3 4 5 6 x / cm –5 –10 –15 Fig. 6.2 (i) Use Fig. 6.2 to explain whether the two spheres have charges of the same, or opposite, sign. … … … … [2] (ii) A proton is at point P where x = 5.0 cm. Use data from Fig. 6.2 to determine the acceleration of the proton. acceleration = … m s–2 [3] (c) Use data from Fig. 6.2 to state the value of x at which the rate of change of electric potential is maximum. Give the reason for the value you have chosen. … … … [2] [Total: 9]
9 marks
Mark scheme: 6(a) force proportional to product of charges and inversely proportional to the square of the separation M1 reference to point charges A1 6(b)(i) (near to each sphere,) fields are in opposite directions or point (between spheres) where fields are equal and opposite or point (between spheres) where field strength is zero M1 so same (sign of charge) A1 6(b)(ii) (at x = 5.0 cm,) E = 3.0 × 103 V m–1 and a = qE / m C1 E = (1.60 × 10–19 × 3.0 × 103) / (1.67 × 10–27) C1 = 2.9 × 1011 m s–2 A1 6(c) field strength or E is potential gradient or field strength is rate of change of (electric) potential M1 (field strength) maximum at x = 6 cm A1
6 (a) For any point outside a spherical conductor, the charge on the sphere may be considered to act as a point charge at its centre. By reference to electric field lines, explain this. … … … … [2] (b) An isolated spherical conductor has charge q, as shown in Fig. 6.1. x sphere, charge q P Fig. 6.1 Point P is a movable point that, at any one time, is a distance x from the centre of the sphere. The variation with distance x of the electric potential V at point P due to the charge on the sphere is shown in Fig. 6.2. 14 12 V / 103 V 10 8 6 4 2 0 0 2 4 6 8 10 12 x / cm Fig. 6.2 Use Fig. 6.2 to determine (i) the electric field strength E at point P where x = 6.0 cm, E = … N C–1 [3] (ii) the radius R of the sphere. Explain your answer. R = … cm [2] [Total: 7]
7 marks
Mark scheme: 6(a) electric field lines are radial/normal to surface (of sphere) B1 electric field lines appear to originate from centre (of sphere) B1 6(b)(i) tangent drawn at x = 6.0 cm and gradient calculation attempted C1 E = 9.0 × 104 N C–1 (1 mark if in range ±1.2; 2 marks if in range ±0.6) A2 or correct pair of values of V and x read from curved part of graph and substituted into V = q / 4πε0x (C1) to give q = 3.6 × 10–8 C (C1) (then E = q / 4πε0x2 and x = 6 cm gives) E = 9.0 × 104 N C–1 (A1) or (E = q / 4πε0x2 and V = q / 4πε0x and so) E = V / x (C1) giving E = 5.4 × 103 / 0.060 (C1) = 9.0 × 104 N C–1 (A1) 6(b)(ii) (R =) 2.5 cm B1 potential inside a conductor is constant or field strength inside a conductor zero (so gradient is zero) B1
6 (a) State what is meant by electric field strength. … … [1] (b) An isolated metal sphere A of radius 26 cm is positively charged. Sphere A is shown in Fig. 6.1. charged sphere A 26 cm Fig. 6.1 Electrical breakdown (a spark) occurs when the electric field strength at the surface of the sphere exceeds 2.0 × 104 V m–1. Calculate the maximum charge Q that can be stored on the sphere. Q = … C [2] (c) A second isolated metal sphere B, also with charge +Q, has a radius of 52 cm. Calculate the additional charge, in terms of Q, that may be stored on this sphere before electrical breakdown occurs. additional charge = … [2] [Total: 5]
5 marks
Mark scheme: 6(a) force per unit charge B1 6(b) E = Q / (4πε0r2) C1 2.0 × 104 = Q / (4π × 8.85 × 10–12 × 0.262) charge = 1.5 × 10–7 C A1 6(c) charge (= Q [52 / 26]2) = 4Q C1 additional charge = 3Q A1
6 (a) State what is meant by electric field strength. … … [1] (b) An isolated metal sphere A of radius 26 cm is positively charged. Sphere A is shown in Fig. 6.1. charged sphere A 26 cm Fig. 6.1 Electrical breakdown (a spark) occurs when the electric field strength at the surface of the sphere exceeds 2.0 × 104 V m–1. Calculate the maximum charge Q that can be stored on the sphere. Q = … C [2] (c) A second isolated metal sphere B, also with charge +Q, has a radius of 52 cm. Calculate the additional charge, in terms of Q, that may be stored on this sphere before electrical breakdown occurs. additional charge = … [2] [Total: 5]
5 marks
Mark scheme: 6(a) force per unit charge B1 6(b) E = Q / (4πε0r2) C1 2.0 × 104 = Q / (4π × 8.85 × 10–12 × 0.262) charge = 1.5 × 10–7 C A1 6(c) charge (= Q [52 / 26]2) = 4Q C1 additional charge = 3Q A1
5 (a) State what is meant by an electric field. … … [1] (b) An isolated solid metal sphere has radius R. The charge on the sphere is +Q and the electric field strength at its surface is E. On Fig. 5.1, draw a line to show the variation of the electric field strength with distance x from the centre of the solid sphere for values of x from x = 0 to x = 3R. 1.00E 0.75E electric field strength 0.50E 0.25E 0 0 R 2R 3R distance x Fig. 5.1 [4] (c) The sphere in (b) has radius R = 0.26 m. Electrical breakdown (a spark) occurs when the electric field strength at the surface of the sphere exceeds 2.0 × 106 V m–1. Determine the maximum charge that can be stored on the sphere before electrical breakdown occurs. charge = … C [3]
8 marks
Mark scheme: 5(a) region where charge experiences an (electric) force B1 5(b) graph: field strength zero from x = 0 to x = R B1 curve with negative gradient, decreasing from x = R to x = 3R B1 line passes through field strength E at x = R, B1 line passes through field strength 0.25E at x = 2R and field strength 0.11E at x = 3R B1 Question Answer Marks 5(c) field strength = q / 4πϵ0x2 C1 2.0 × 106 = q / (4 × π × 8.85 × 10–12 × 0.262) C1 q = 1.5 × 10–5 C A1
5 (a) State what is meant by electric field strength. … … … [2] (b) Two point charges A and B are situated a distance 15 cm apart in a vacuum, as illustrated in Fig. 5.1. A P B x 15 cm Fig. 5.1 Point P lies on the line joining the charges and is a distance x from charge A. The variation with distance x of the electric field strength E at point P is shown in Fig. 5.2. 10 8 E / 103 N C–1 6 4 2 0 0 2 4 6 8 10 12 14 x / cm –2 –4 –6 Fig. 5.2 (i) By reference to the direction of the electric field, state and explain whether the charges A and B have the same, or opposite, signs. … … … [2] (ii) State why, although charge A is a point charge, the electric field strength between x = 3 cm and x = 7 cm does not obey an inverse-square law. … … [1] (iii) Use Fig. 5.2 to determine the ratio magnitude of charge A . magnitude of charge B ratio = … [3] [Total: 8]
8 marks
Mark scheme: 5(a) force per unit charge B1 (force on) positive charge B1 5(b)(i) field changes direction (between A and B)/field is zero at a point (between A and B) M1 so charges have same sign A1 5(b)(ii) Any one from: • field is (also) influenced by charge B • charge A is not isolated/is not the only charge present • field is due to two/both charges • field is the resultant of two fields B1 5(b)(iii) E = Q / (4πε0x2) C1 at x = 10 cm, EA = EB C1 QA / 102 = QB / 52 QA / QB = 4.0 A1
6 (a) State what is meant by electric potential at a point. … … … [2] (b) Two parallel metal plates A and B are held a distance d apart in a vacuum, as illustrated in Fig. 6.1. plate B +V0 x P d 0 V plate A Fig. 6.1 Plate A is earthed and plate B is at a potential of +V0. Point P is situated in the centre region between the plates at a distance x from plate B. The potential at point P is V. On Fig. 6.2, show the variation with x of the potential V for values of x from x = 0 to x = d. +V0 potential V 00 d distance x Fig. 6.2 [3] (c) Two isolated solid metal spheres M and N, each of radius R, are situated in a vacuum. Their centres are a distance D apart, as illustrated in Fig. 6.3. D sphere M sphere N charge +Q charge +Q P R R y Fig. 6.3 Each sphere has charge +Q. Point P lies on the line joining the centres of the two spheres, and is a distance y from the centre of sphere M. On Fig. 6.4, show the variation with distance y of the electric potential at point P, for values of y from y = 0 to y = D. + potential 0 0 R (D – R) D y – Fig. 6.4 [4] [Total: 9]
9 marks
Mark scheme: 6(a) work done per unit charge B1 (work done) moving positive charge from infinity B1 6(b) straight line with non-zero gradient from x = 0 to x = d B1 line with gradient of constant sign and end-points between which ∆V = V0 and ∆x = d B1 line passes through (d, 0) and (0, +V0) with negative gradient throughout B1 6(c) V constant (and non-zero) from 0 → R and from (D – R) → D B1 equal (non-zero) values of (magnitude of) V at R and (D – R). B1 curve (with a minimum) from R to (D – R) with V always positive B1 minimum at mid-point of curve B1
5 (a) State what is meant by electric field strength. … … … [2] (b) Two point charges A and B are situated a distance 15 cm apart in a vacuum, as illustrated in Fig. 5.1. A P B x 15 cm Fig. 5.1 Point P lies on the line joining the charges and is a distance x from charge A. The variation with distance x of the electric field strength E at point P is shown in Fig. 5.2. 10 8 E / 103 N C–1 6 4 2 0 0 2 4 6 8 10 12 14 x / cm –2 –4 –6 Fig. 5.2 (i) By reference to the direction of the electric field, state and explain whether the charges A and B have the same, or opposite, signs. … … … [2] (ii) State why, although charge A is a point charge, the electric field strength between x = 3 cm and x = 7 cm does not obey an inverse-square law. … … [1] (iii) Use Fig. 5.2 to determine the ratio magnitude of charge A . magnitude of charge B ratio = … [3] [Total: 8]
8 marks
Mark scheme: 5(a) force per unit charge B1 (force on) positive charge B1 5(b)(i) field changes direction (between A and B)/field is zero at a point (between A and B) M1 so charges have same sign A1 5(b)(ii) Any one from: • field is (also) influenced by charge B • charge A is not isolated/is not the only charge present • field is due to two/both charges • field is the resultant of two fields B1 5(b)(iii) E = Q / (4πε0x2) C1 at x = 10 cm, EA = EB C1 QA / 102 = QB / 52 QA / QB = 4.0 A1
6 (a) State an expression for the electric field strength E at a distance r from a point charge Q in a vacuum. State the name of any other symbol used. … … … [2] (b) Two point charges A and B are situated a distance 10.0 cm apart in a vacuum, as illustrated in Fig. 6.1. charge A charge B P x 10.0 cm Fig. 6.1 A point P lies on the line joining the charges A and B. Point P is a distance x from A. The variation with distance x of the electric field strength E at point P is shown in Fig. 6.2. 2.5 E / 10–2 N C–1 2.0 1.5 1.0 0 2 4 6 8 10 x / cm Fig. 6.2 State and explain whether the charges A and B: (i) have the same, or opposite, signs … … … [2] (ii) have the same, or different, magnitudes. … … … [2] (c) An electron is situated at point P. Without calculation, state and explain the variation in the magnitude of the acceleration of the electron as it moves from the position where x = 3 cm to the position where x = 7 cm. … … … … … … [4] [Total: 10]
10 marks
Mark scheme: 6(a) M1 where ε0 is permittivity (of free space) A1 6(b)(i) field does not change direction/field does not become zero M1 so (charges have) opposite (sign) A1 6(b)(ii) minimum is at the midpoint (between the charges) M1 so (magnitudes are the) same A1 6(c) force = field strength × charge and force = mass × acceleration or acceleration is proportional to field strength B1 (from x = 3.0 cm) to x = 5.0 cm: acceleration decreases B1 at x = 5.0 cm: acceleration is a minimum B1 from x = 5.0 cm (to x = 7.0 cm): acceleration increases B1
6 (a) State an expression for the electric field strength E at a distance r from a point charge Q in a vacuum. State the name of any other symbol used. … … … [2] (b) Two point charges A and B are situated a distance 10.0 cm apart in a vacuum, as illustrated in Fig. 6.1. charge A charge B P x 10.0 cm Fig. 6.1 A point P lies on the line joining the charges A and B. Point P is a distance x from A. The variation with distance x of the electric field strength E at point P is shown in Fig. 6.2. 2.5 E / 10–2 N C–1 2.0 1.5 1.0 0 2 4 6 8 10 x / cm Fig. 6.2 State and explain whether the charges A and B: (i) have the same, or opposite, signs … … … [2] (ii) have the same, or different, magnitudes. … … … [2] (c) An electron is situated at point P. Without calculation, state and explain the variation in the magnitude of the acceleration of the electron as it moves from the position where x = 3 cm to the position where x = 7 cm. … … … … … … [4] [Total: 10]
10 marks
Mark scheme: 6(a) M1 where ε0 is permittivity (of free space) A1 6(b)(i) field does not change direction/field does not become zero M1 so (charges have) opposite (sign) A1 6(b)(ii) minimum is at the midpoint (between the charges) M1 so (magnitudes are the) same A1 6(c) force = field strength × charge and force = mass × acceleration or acceleration is proportional to field strength B1 (from x = 3.0 cm) to x = 5.0 cm: acceleration decreases B1 at x = 5.0 cm: acceleration is a minimum B1 from x = 5.0 cm (to x = 7.0 cm): acceleration increases B1
6 Two positively charged identical metal spheres A and B have their centres separated by a distance of 24 cm, as shown in Fig. 6.1. 24 cm x sphere A sphere B Fig. 6.1 (not to scale) The variation with distance x from the centre of A of the electric field strength E due to the two spheres, along the line joining their centres, is represented in Fig. 6.2. 9 8 E / 104 N C–1 7 6 5 4 3 2 1 0 0 2 4 6 8 10 12 14 16 18 20 22 24 – 1 x / cm – 2 Fig. 6.2 (a) State the radius of the two spheres. radius = … cm [1] (b) The charge on sphere A is 3.6 × 10−9 C. Determine the charge QB on sphere B. Assume that spheres A and B can be treated as point charges at their centres. Explain your working. QB = … C [3] (c) (i) Sphere B is removed. Use information from (b) to determine the electric potential on the surface of sphere A. electric potential = … V [2] (ii) Calculate the capacitance of sphere A. capacitance = … F [2] [Total: 8]
8 marks
Mark scheme: 6(a) 2.0 cm B1 6(b) At 16 (cm) from A the electric fields are equal or EA = EB B1 E = Q / 4πεor2 QA / (4πεorA2) = QB / (4πεorB2) 3.6 × 10-9 / 0.162 = QB / 0.082 C1 QB = 9.0 × 10–10 C A1 6(c)(i) V = Q / 4πεorA V = 3.6 × 10–9 / (4 × π × 8.85 × 10–12 × 0.020) C1 V = 1600 V A1 6(c)(ii) C = Q / V = 3.6 × 10–9 / 1600 C1 = 2.3 × 10–12 F A1
5 (a) State one similarity and one difference between the fields of force produced by an isolated point charge and by an isolated point mass. similarity: … … difference: … … [2] (b) An isolated solid metal sphere A of radius R has charge +Q, as illustrated in Fig. 5.1. R P 2R sphere A charge +Q Fig. 5.1 A point P is distance 2R from the surface of the sphere. Determine an expression that includes the terms R and Q for the electric field strength E at point P. E = … [2] (c) A second identical solid metal sphere B is now placed near sphere A. The centres of the spheres are separated by a distance 6R, as shown in Fig. 5.2. R R P sphere A sphere B charge +Q charge –Q 6R Fig. 5.2 Point P lies midway between spheres A and B. Sphere B has charge –Q. Explain why: (i) the magnitude of the electric field strength at P is given by the sum of the magnitudes of the field strengths due to each sphere … … [1] (ii) the electric field strength at point P due to the charged metal spheres is not, in practice, equal to 2E, where E is the electric field strength determined in (b). … … … [2] [Total: 7]
7 marks
Mark scheme: 5(a) similarity: both are radial or both have inverse square (variations) B1 difference: direction is always/only towards the mass or direction can be towards or away from charge B1 5(b) field strength = Q / 4πε0x2 C1 E = Q / 36πε0R 2 A1 5(c)(i) fields (due to each sphere) are in same direction B1 5(c)(ii) charges on spheres attract/affect each other or charge distribution on each sphere distorted by the other sphere or charges on the surface of the spheres move B1 spheres are not point charges (at their centres) B1
7 A metal sphere of radius R is isolated in space. Point P is a distance x from the centre of the sphere, as illustrated in Fig. 7.1. R P x Fig. 7.1 The variation with distance x of the electric field strength E due to the charge on the sphere is shown in Fig. 7.2. 20 15 E / 105 V m–1 10 5 0 0 2 4 6 8 10 12 x / cm Fig. 7.2 (a) State what is meant by electric field strength. … … … [2] (b) (i) Use Fig. 7.2 to determine the radius R of the sphere. Explain your working. R = … cm [2] (ii) Use Fig. 7.2 to determine the charge Q on the sphere. Q = … C [3] (c) An α‑particle is situated a distance 8.0 cm from the centre of the sphere. Calculate the acceleration of the α‑particle. acceleration = … m s–2 [3] [Total: 10]
10 marks
Mark scheme: 7(a) force per unit charge M1 (force on) positive charge A1 7(b)(i) no electric field inside a conductor B1 R = 4.5 cm A1 7(b)(ii) E = Q / (4πε0x2) C1 clear correct read-off of a pair of values of E and x C1 e.g. Q = 18 × 105 × 4π × 8.85 × 10–12 × (4.5 × 10–2)2 = 4.0 × 10–7 C or 4.1 × 10–7 C A1 7(c) At 8.0 cm, E = 5.75 × 105 V m–1 C1 F = Eq and a = F / m C1 F = (5.75 × 105 × 2 × 1.6 × 10–19) / (4 × 1.66 × 10–27) = 2.8 × 1013 m s–2 A1
5 (a) State one similarity and one difference between the fields of force produced by an isolated point charge and by an isolated point mass. similarity: … … difference: … … [2] (b) An isolated solid metal sphere A of radius R has charge +Q, as illustrated in Fig. 5.1. R P 2R sphere A charge +Q Fig. 5.1 A point P is distance 2R from the surface of the sphere. Determine an expression that includes the terms R and Q for the electric field strength E at point P. E = … [2] (c) A second identical solid metal sphere B is now placed near sphere A. The centres of the spheres are separated by a distance 6R, as shown in Fig. 5.2. R R P sphere A sphere B charge +Q charge –Q 6R Fig. 5.2 Point P lies midway between spheres A and B. Sphere B has charge –Q. Explain why: (i) the magnitude of the electric field strength at P is given by the sum of the magnitudes of the field strengths due to each sphere … … [1] (ii) the electric field strength at point P due to the charged metal spheres is not, in practice, equal to 2E, where E is the electric field strength determined in (b). … … … [2] [Total: 7]
7 marks
Mark scheme: 5(a) similarity: both are radial or both have inverse square (variations) B1 difference: direction is always/only towards the mass or direction can be towards or away from charge B1 5(b) field strength = Q / 4πε0x2 C1 E = Q / 36πε0R 2 A1 5(c)(i) fields (due to each sphere) are in same direction B1 5(c)(ii) charges on spheres attract/affect each other or charge distribution on each sphere distorted by the other sphere or charges on the surface of the spheres move B1 spheres are not point charges (at their centres) B1
5 (a) Define electric potential at a point. … … … [2] (b) Two point charges A and B are separated by a distance of 12.0 cm in a vacuum, as illustrated in Fig. 5.1. x charge A P charge B 12.0 cm Fig. 5.1 The charge of A is +2.0 × 10–9 C. A point P lies on the line joining charges A and B. Its distance from charge A is x. The variation with distance x of the electric potential V at point P is shown in Fig. 5.2. 20 V / 102 V 10 0 0 2 4 6 8 10 12 x / cm –10 –20 –30 –40 Fig. 5.2 Use Fig. 5.2 to determine: (i) the charge of B charge = … C [3] (ii) the change in electric potential when point P moves from the position where x = 9.0 cm to the position where x = 3.0 cm. change = … V [1] (c) An α-particle moves along the line joining point charges A and B in Fig. 5.1. The α-particle moves from the position where x = 9.0 cm and just reaches the position where x = 3.0 cm. Use your answer in (b)(ii) to calculate the speed v of the α-particle at the position where x = 9.0 cm. v = … m s–1 [3] [Total: 9]
9 marks
Mark scheme: 5(a) work done per unit charge B1 (work done on charge) moving positive charge from infinity B1 5(b)(i) (2.0 × 10–9) / 4πε0(4.0 × 10–2) + Q / 4πε0(8.0 × 10–2) = 0 C1 Q = 4.0 × 10–9 C A1 Q given with negative sign B1 5(b)(ii) change = 1200 V A1 5(c) ½mv2 = qV C1 ½ × 4 × 1.66 × 10–27 × v2 = 2 × 1.60 × 10–19 × 1200 C1 v = 3.4 × 105 m s–1 A1
5 (a) (i) State what is meant by a field of force. … … … [2] (ii) State one similarity and one difference between the electric field due to a point charge and the gravitational field due to a point mass. similarity: … … … difference: … … … [2] (b) An isolated solid metal sphere of radius 0.15 m is situated in a vacuum, as illustrated in Fig. 5.1. 0.15 m P x Fig. 5.1 The electric field strength at the surface of the sphere is 84 V m–1. Determine: (i) the charge Q on the sphere Q = … C [2] (ii) the electric field strength at point P, a distance x = 0.45 m from the centre of the sphere. electric field strength = … V m–1 [2] (c) Use information from (b) to show, on the axes of Fig. 5.2, the variation of the electric field strength E with distance x from the centre of the sphere for values of x from x = 0 to x = 0.45 m. 100 80 E / V m–1 60 40 20 0 0 0.1 0.2 0.3 0.4 0.5 x / m Fig. 5.2 [3] [Total: 11]
11 marks
Mark scheme: 5(a)(i) region (of space) B1 where a particle experiences a force B1 5(a)(ii) similarity – any one point from: • both have an inverse square variation • both decrease with distance • both are radial B1 difference – any one point from: • gravitational field always towards (the mass) • electric field can be towards or away from (the charge) B1 5(b)(i) E = Q / 4πε0x2 C1 Q = 4π × 8.85 × 10–12 × 84 × 0.152 = 2.1 × 10–10 C A1 5(b)(ii) E = 84 × (0.15 / 0.45)2 or E = (2.1 × 10–10) / (4π × 8.85 × 10–12 × 0.452) C1 E = 9.3 V m–1 A1 5(c) line at E = 0 from x = 0 to x = 0.15 m B1 smooth curve with decreasing negative gradient throughout, from x = 0.15 m to x = 0.45 m, passing through (0.15, 84) B1 line passing through (0.45, 9.3) B1
5 (a) Define electric potential at a point. … … … [2] (b) Two point charges A and B are separated by a distance of 12.0 cm in a vacuum, as illustrated in Fig. 5.1. x charge A P charge B 12.0 cm Fig. 5.1 The charge of A is +2.0 × 10–9 C. A point P lies on the line joining charges A and B. Its distance from charge A is x. The variation with distance x of the electric potential V at point P is shown in Fig. 5.2. 20 V / 102 V 10 0 0 2 4 6 8 10 12 x / cm –10 –20 –30 –40 Fig. 5.2 Use Fig. 5.2 to determine: (i) the charge of B charge = … C [3] (ii) the change in electric potential when point P moves from the position where x = 9.0 cm to the position where x = 3.0 cm. change = … V [1] (c) An α-particle moves along the line joining point charges A and B in Fig. 5.1. The α-particle moves from the position where x = 9.0 cm and just reaches the position where x = 3.0 cm. Use your answer in (b)(ii) to calculate the speed v of the α-particle at the position where x = 9.0 cm. v = … m s–1 [3] [Total: 9]
9 marks
Mark scheme: 5(a) work done per unit charge B1 (work done on charge) moving positive charge from infinity B1 5(b)(i) (2.0 × 10–9) / 4πε0(4.0 × 10–2) + Q / 4πε0(8.0 × 10–2) = 0 C1 Q = 4.0 × 10–9 C A1 Q given with negative sign B1 5(b)(ii) change = 1200 V A1 5(c) ½mv2 = qV C1 ½ × 4 × 1.66 × 10–27 × v2 = 2 × 1.60 × 10–19 × 1200 C1 v = 3.4 × 105 m s–1 A1
6 (a) State a similarity between the gravitational field lines around a point mass and the electric field lines around a point charge. … … [1] (b) The variation with radius r of the electric field strength E due to an isolated charged sphere in a vacuum is shown in Fig. 6.1. 1.3 1.2 1.1 E / 105 V m–1 1.0 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 0 1 2 3 4 5 6 r / cm Fig. 6.1 Use data from Fig. 6.1 to: (i) state the radius of the sphere radius = … cm [1] (ii) calculate the charge on the sphere. charge = … C [2] (c) Using the formula for the electric potential due to an isolated point charge, determine the capacitance of the sphere in (b). capacitance = … F [3] [Total: 7]
7 marks
Mark scheme: 6(a) (both have) radial field lines B1 6(b)(i) 2.1 cm B1 6(b)(ii) 2 4 o Q E r πε = e.g. r = 2.1 cm, E = 1.30 × 105 V m–1 2 4 o Q r E πε = 12 2 5 4 8.85 10 0.021 1.30 10 π − = × × × × × × C1 9 6.4 10 C − = × A1 Question Answer Marks 6(c) Q C V = either 4 o Q V r πε = leading to 4 o C r πε = C1 12 4 8.85 10 0.021 C π − = × × × × C1 ( ) 12 2.3 10 C − = × F A1 or 4 o Q V r πε = 9 12 6.4 10 4 8.85 10 0.021 π − − × = × × × × 2740 V = 9 6.4 10 2740 C − × = (C1) 12 2.3 10 F − = × (A1)
6 (a) An isolated metal sphere of radius r is charged so that the electric field strength at its surface is E0. On Fig. 6.1, sketch the variation of the electric field strength E with distance x from the centre of the sphere. Your sketch should extend from x = 0 to x = 3r. E0 field strength E 0 0 r 2r 3r distance x Fig. 6.1 [3] (b) The de Broglie wavelength of a particle is λ 0 when its momentum is p0. On Fig. 6.2, sketch the variation with momentum p of the de Broglie wavelength λ of the p0 particle for values of momentum from to p0. 2 2λ0 wavelength λ λ 0 0 0 p0 p0 2 momentum p Fig. 6.2 [2] (c) A radioactive isotope decays with a half-life of 15 s to form a stable product. A fresh sample of the radioactive isotope at time t = 0 contains N0 nuclei and no nuclei of the stable product. On Fig. 6.3, sketch the variation with t of the number n of nuclei of the stable product for time t = 0 to time t = 45 s. N0 number n 0.5 N0 0 0 15 30 45 time t / s Fig. 6.3 [3] [Total: 8]
8 marks
Mark scheme: 6(a) from x = 0 to x = r: E = 0 B1 from x = r to x = 3r: curve with negative gradient of decreasing magnitude passing through (r, E0) B1 line passing through (2r, E0 / 4) and (3r, E0 / 9) B1 6(b) from p = p0 / 2 to p = p0: curve with negative gradient of decreasing magnitude passing through (p0, λ0) B1 line passing through (½p0, 2λ0) B1 6(c) from t = 0 to t = 45 s: curve with positive gradient of decreasing magnitude starting at (0, 0) B1 line passing through (15, ½N0) B1 line passing through (30, 0.75N0) and (45, 0.88N0) B1
6 (a) An isolated metal sphere of radius r is charged so that the electric field strength at its surface is E0. On Fig. 6.1, sketch the variation of the electric field strength E with distance x from the centre of the sphere. Your sketch should extend from x = 0 to x = 3r. E0 field strength E 0 0 r 2r 3r distance x Fig. 6.1 [3] (b) The de Broglie wavelength of a particle is λ 0 when its momentum is p0. On Fig. 6.2, sketch the variation with momentum p of the de Broglie wavelength λ of the p0 particle for values of momentum from to p0. 2 2λ0 wavelength λ λ 0 0 0 p0 p0 2 momentum p Fig. 6.2 [2] (c) A radioactive isotope decays with a half-life of 15 s to form a stable product. A fresh sample of the radioactive isotope at time t = 0 contains N0 nuclei and no nuclei of the stable product. On Fig. 6.3, sketch the variation with t of the number n of nuclei of the stable product for time t = 0 to time t = 45 s. N0 number n 0.5 N0 0 0 15 30 45 time t / s Fig. 6.3 [3] [Total: 8]
8 marks
Mark scheme: 6(a) from x = 0 to x = r: E = 0 B1 from x = r to x = 3r: curve with negative gradient of decreasing magnitude passing through (r, E0) B1 line passing through (2r, E0 / 4) and (3r, E0 / 9) B1 6(b) from p = p0 / 2 to p = p0: curve with negative gradient of decreasing magnitude passing through (p0, λ0) B1 line passing through (½p0, 2λ0) B1 6(c) from t = 0 to t = 45 s: curve with positive gradient of decreasing magnitude starting at (0, 0) B1 line passing through (15, ½N0) B1 line passing through (30, 0.75N0) and (45, 0.88N0) B1
5 (a) Define electric potential at a point. … … … [2] (b) An isolated conducting sphere is charged. Fig. 5.1 shows the variation of the potential V due to the sphere with displacement x from its centre. 0 – 0.3 – 0.2 – 0.1 0 0.1 0.2 0.3 x / m – 250 V / V – 500 – 750 – 1000 Fig. 5.1 Use Fig. 5.1 to determine: (i) the radius of the sphere radius = … m [1] (ii) the charge on the sphere. charge = … C [2] (c) Two spheres are identical to the sphere in (b). Each sphere has the same charge as the sphere in (b). The spheres are held in a vacuum so that their centres are separated by a distance of 0.46 m. Assume that the charge on each sphere is a point charge at the centre of the sphere. (i) Calculate the electric potential energy EP of the two spheres. EP = … J [2] (ii) The two spheres are now released simultaneously so that they are free to move. Describe and explain the subsequent motion of the spheres. … … … … [3] [Total: 10]
10 marks
Mark scheme: 5(a) work done per unit charge B1 work done (on charge) in moving positive charge from infinity (to the point) B1 5(b)(i) radius = 0.060 m A1 5(b)(ii) V = Q / 40x C1 Q = (–) 850 4 8.85 10–12 0.060 or Q = (–) 850 0.060 / 8.99 109 (any correct pair of V and x values from curve) Q = – 5.7 10–9 C A1 5(c)(i) EP = Q2 / 40x C1 = (5.67 10–9)2 / (4 8.85 10–12 0.46) = 6.3 10–7 J A1 5(c)(ii) • force is repulsive so spheres move apart B3 • force in direction of motion so speed increases • potential energy converted to kinetic energy so speed increases • force decreases with distance so acceleration decreases • momentum is conserved (at zero) (and masses are equal) so velocities are always equal and opposite Any three points, 1 mark each
5 (a) State the relationship between electric field and electric potential. … … … [2] (b) Two charged isolated insulating spheres X and Y are near to each other, as shown in Fig. 5.1. X Y P Fig. 5.1 P is a point on the line joining the centres of the spheres. Explain why it is not possible for the total electric potential and the resultant electric field to simultaneously be zero at point P. … … … … … [3] (c) The magnitudes of the charges on spheres X and Y in Fig. 5.1 are Q and 2Q respectively. The spheres may be considered as point charges at their centres. Point P is a distance x from the centre of sphere X. The electric potential at point P is zero. (i) Show that the distance y of point P from the centre of sphere Y is equal to 2x. [2] (ii) State an expression, in terms of Q, x and the permittivity of free space ε0, for the electric field strength EX at P due to sphere X. EX = … [1] (iii) Determine an expression, in terms of Q, x and ε0, for the resultant electric field strength E at point P due to the two spheres. E = … [2] [Total: 10]
10 marks
Mark scheme: 5(a) (electric) field equals (electric) potential gradient M1 reference to minus sign A1 5(b) • for potential to be zero, one potential must be positive and the other potential must be negative B3 • for potential to be zero, the charges must have opposite sign • for field to be zero, the fields (due to X and Y) must be in opposite directions • for field to be zero, the charges must have the same sign • the signs of the charges cannot (simultaneously) be both the same and opposite (so not possible) Any three points, 1 mark each 5(c)(i) VX = (–) Q / 4ε0x and VY = (–) 2Q / 4ε0y C1 (VX + VY = 0 so) Q / 4ε0x = 2Q / 4ε0y leading to y = 2x A1 5(c)(ii) EX = Q / 4ε0x2 A1 5(c)(iii) EY = 2Q / 4ε0(2x)2 C1 ( = Q / 8ε0x2) (opposite charges so fields in same direction so magnitudes add): A1 E = (Q / 4ε0x2) + (Q / 8ε0x2) = 3Q / 8ε0x2
6 (a) State Coulomb’s law. … … … [2] (b) Fig. 6.1 shows an isolated hollow conducting sphere that is positively charged. + + + + + + + + Fig. 6.1 On Fig. 6.1, draw field lines to represent the electric field outside the sphere. [3] (c) Fig. 6.2 shows the variation of the electric field strength E with distance x from the centre of the sphere in (b). 3 E / 105 N C–1 2 1 0 0 2 4 6 8 x / cm Fig. 6.2 (i) Determine the radius, in cm, of the sphere. radius = … cm [1] (ii) Calculate the charge on the sphere. charge = … C [3] (iii) Suggest an explanation for the fact that the electric field inside the sphere is zero. … … … [1] [Total: 10]
10 marks
Mark scheme: 6(a) (electric) force is (directly) proportional to product of charges B1 force (between point charges) is inversely proportional to the square of their separation B1 6(b) at least four straight, radial lines to/from surface of sphere B1 at least four straight radial lines drawn, approximately equally spaced B1 arrows pointing away from the surface of the sphere B1 6(c)(i) radius = 3.2 cm A1 6(c)(ii) E = Q / (40x2) C1 Q = e.g. 2.2 105 4 8.85 10–12 0.0322 C1 = 2.5 10–8 C A1 6(c)(iii) • the (positive) charge is all the way around the surface B1 • a charge placed inside the sphere is pulled equally in all directions • if the field was not zero, the charges would move (until field is zero) • electric field lines go from positive charge to negative charge, and there are no negative charges inside the sphere Any point, 1 mark
5 (a) State the relationship between electric field and electric potential. … … … [2] (b) Two charged isolated insulating spheres X and Y are near to each other, as shown in Fig. 5.1. X Y P Fig. 5.1 P is a point on the line joining the centres of the spheres. Explain why it is not possible for the total electric potential and the resultant electric field to simultaneously be zero at point P. … … … … … [3] (c) The magnitudes of the charges on spheres X and Y in Fig. 5.1 are Q and 2Q respectively. The spheres may be considered as point charges at their centres. Point P is a distance x from the centre of sphere X. The electric potential at point P is zero. (i) Show that the distance y of point P from the centre of sphere Y is equal to 2x. [2] (ii) State an expression, in terms of Q, x and the permittivity of free space ε0, for the electric field strength EX at P due to sphere X. EX = … [1] (iii) Determine an expression, in terms of Q, x and ε0, for the resultant electric field strength E at point P due to the two spheres. E = … [2] [Total: 10]
10 marks
Mark scheme: 5(a) (electric) field equals (electric) potential gradient M1 reference to minus sign A1 5(b) • for potential to be zero, one potential must be positive and the other potential must be negative B3 • for potential to be zero, the charges must have opposite sign • for field to be zero, the fields (due to X and Y) must be in opposite directions • for field to be zero, the charges must have the same sign • the signs of the charges cannot (simultaneously) be both the same and opposite (so not possible) Any three points, 1 mark each 5(c)(i) VX = (–) Q / 4ε0x and VY = (–) 2Q / 4ε0y C1 (VX + VY = 0 so) Q / 4ε0x = 2Q / 4ε0y leading to y = 2x A1 5(c)(ii) EX = Q / 4ε0x2 A1 5(c)(iii) EY = 2Q / 4ε0(2x)2 C1 ( = Q / 8ε0x2) (opposite charges so fields in same direction so magnitudes add): A1 E = (Q / 4ε0x2) + (Q / 8ε0x2) = 3Q / 8ε0x2
2 A helium atom may be modelled as a nucleus surrounded by two electrons in diametrically opposite circular orbits, each of radius 170 pm, as shown in Fig. 2.1. orbit of electrons 170 pm electron electron nucleus Fig. 2.1 (a) State Coulomb’s law. … … … [2] (b) (i) State the charge on the nucleus, in terms of the elementary charge e. charge = … e [1] (ii) Show that the electric force between the nucleus and one of the electrons is 1.6 × 10–8 N. [1] (c) Assume that the force in (b)(ii) is the only force on the electrons. (i) Calculate the speed of the orbiting electrons. speed = … m s–1 [2] (ii) Calculate the period of the orbit of the electrons. period = … s [2] (d) In practice, the orbit of each electron is affected by the presence of the other electron. (i) For the position of one of the electrons, determine the ratio electric field strength due to the other electron . electric field strength due to the nucleus ratio = … [2] (ii) Use your answer in (d)(i) to suggest and explain how the orbit of the electron is affected by the presence of the other electron. … … [1] [Total: 11]
11 marks
Mark scheme: 2(a) (electric) force is (directly) proportional to product of charges B1 force (between point charges) is inversely proportional to the square of their separation B1 2(b)(i) charge = (+)2e A1 2(b)(ii) F = 2 × (1.60 × 10–19)2 / [4 × 8.85 × 10–12 × (170 × 10–12)2] = 1.6 × 10–8 N A1 2(c)(i) F = mv2 / r C1 v = [ (1.6 × 10–8 × 170 × 10–12) / (9.11 × 10–31) ]½ A1 = 1.7 × 106 m s–1 2(c)(ii) F = mr2 and = 2 / T C1 F = 42mr / T2 T = [ (42 × 9.11 × 10–31 × 170 × 10–12) / (1.6 × 10–8) ]½ A1 = 6.2 × 10–16 s or v = 2r / T (C1) T = (2 × 170 × 10–12) / (1.73 × 106) (A1) = 6.2 × 10–16 s 2(d)(i) E Q / r2 C1 ratio = [1.60 × 10–19 × (170 × 10–12)2] / [3.2 × 10–19 × (340 × 10–12)2] A1 = 0.13 2(d)(ii) resultant force slightly less (than 1.6 × 10–8 N) so speed lower B1 or resultant force slightly less (than 1.6 × 10–8 N) so period greater
2 A helium atom may be modelled as a nucleus surrounded by two electrons in diametrically opposite circular orbits, each of radius 170 pm, as shown in Fig. 2.1. orbit of electrons 170 pm electron electron nucleus Fig. 2.1 (a) State Coulomb’s law. … … … [2] (b) (i) State the charge on the nucleus, in terms of the elementary charge e. charge = … e [1] (ii) Show that the electric force between the nucleus and one of the electrons is 1.6 × 10–8 N. [1] (c) Assume that the force in (b)(ii) is the only force on the electrons. (i) Calculate the speed of the orbiting electrons. speed = … m s–1 [2] (ii) Calculate the period of the orbit of the electrons. period = … s [2] (d) In practice, the orbit of each electron is affected by the presence of the other electron. (i) For the position of one of the electrons, determine the ratio electric field strength due to the other electron . electric field strength due to the nucleus ratio = … [2] (ii) Use your answer in (d)(i) to suggest and explain how the orbit of the electron is affected by the presence of the other electron. … … [1] [Total: 11]
11 marks
Mark scheme: 2(a) (electric) force is (directly) proportional to product of charges B1 force (between point charges) is inversely proportional to the square of their separation B1 2(b)(i) charge = (+)2e A1 2(b)(ii) F = 2 × (1.60 × 10–19)2 / [4 × 8.85 × 10–12 × (170 × 10–12)2] = 1.6 × 10–8 N A1 2(c)(i) F = mv2 / r C1 v = [ (1.6 × 10–8 × 170 × 10–12) / (9.11 × 10–31) ]½ A1 = 1.7 × 106 m s–1 2(c)(ii) F = mr2 and = 2 / T C1 F = 42mr / T2 T = [ (42 × 9.11 × 10–31 × 170 × 10–12) / (1.6 × 10–8) ]½ A1 = 6.2 × 10–16 s or v = 2r / T (C1) T = (2 × 170 × 10–12) / (1.73 × 106) (A1) = 6.2 × 10–16 s 2(d)(i) E Q / r2 C1 ratio = [1.60 × 10–19 × (170 × 10–12)2] / [3.2 × 10–19 × (340 × 10–12)2] A1 = 0.13 2(d)(ii) resultant force slightly less (than 1.6 × 10–8 N) so speed lower B1 or resultant force slightly less (than 1.6 × 10–8 N) so period greater
5 (a) Define electric potential at a point. … … … [2] (b) An isolated solid metal sphere of radius r is given a positive charge. The potential at the surface of the sphere is 9.0 × 104 V. At a distance of 3r from the centre of the sphere, the electric field strength is 2.0 × 105 N C–1. (i) Determine the electric field strength at the surface of the sphere. electric field strength = … N C–1 [2] (ii) Show that the radius of the sphere is 5.0 cm. [2] (iii) Calculate the charge on the sphere. charge = … C [2] (iv) Use your answer in (b)(iii) to determine the capacitance of the sphere. capacitance = … F [2] [Total: 10]
10 marks
Mark scheme: 5(a) work done per unit charge B1 work done (on charge) in moving positive charge from infinity (to the point) B1 5(b)(i) electric field strength inversely proportional to distance2 C1 E = 32 2.0 105 A1 = 1.8 106 N C–1 5(b)(ii) V = Q / 40r and E = Q / 40r2 (so E = V / r) B1 r = (9.0 104) / (1.8 106) = 0.050 m = 5.0 cm A1 5(b)(iii) Q = 40Vr C1 = 4 8.85 10–12 9.0 104 0.050 = 5.0 10–7 C A1 5(b)(iv) C = Q / V C1 = (5.0 10–7) / (9.0 104) A1 = 5.6 10–12 F
5 (a) Explain why the electric potential near an isolated proton is positive. … … … … … [3] (b) An isolated metal sphere is positively charged and has radius R, as shown in Fig. 5.1. sphere + + + + R + + P X Y + + Q + + + + x Fig. 5.1 Line XY passes through the centre of the sphere. Point P lies on line XY at a variable displacement x from the centre of the sphere. Point Q is at a fixed position that is not on line XY. The electric field strength at the surface of the sphere is E0. (i) On Fig. 5.1, draw an arrow at point Q to show the direction of the electric field at that point. [1] (ii) On Fig. 5.2, sketch the variation of the electric field E at point P with x for values of x between x = –3R and x = 3R. Do not include the region inside the sphere between x = –R and x = R. E0 E ½E0 0 –3R –2R –R 0 R 2R 3R x –½E0 –E0 Fig. 5.2 [3] (c) The proton and the electron in a hydrogen atom are separated by a distance of 5.3 × 10–11 m. Calculate the electric potential energy of the proton and the electron. electric potential energy = … J [2] [Total: 9]
9 marks
Mark scheme: 5(a) potential is (defined as) zero at infinity B1 proton has a positive charge and so repels another positive charge B1 work is done on two (positive) charges to move them towards each other B1 or work is done by two (positive) charges as they move apart from each other 5(b)(i) arrow drawn through Q in a WSW direction directly away from the centre of the sphere B1 5(b)(ii) curve in at least one quadrant passing through (R, E0) and (2R, ¼E0) B1 curve between –3R and –R of increasing magnitude of gradient B1 and curve between R and 3R of decreasing magnitude of gradient two lines drawn, one in the top right quadrant, the other in the bottom left quadrant B1 5(c) EP = – (1.60 10–19)2 / [4 8.85 10–12 (5.3 10–11)] C1 = –4.3 10–18 J A1