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Questions on electric potential
Electric potential is the work done per unit positive charge in bringing a charge from infinity to the point, and its sign follows the sign of the source charge. V = Q/4πε₀r is positive around a positive charge and negative around a negative one, unlike gravitational potential. A volt is a joule per coulomb, and ΔW = QΔV gives the energy transferred.
19 original questions · 51 marks · the electric potential notes · Electric fields
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Define the absolute electric potential at a point in an electric field.
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Work done per unit positive charge (1); in bringing a small test charge from infinity to the point (where the potential at infinity is zero) (1).Calculate the electric potential at a distance of 0.10 m from a point charge of 5.0 × 10−9 C.
k = 8.99 × 109 N m2 C−2Mark scheme
V = kQ/r = (8.99 × 109 × 5.0 × 10−9)/0.10 (1)
V = 450 V (1)Describe the equipotential surfaces around an isolated point charge and state how they are related to the electric field lines.
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Concentric spheres centred on the charge (1); everywhere perpendicular to the radial field lines (and no work is done moving a charge along an equipotential) (1).A charge of 5.0 μC is moved 0.40 m along an equipotential surface. State the work done on the charge.
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Zero: the potential difference along an equipotential is zero (1).The electric potential at a distance r from a point charge is 800 V. State the potential at a distance 2r, and at a distance 4r, from the charge.
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V ∝ 1/r, so at 2r the potential is 400 V (1) and at 4r it is 200 V (1).State what a potential difference of one volt means, in terms of energy and charge.
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One joule of energy is transferred per coulomb of charge moved through it (1).Calculate the electric potential at a distance of 0.20 m from a point charge of −3.0 × 10−9 C.
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V = kQ/r = (8.99 × 109 × (−3.0 × 10−9))/0.20 (1)
V = −135 V (negative because the charge is negative) (1)A charge of +2.0 × 10−9 C is moved from a point 0.30 m from a fixed point charge of 5.0 × 10−9 C to a point 0.10 m from it. Calculate the potential difference between the two points and the work done on the charge.
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V at 0.10 m = 450 V (1)
V at 0.30 m = 150 V (1)
ΔV = 300 V (1)
W = QΔV = 2.0 × 10−9 × 300 = 6.0 × 10−7 J (1)In a uniform electric field the potential changes by 200 V over a distance of 0.050 m along a field line. Calculate the electric field strength.
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E = ΔV/Δd = 200/0.050 (1)
E = 4000 V m−1 (1)Two point charges, each of +4.0 μC, are placed so that each is 0.20 m from a point P. Determine the total electric potential at P.
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Potential is a scalar, so the contributions add (1)
V = 2 × kQ/r = 2 × (8.99 × 109 × 4.0 × 10−6/0.20) (1)
V = 3.60 × 105 V (1)Determine the distance from a point charge of +12 nC at which the electric potential is 450 V.
k = 8.99 × 109 N m2 C−2Mark scheme
V = kQ/r, so r = kQ/V (1)
r = (8.99 × 109 × 12 × 10−9)/450 (1)
r = 0.24 m (1)In a vacuum tube, an electron moves from a point at a potential of +150 V to a point at a potential of +650 V. Calculate the kinetic energy the electron gains, in J and in eV.
e = 1.60 × 10−19 CMark scheme
ΔV = 650 − 150 = 500 V (1)
The electron's charge is negative, so moving to the higher potential lowers its potential energy by qΔV and that fall becomes kinetic energy: ΔEk = eΔV = 1.60 × 10−19 × 500 = 8.0 × 10−17 J (1)
= 500 eV (1)A small charge is moved from point X to point Y in the field of a fixed point charge, once along a straight line and once along a much longer curved path. State and explain how the work done in the two cases compares.
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The work done is the same (1); it depends only on the potential difference between X and Y, not on the path taken (1).A charge of +5.0 μC is placed at a point where the electric potential is 2000 V. Calculate the electric potential energy of the charge and state the work done in bringing it to this point from infinity.
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Ep = QV = 5.0 × 10−6 × 2000 (1)
Ep = 0.010 J (1)
Work done from infinity = 0.010 J, equal to the potential energy gained (1).A +6.0 μC charge and a −6.0 μC charge are placed so that each is 0.30 m from a point P. Calculate the total electric potential at P and explain your result.
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V = kQ1/r + kQ2/r (1)
V = (8.99 × 109 × 6.0 × 10−6/0.30) + (8.99 × 109 × (−6.0 × 10−6)/0.30) (1)
V = 0 V (1)
The two contributions are equal in magnitude but opposite in sign, and potential is a scalar, so they cancel exactly (1).Explain how the electric field strength at a point can be found from a graph of electric potential against distance.
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E equals the magnitude of the gradient of the potential-distance graph at that point, E = ΔV/Δr (1); the field is directed from high to low potential (1). Conversely, the change in potential between two points equals the area under the field strength-distance graph (1).A charge of +8.0 nC is fixed at point A and a charge of −2.0 nC is fixed at point B, 0.50 m from A. Determine the distance from A of the point on the line between the charges at which the total electric potential is zero.
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Potential is a scalar, so the two contributions must sum to zero: in magnitude, kQA/d = kQB/(0.50 − d) (1)
8.0(0.50 − d) = 2.0d (1)
d = (8.0 × 0.50)/10.0 (1)
d = 0.40 m from A (1)Two protons are held 1.0 × 10−12 m apart in a vacuum. One is kept fixed and the other is released from rest. Calculate the speed of the released proton when it is very far from the fixed one. Assume that only the electrostatic force acts.
k = 8.99 × 109 N m2 C−2, e = 1.60 × 10−19 C, mp = 1.67 × 10−27 kgMark scheme
Potential at the released proton due to the fixed one: V = ke/r = 1438 V (1)
Ep = QV = 1.60 × 10−19 × 1438 = 2.30 × 10−16 J (1)
Far away V → 0, so all this potential energy becomes kinetic energy (1)
½mv2 = Ep (1)
v = √(2Ep/m) = 5.2 × 105 m s−1 (1)A bird perches with both feet on a single bare overhead cable at a potential of 25 kV. Suggest why the bird is unharmed.
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Both feet touch the same cable, so they are at almost exactly the same potential (1); the potential difference across the bird is therefore almost zero (1). Since W = QΔV, almost no energy is transferred through the bird and no significant current flows in it (1).
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