33 Years NEET-AIPMT Chapterwise Solutions - Physics 2020
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Electric Charges and FieldsTelegram @unacademyplusdiscounts320. A thin conducting ring of radius R is given a charge+Q. The electric field at the centre O of the ring dueto the charge on the part AKB of the ring is E. Theelectric field at the centre due to the charge on thepart ACDB of the ring is(a) E along KO(b) 3E along OK(c) 3E along KO(d) E along OK (2008)21. Electric field at centre O of semicircleof radius a having linear charge densityl given as2λλπ(a)(b)ε aε 0 a(c)0λ2πε0 a (d)1.14 Gauss’s Lawλπε 0 a(2000)22. What is the flux through a cube of side a if a pointcharge of q is at one of its corner?(a)2qq q q 2(b) (c) (d) 6aε 8ε00 ε 0 2ε 0 (2012)23. A charge Q is enclosed by a Gaussian sphericalsurface of radius R. If the radius is doubled, then theoutward electric flux will(a) increase four times (b) be reduced to half(c) remain the same (d) be doubled (2011)24. A hollow cylinder has a charge q coulomb withinit. If f is the electric flux in units of volt meterassociated with the curved surface B, the flux linkedwith the plane surface A in units of V-m will beq(a)2ε0(b) φ 3q(c) − φ(d) 1 ⎛ q ⎞− φε02 ⎝⎜ε0⎠⎟(2007)25. A charge q is located at the centre of a cube. Theelectric flux through any face is2πq4πq(a)(b)64 ( πε0)64 ( πε0)πqq(c)(d)(2003)64 ( πε0)64 ( πε0)26. A charge Q mC is placed at the centre of a cube, theflux coming out from each face will beQ(a)6106ε × − Q(b) 1006ε × −30QQ(c)(d)(2001)24ε08ε027. A charge Q is situated at the corner of a cube, the electricflux passed through all the six faces of the cube isQ Q Q Q(a) (b) (c) (d) (2000)6ε0 8ε0 ε 0 2ε028. A point charge + q is placed at the centre of a cubeof side l. The electric flux emerging from the cube is6ql2 q(a) (b)ε06l2 (c) zero (d) q . (1996)εε001.15 Applications of Gauss’s Law29. A hollow metal sphere of radius R is uniformlycharged. The electric field due to the sphere at adistance r from the centre(a) decreases as r increases for r < R and for r > R(b) increases as r increases for r < R and for r > R(c) zero as r increases for r < R, decreases as rincreases for r > R(d) zero as r increases for r < R, increases as rincreases for r > R (NEET 2019)30. Two parallel infinite line charges with linear chargedensities +l C/m and –l C/m are placed at a distanceof 2R in free space. What is the electric field midwaybetween the two line charges ?λ(a) N/C (b) zero2πε0R 2λ(c)πε0R N/C (d) λN/C (NEET 2019)πε 0 R31. The electric field at a distance 3 R from the centre of2a charged conducting spherical shell of radius R is E.The electric field at a distance R from the centre ofthe sphere is2E(a) zero (b) E (c) (d) E2 3(Mains 2010)32. A hollow insulated conduction sphere is given apositive charge of 10 mC. What will be the electric fieldat the centre of the sphere if its radius is 2 metres ?(a) 20 mC m –2 (b) 5 mC m –2(c) zero (d) 8 mC m –2 (1998)ANSWER KEY1. (c) 2. (b) 3. (a) 4. (d) 5. (c) 6. (c) 7. (a) 8. (c) 9. (a) 10. (b)11. (a) 12. (c) 13. (d) 14. (d) 15. (a) 16. (d) 17. (b) 18. (b) 19. (b) 20. (d)21. (c) 22. (b) 23. (c) 24. (d) 25. (b) 26. (a) 27. (b) 28. (d) 29. (c) 30. (d)31. (a) 32. (c)
Telegram @unacademyplusdiscounts4 NEET-AIPMT Chapterwise Topicwise Solutions PhysicsHints & Explanations1. (c) : In case I : Q r – QABQF =− 1 24πε20 r In Case II : Q Q Q Q Q QA = − , B =− +4 41∴ F′ =4πε0⎛ ⎞−⎝⎜⎠⎟ ⎛⎝⎜ − + ⎞Q Q Q Q⎠⎟4 4r2....(i)⎛ 3 ⎞ ⎛ −3⎞⎝⎜ Q⎠⎟⎝⎜ Q1⎠⎟24 4 1 9 Q...(ii)==−4πε204πε016 2rr From equations (i) and (ii), F′= 9 F162. (b) : A hydrogen atom consists of an electron and aproton.\ Charge on one hydrogen atom= q e + q p = –e + (e + De) = DeSince a hydrogen atom carries a net charge Dee\ Electrostatic force, Fe= 1 2( ∆ )...(i)4πε2o dwill act between two hydrogen atoms.The gravitational force between two hydrogen atoms isgiven asGmhmhFg=...(ii)2dSince, the net force on the system is zero, F e = F gUsing eqns. (i) and (ii), we get2 2( ∆e)Gmh= or, 22( ∆e)= 4πεGm2 20 h4πεodd= 6.67 × 10 –11 × (1.67 × 10 –27 ) 2 [1/(9 × 10 9 )]De ≈ 10 –37 C3. (a) :From figure, T cos q = mg...(i)2kqT sinθ=...(ii)2xFrom eqns. (i) and (ii), tanθ= kq 22xmgSinceθissmall, ∴ tanθ≈ sinθ= x 2l2x kq2 3∴ = ⇒ q = x mg32 /or q∝x2l2xmg2lkdq 3⇒ ∝ x dx 3= xvdt 2 dt 2dqSince,constantdt = 1; ∴ v ∝x4. (d) : Let m be mass of each ball and q be charge oneach ball. Force of repulsion,qF = 1 24πε20 rIn equilibriumTcosq = mgTsinq = F...(i)...(ii)Divide (ii) by (i), we get, tanθFrom figure (a),1 qr/24 0 r= πε 2y mg...(iii)For figure (b)12q14πε20 r′r′/ 2 4πεtan θ′ = ⇒0=mg y/2F= =mgrmg2q2′1 q4πε0 r2mg r...(iv)Divide (iv) by (iii), we get232r′ r 3 rr= ⇒ r′ = ⇒ r′ =r ′2 2 3r25. (c) : According to Coulomb’s law, the force ofrepulsion between the two positive ions each of charge q,separated by a distance d is given byq qF = 12( )( )qor F =4πε20 d4πε 0d2q 2 = 4pe 0 Fd 2 or q= 24πε 0Fd...(i)Since, q = newhere, n = number of electrons missing from each ion,e = magnitude of charge on electron
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4 NEET-AIPMT Chapterwise Topicwise Solutions Physics
Hints & Explanations
1. (c) : In case I : Q r – Q
A
B
Q
F =− 1 2
4πε
2
0 r
In Case II : Q Q Q Q Q Q
A = − , B =− +
4 4
1
∴ F′ =
4πε
0
⎛ ⎞
−
⎝
⎜
⎠
⎟ ⎛
⎝
⎜ − + ⎞
Q Q Q Q
⎠
⎟
4 4
r
2
....(i)
⎛ 3 ⎞ ⎛ −3
⎞
⎝
⎜ Q
⎠
⎟
⎝
⎜ Q
1
⎠
⎟
2
4 4 1 9 Q
...(ii)
=
=−
4πε
2
0
4πε0
16 2
r
r
From equations (i) and (ii), F′= 9 F
16
2. (b) : A hydrogen atom consists of an electron and a
proton.
\ Charge on one hydrogen atom
= q e + q p = –e + (e + De) = De
Since a hydrogen atom carries a net charge De
e
\ Electrostatic force, Fe
= 1 2
( ∆ )
...(i)
4πε
2
o d
will act between two hydrogen atoms.
The gravitational force between two hydrogen atoms is
given as
Gmhmh
Fg
=
...(ii)
2
d
Since, the net force on the system is zero, F e = F g
Using eqns. (i) and (ii), we get
2 2
( ∆e)
Gmh
= or, 2
2
( ∆e)
= 4πε
Gm
2 2
0 h
4πεod
d
= 6.67 × 10 –11 × (1.67 × 10 –27 ) 2 [1/(9 × 10 9 )]
De ≈ 10 –37 C
3. (a) :
From figure, T cos q = mg...(i)
2
kq
T sinθ=
...(ii)
2
x
From eqns. (i) and (ii), tanθ= kq 2
2
xmg
Sinceθissmall, ∴ tanθ≈ sinθ
= x 2l
2
x kq
2 3
∴ = ⇒ q = x mg
32 /
or q∝
x
2l
2
xmg
2lk
dq 3
⇒ ∝ x dx 3
= xv
dt 2 dt 2
dq
Since,
constant
dt = 1
; ∴ v ∝
x
4. (d) : Let m be mass of each ball and q be charge on
each ball. Force of repulsion,
q
F = 1 2
4πε
2
0 r
In equilibrium
Tcosq = mg
Tsinq = F
...(i)
...(ii)
Divide (ii) by (i), we get, tanθ
From figure (a),
1 q
r/2
4 0 r
= πε 2
y mg
...(iii)
For figure (b)
1
2
q
1
4πε
2
0 r′
r′
/ 2 4πε
tan θ′ = ⇒
0
=
mg y/
2
F
= =
mg
r
mg
2
q
2
′
1 q
4πε0 r
2
mg
r
...(iv)
Divide (iv) by (iii), we get
2
3
2r′ r 3 r
r
= ⇒ r′ = ⇒ r′ =
r ′
2 2 3
r
2
5. (c) : According to Coulomb’s law, the force of
repulsion between the two positive ions each of charge q,
separated by a distance d is given by
q q
F = 1
2
( )( )
q
or F =
4πε
2
0 d
4πε 0d
2
q 2 = 4pe 0 Fd 2 or q= 2
4πε 0Fd
...(i)
Since, q = ne
where, n = number of electrons missing from each ion,
e = magnitude of charge on electron