Current Electricity

JEE Physics · 159 questions · Page 7 of 16 · Click an option or "Show Solution" to reveal answer

Q61
In a building there are 15 bulbs of 45 W, 15 bulbs of 100 W, 15 small fans of 10 W and 2 heaters of 1 kW. The voltage of electric main is 220 V. The minimum fuse capacity (rated value) of the building will be :
A 15 A
B 20 A
C 25 A
D 10 A
Correct Answer
Option B
Solution

Total power is = (15 × 45) + (15 × 100) + (15 × 10) + (2 × 1000) = 4325 W \therefore Current =

4325220{{4325} \over {220}}

= 19.66 A

\simeq

20 A

Q62
A galvanometer having a coil resistance 100 Ω\Omega gives a full scale deflection when a current of 1 mA is passed through it. What is the value of the resistance which can convert this galvanometer into a voltmeter giving full scale deflection for a potential difference of 10 V?
A 8.9 kΩ\Omega
B 10 kΩ\Omega
C 9.9 kΩ\Omega
D 7.9 kΩ\Omega
Correct Answer
Option C
Solution

ig = 1 mA , Rg = 100

Ω\Omega

V = ig(R + Rg) \Rightarrow10 = 1 × 10–3 (R + 100) \RightarrowR = 9.9 k

Ω\Omega
Q63
A current through a wire depends on time as i = α\alpha0t + β\betat2 where α\alpha0 = 20 A/s and β\beta = 8 As-2. Find the charge crossed through a section of the wire in 15 s.
A 2250 C
B 2100 C
C 260 C
D 11250 C
Correct Answer
Option D
Solution

Given,

i=α0t+βt2i = {\alpha _0}t + \beta {t^2}

where, α\alpha0 = 20 A/s, β\beta = 8 A/s2 We know that,

i=dqdti = {{dq} \over {dt}}
dqdt=i=α0t+βt2=20t+8t2\Rightarrow {{dq} \over {dt}} = i = {\alpha _0}t + \beta {t^2} = 20t + 8{t^2}
dq=(20t+8t2)dt\Rightarrow dq = (20t + 8{t^2})dt

On integrating both sides, we get

0qdq=015(2t+8t2)dt\int\limits_0^q {dq = \int\limits_0^{15} {(2t + 8{t^2})dt} }
q=[20t22+8t33]015=10×(15)2+83×(15)3q = \left[ {{{20{t^2}} \over 2} + {{8{t^3}} \over 3}} \right]_0^{15} = 10 \times {(15)^2} + {8 \over 3} \times {(15)^3}

\therefore q = 11250 C

Q64
A wire of 1Ω\Omega has a length of 1 m. It is stretched till its length increases by 25%. The percentage change in resistance to the nearest integer is :
A 76%
B 12.5%
C 25%
D 56%
Correct Answer
Option D
Solution

R0 = 1

Ω\Omega

R1 = ? l0 = 1m l1 = 1.25 m A0 = A As volume of wire remains constant so A0l0 = A1l1 \Rightarrow A1 =

l0A0l1{{{l_0}{A_0}} \over {{l_1}}}

Now Resistance (R) =

plA{{pl} \over A}
R0R1=l0A0(l0A0l1×l1){{{R_0}} \over {{R_1}}} = {{{l_0}} \over {{A_0}}}\left( {{{{l_0}{A_0}} \over {{l_1} \times {l_1}}}} \right)

\Rightarrow

R1=l12l02=1.5625Ω{R_1} = {{l_1^2} \over {l_0^2}} = 1.5625 \,\Omega

So % change in resistance

=R1R0R0×100%= {{{R_1} - {R_0}} \over {{R_0}}} \times 100\%
=1.562511×100%= {{1.5625 - 1} \over 1} \times 100\%
=56.25%= 56.25\%
Q65
A conducting wire of length 'l', area of cross-section A and electric resistivity ρ\rho is connected between the terminals of a battery. A potential difference V is developed between its ends, causing an electric current. If the length of the wire of the same material is doubled and the area of cross-section is halved, the resultant current would be :
A 4VAρl4{{VA} \over {\rho l}}
B 34VAρl{3 \over 4}{{VA} \over {\rho l}}
C 14VAρl{1 \over 4}{{VA} \over {\rho l}}
D 14ρlVA{1 \over 4}{{\rho l} \over {VA}}
Correct Answer
Option C
Solution

We know that

R=ρlAR = \rho {l \over A}

Now, new length :

l=2ll' = 2l

new area of cross section :

A=A/2A' = A/2

\therefore New resistance :

R=ρ.2lA/2R' = \rho .{{2l} \over {A/2}}
R=4ρlA\Rightarrow R' = 4{{\rho l} \over A}
R=4R\Rightarrow R' = 4R

\therefore Resultant current :

I=V4RI = {V \over {4R}}

\Rightarrow

I=14VAρlI = {1 \over 4}{{VA} \over {\rho l}}
Q66
In the experiment of Ohm's law, a potential difference of 5.0 V is applied across the end of a conductor of length 10.0 cm and diameter of 5.00 mm. The measured current in the conductor is 2.00 A. The maximum permissible percentage error in the resistivity of the conductor is :
A 3.9
B 8.4
C 7.5
D 3.0
Correct Answer
Option A
Solution
V=I×ρlAV = I \times \rho {l \over A}
ρ=VAIl=π4Vd2Il\Rightarrow \rho = {{VA} \over {Il}} = {\pi \over 4}{{V{d^2}} \over {Il}}
Δρρ=2Δdd+ΔVV+ΔII+Δll{{\Delta \rho } \over \rho } = {{2\Delta d} \over d} + {{\Delta V} \over V} + {{\Delta I} \over I} + {{\Delta l} \over l}
=2(0.015)+0.15+0.012+0.110= 2\left( {{{0.01} \over 5}} \right) + {{0.1} \over 5} + {{0.01} \over 2} + {{0.1} \over {10}}

\Rightarrow

Δρρ=0.039=3.9%{{\Delta \rho } \over \rho } = 0.039 = 3.9\%
Q67
The combination of two identical cells, whether connected in series or parallel combination provides the same current through an external resistance of 2Ω\Omega. The value of internal resistance of each cell is
A 2Ω\Omega
B 4Ω\Omega
C 6Ω\Omega
D 8Ω\Omega
Correct Answer
Option A
Solution

From diagram

ip=E2+r2{i_p} = {E \over {2 + {r \over 2}}}

and

is=2E2+2r{i_s} = {{2E} \over {2 + 2r}}

given

ip=is{i_p} = {i_s}
12+r2=11+r{1 \over {2 + {r \over 2}}} = {1 \over {1 + r}}
1+r=2+r21 + r = 2 + {r \over 2}
r=2Ωr = 2\,\Omega
Q68
A current of 5 A is passing through a non-linear magnesium wire of cross-section 0.04 m2. At every point the direction of current density is at an angle of 60^\circ with the unit vector of area of cross-section. The magnitude of electric field at every point of the conductor is : (Resistivity of magnesium ρ\rho = 44 ×\times 10-8 Ω\Omegam)
A 11 ×\times 10-5 V/m
B 11 ×\times 10-3 V/m
C 11 ×\times 10-7 V/m
D 11 ×\times 10-2 V/m
Correct Answer
Option A
Solution

Given, current, I = 5A Area of cross-section of wire, A = 0.04 m2 We know that,

J=IAJ = {I \over A}
I=JA\Rightarrow I = JA

or

I=J.AI = J\,.\,A

or

I=JAcosθI = JA\cos \theta

where, J = current density.

5=J(4100)×cos(60)\Rightarrow 5 = J\left( {{4 \over {100}}} \right) \times \cos (60^\circ )

[\because Given, θ\theta = 60

^\circ

]

J=500×12J = 500 \times {1 \over 2}

[\because cos60

^\circ

=

12{1 \over 2}

] \Rightarrow J = 250 Am-2 The relation between electric field, current density and resistivity can be given as, E = ρ\rho .

J = 44 ×\times 10-8 ×\times 250 [\because Resistivity, ρ\rho = 44 ×\times 10-8

Ω\Omega

-m] = 11 ×\times 10-5 V/m

Q69
The resistance of a conductor at 15^\circC is 16Ω\Omega and at 100^\circC is 20Ω\Omega. What will be the temperature coefficient of resistance of the conductor?
A 0.010^\circC-1
B 0.033^\circC-1
C 0.003^\circC-1
D 0.042^\circC-1
Correct Answer
Option C
Solution

16 = R0 [1 + α\alpha (15 - T0)] 20 = R0 [1 + α\alpha (100 - T0)] Assuming T0 = 0

^\circ

C, as a general convention. \Rightarrow

1620=1+α×151+α×100{{16} \over {20}} = {{1 + \alpha \times 15} \over {1 + \alpha \times 100}}

\Rightarrow α\alpha = 0.003

^\circ

C-1

Q70
What equal length of an iron wire and a copper-nickel alloy wire, each of 2 mm diameter connected parallel to give an equivalent resistance of 3Ω\Omega ? (Given resistivities of iron and copper-nickel alloy wire are 12 μ\muΩ\Omega and 51 μ\muΩ\Omega cm respectively)
A 82 m
B 97 m
C 110 m
D 90 m
Correct Answer
Option B
Solution
R1R2R1+R2=3{{{R_1}{R_2}} \over {{R_1} + {R_2}}} = 3
(12×106×102)π(2)2×106×(51×106×102)l×4π(2)2×10663×106×102×l×4π(2)2×106{{{{(12 \times {{10}^{ - 6}} \times {{10}^{ - 2}})} \over {\pi {{(2)}^2} \times {{10}^{ - 6}}}} \times {{(51 \times {{10}^{ - 6}} \times {{10}^{ - 2}})l \times 4} \over {\pi {{(2)}^2} \times {{10}^{ - 6}}}}} \over {{{63 \times {{10}^{ - 6}} \times {{10}^{ - 2}} \times l \times 4} \over {\pi {{(2)}^2} \times {{10}^{ - 6}}}}}}

= 3 \Rightarrow l = 97 m

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