33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020
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Telegram @unacademyplusdiscounts8 NEET-AIPMT Chapterwise Topicwise Solutions Physics10. Three concentric spherical shells have radii a, b and c(a < b < c) and have surface charge densities s, –s and srespectively. If V A , V B and V C denote the potentials ofthe three shells, then, for c = a + b, we have(a) V C = V B ≠ V A (b) V C ≠ V B ≠ V A(c) V C = V B = V A (d) V C = V A ≠ V B (2009)11. A hollow metallic sphere of radius 10 cm is chargedsuch that potential of its surface is 80 V. The potentialat the centre of the sphere would be(a) 80 V (b) 800 V (c) zero (d) 8 V (1994)2.6 Equipotential Surfaces12. The diagrams below show regions of equipotentials.17. The electric potential at a point (x, y, z) is given byV = –x 2 y – xz 3 + 4. The electric field at that point is(a) E= ^ i xy + j ^ 2 2x + y + k ^ 22 ( ) ( 3xz − y ) ^(b)3 ^ ^ 2E= iz + j xyz + kz ^(c)3 ^ 2 ^ 2E= i ( 2xy − z ) + j xy + k3z x ^(d)3 ^ 2 ^ 2E= i ( 2xy + z ) + j x + k3xz(2009)18. Charge q 2 is at the centre of a circular path withradius r. Work done in carrying charge q 1 , oncearound this equipotential path, would be1 1 2(a)4πε × qq1 1 2(b)20 r4πε × qq 0 r(c) zero (d) infinite. (1994)2.7 Potential Energy of a System of ChargesA positive charge is moved from A to B in each diagram.(a) In all the four cases the work done is the same.(b) Minimum work is required to move q in figure (I).(c) Maximum work is required to move q in figure (II).(d) Maximum work is required to move q infigure (III). (NEET 2017)13. If potential (in volts) in a region is expressed asV(x, y, z) = 6xy – y + 2yz, the electric field (in N/C)at point (1, 1, 0) is^ ^ ^(a) − ( 2i+ 3j+k ) (b) − ( 6 ^ i+ 9^ j+k^ )^ ^ ^(c) − ( 3i+ 5j+3k )^ ^ ^(d) − ( 6i+ 5j+2k ) (2015)14. In a region, the potential is represented by V(x, y, z) =6x – 8xy – 8y + 6yz, where V is in volts and x, y, z are inmetres. The electric force experienced by a charge of2 coulomb situated at point (1, 1, 1) is(a) 6 5N (b) 30 N (c) 24 N (d) 4 35N(2014)15. A, B and C are three points in a uniform electricfield. The electric potential is(a) maximum at C(b) same at all the threepoints A, B and C(c) maximum at A(d) maximum at B (NEET 2013)16. The electric potential V at any point (x, y, z), all inmetres in space is given by V = 4x 2 volt. The electricfield at the point (1, 0, 2) in volt/meter, is(a) 8 along negative X-axis(b) 8 along positive X-axis(c) 16 along negative X-axis(d) 16 along positive X-axis (Mains 2011)19. Three charges, each +q, are placed atthe corners of an isosceles triangleABC of sides BC and AC, 2a. D and Eare the mid points of BC and CA. Thework done in taking a charge Q fromD to E is(a)3qQ4πε0a(c)qQ4πε0 a(b)3qQ8πε0a(d) zero (Mains 2011)20. Charges +q and –q are placed at points A and Brespectively which are a distance 2L apart, C isthe midpoint between A and B. The work done inmoving a charge +Q along the semicircle CRD is(a)qQ2πε0 L(b)qQ6πε0 LqQ4πε0 L(c) −qQ (d)(2007)6πε0L21. Two charges q 1 and q 2 are placed 30 cm apart, asshown in the figure. A third charge q 3 is movedalong the arc of a circle of radius 40 cm from C to D.The change in the potentialenergy of the system isq3k, where k is4πε 0(a) 8q 1(b) 6q 1(c) 8q 2(d) 6q 2 (2005)
Telegram @unacademyplusdiscountsElectrostatic Potential and Capacitance922. Identical charges (–q) are placed at each corners ofcube of side b, then electrostatic potential energy ofcharge (+q) which is placed at centre of cube will be(a)−4 2 q2(b) −8 2 q2πε0bπε0b(c)2−4 q(d) 8 2 2q3πε0b4πε0b(2002)23. In bringing an electron towards another electron,the electrostatic potential energy of the system(a) becomes zero (b) increases(c) decreases (d) remains same (1999)2.8 Potential Energy in an External Field24. An electric dipole of dipole moment p is alignedparallel to a uniform electric field E. The energyrequired to rotate the dipole by 90° is(a) p 2 E (b) pE (c) infinity (d) pE 2(Karnataka NEET 2013)25. An electric dipole of moment p is placed in an electricfield of intensity E. The dipole acquires a position suchthat the axis of the dipole makes an angle q with thedirection of the field. Assuming that the potential energyof the dipole to be zero when q = 90°, the torque and thepotential energy of the dipole will respectively be(a) pEsinq, –pEcosq (b) pEsinq, –2pEcosq(c) pEsinq, 2pEcosq (d) pEcosq, –pEsinq (2012)26. An electric dipole of moment p is lying along auniform electric field E. The work done in rotatingthe dipole by 90° is(a) pE (b) 2pE (c) pE/2 (d) 2pE (2006)27. An electric dipole has the magnitude of its charge asq and its dipole moment is p. It is placed in a uniformelectric field E. If its dipole moment is along thedirection of the field, the force on it and its potentialenergy are respectively(a) 2q · E and minimum(b) q · E and p · E(c) zero and minimum(d) q · E and maximum (2004)28. There is an electric field E in x-direction. If the workdone on moving a charge of 0.2 C through a distanceof 2 m along a line making an angle 60° with x-axis is4 J, then what is the value of E ?(a) 5 N/C(b) 20 N/C(c) 3 N/C (d) 4 N/C (1995)29. An electric dipole of moment p is placed in theposition of stable equilibrium in uniform electricfield of intensity E. This is rotated through an angleq from the initial position. The potential energy ofthe electric dipole in the final position is(a) –pE cosq (b) pE(1 – cosq)(c) pE cosq (d) pE sinq (1994)2.9 Electrostatics of Conductors30. Some charge is being given to a conductor. Then itspotential is(a) maximum at surface(b) maximum at centre(c) remain same throughout the conductor(d) maximum somewhere between surface andcentre. (2002)2.11 Capacitors and Capacitance31. Two metallic spheres of radii 1 cm and 3 cm are givencharges of –1 × 10 –2 C and 5 × 10 –2 C, respectively. Ifthese are connected by a conducting wire, the finalcharge on the bigger sphere is(a) 2 × 10 –2 C (b) 3 × 10 –2 C(c) 4 × 10 –2 C (d) 1 × 10 –2 C (Mains 2012)32. Two metallic spheres of radii 1 cm and 2 cmare given charges 10 –2 C and 5 × 10 –2 C respectively.If they are connected by a conducting wire, the finalcharge on the smaller sphere is(a) 3 × 10 –2 C (b) 4 × 10 –2 C(c) 1 × 10 –2 C (d) 2 × 10 –2 C (1995)2.12 The Parallel Plate Capacitor33. The electrostatic force between the metal plates of anisolated parallel plate capacitor C having a charge Qand area A, is(a) independent of the distance between the plates(b) linearly proportional to the distance betweenthe plates(c) proportional to the square root of the distancebetween the plates(d) inversely proportional to the distance betweenthe plates. (NEET 2018)34. A parallel plate air capacitor has capacity C, distanceof separation between plates is d and potentialdifference V is applied between the plates. Force ofattraction between the plates of the parallel plate aircapacitor is(a) CV 2(b) CV 2 2(c) CV 2 22CV(d) (2015)d22d2d2d35. A parallel plate air capacitor is charged to a potentialdifference of V volts. After disconnecting the chargingbattery the distance between the plates of thecapacitor is increased using an insulating handle. Asa result the potential difference between the plates(a) increases (b) decreases(c) does not change (d) becomes zero (2006)
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8 NEET-AIPMT Chapterwise Topicwise Solutions Physics
10. Three concentric spherical shells have radii a, b and c
(a < b < c) and have surface charge densities s, –s and s
respectively. If V A , V B and V C denote the potentials of
the three shells, then, for c = a + b, we have
(a) V C = V B ≠ V A (b) V C ≠ V B ≠ V A
(c) V C = V B = V A (d) V C = V A ≠ V B (2009)
11. A hollow metallic sphere of radius 10 cm is charged
such that potential of its surface is 80 V. The potential
at the centre of the sphere would be
(a) 80 V (b) 800 V (c) zero (d) 8 V (1994)
2.6 Equipotential Surfaces
12. The diagrams below show regions of equipotentials.
17. The electric potential at a point (x, y, z) is given by
V = –x 2 y – xz 3 + 4. The electric field at that point is
(a) E= ^ i xy + j ^ 2 2
x + y + k ^ 2
2 ( ) ( 3xz − y )
^
(b)
3 ^ ^ 2
E= iz + j xyz + kz
^
(c)
3 ^ 2 ^ 2
E= i ( 2xy − z ) + j xy + k3z x
^
(d)
3 ^ 2 ^ 2
E= i ( 2xy + z ) + j x + k3xz
(2009)
18. Charge q 2 is at the centre of a circular path with
radius r. Work done in carrying charge q 1 , once
around this equipotential path, would be
1 1 2
(a)
4πε × qq
1 1 2
(b)
2
0 r
4πε × qq 0 r
(c) zero (d) infinite. (1994)
2.7 Potential Energy of a System of Charges
A positive charge is moved from A to B in each diagram.
(a) In all the four cases the work done is the same.
(b) Minimum work is required to move q in figure (I).
(c) Maximum work is required to move q in figure (II).
(d) Maximum work is required to move q in
figure (III). (NEET 2017)
13. If potential (in volts) in a region is expressed as
V(x, y, z) = 6xy – y + 2yz, the electric field (in N/C)
at point (1, 1, 0) is
^ ^ ^
(a) − ( 2i+ 3j+
k ) (b) − ( 6 ^ i+ 9
^ j+
k
^ )
^ ^ ^
(c) − ( 3i+ 5j+
3k )
^ ^ ^
(d) − ( 6i+ 5j+
2k ) (2015)
14. In a region, the potential is represented by V(x, y, z) =
6x – 8xy – 8y + 6yz, where V is in volts and x, y, z are in
metres. The electric force experienced by a charge of
2 coulomb situated at point (1, 1, 1) is
(a) 6 5N (b) 30 N (c) 24 N (d) 4 35N(2014)
15. A, B and C are three points in a uniform electric
field. The electric potential is
(a) maximum at C
(b) same at all the three
points A, B and C
(c) maximum at A
(d) maximum at B (NEET 2013)
16. The electric potential V at any point (x, y, z), all in
metres in space is given by V = 4x 2 volt. The electric
field at the point (1, 0, 2) in volt/meter, is
(a) 8 along negative X-axis
(b) 8 along positive X-axis
(c) 16 along negative X-axis
(d) 16 along positive X-axis (Mains 2011)
19. Three charges, each +q, are placed at
the corners of an isosceles triangle
ABC of sides BC and AC, 2a. D and E
are the mid points of BC and CA. The
work done in taking a charge Q from
D to E is
(a)
3qQ
4πε0a
(c)
4πε0 a
(b)
3qQ
8πε0a
(d) zero (Mains 2011)
20. Charges +q and –q are placed at points A and B
respectively which are a distance 2L apart, C is
the midpoint between A and B. The work done in
moving a charge +Q along the semicircle CRD is
(a)
2πε0 L
(b)
6πε0 L
4πε0 L
(c) −
qQ (d)
(2007)
6πε0L
21. Two charges q 1 and q 2 are placed 30 cm apart, as
shown in the figure. A third charge q 3 is moved
along the arc of a circle of radius 40 cm from C to D.
The change in the potential
energy of the system is
q
3
k, where k is
4πε 0
(a) 8q 1
(b) 6q 1
(c) 8q 2
(d) 6q 2 (2005)