Current Electricity

NEET Physics · 105 questions · Page 2 of 11 · Click an option or "Show Solution" to reveal answer

Q11
A wire of length 'll' and resistance 100Ω100 \Omega is divided into 10 equal parts. The first 5 parts are connected in series while the next 5 parts are connected in parallel. The two combinations are again connected in series. The resistance of this final combination is:
A 26Ω26 \Omega
B 52Ω52 \Omega
C 55Ω55 \Omega
D 60Ω60 \Omega
Correct Answer
Option B
Solution

To solve this problem, we first need to understand how the resistance changes when we cut the wire into equal parts and how it behaves when connected in different configurations (series and parallel).

Given: Original length of the wire, l l .

Total resistance of the wire R=100Ω R = 100 \Omega .

The wire is divided into 10 equal parts.

Resistance of each part: Since the wire is divided into 10 equal parts, the length of each part is l10\dfrac{l}{10}.

Resistance is proportional to length (as long as the cross-sectional area and material of the wire remain constant).

Therefore, the resistance of each part, denoted as r r , is 110\dfrac{1}{10}th of the total resistance:

r=R10=100Ω10=10Ωr = \frac{R}{10} = \frac{100 \Omega}{10} = 10 \Omega

First 5 parts in series: When resistors are connected in series, the total resistance is the sum of the individual resistances:

Rseries=5×10Ω=50ΩR_{\text{series}} = 5 \times 10 \Omega = 50 \Omega

Next 5 parts in parallel: When resistors are connected in parallel, the total resistance Rparallel R_{\text{parallel}} can be calculated using the reciprocal formula:

1Rparallel=110Ω+110Ω+110Ω+110Ω+110Ω=5×110Ω=510Ω=12Ω\frac{1}{R_{\text{parallel}}} = \frac{1}{10 \Omega} + \frac{1}{10 \Omega} + \frac{1}{10 \Omega} + \frac{1}{10 \Omega} + \frac{1}{10 \Omega} = 5 \times \frac{1}{10 \Omega} = \frac{5}{10 \Omega} = \frac{1}{2 \Omega}

Thus,

Rparallel=2ΩR_{\text{parallel}} = 2 \Omega

Final combination in series: The total resistance of the combination, where the series and parallel groups are again connected in series, will be:

Rtotal=Rseries+Rparallel=50Ω+2Ω=52ΩR_{\text{total}} = R_{\text{series}} + R_{\text{parallel}} = 50 \Omega + 2 \Omega = 52 \Omega

Thus, the correct answer to the resistance of the final combination is: Option B

52Ω52 \Omega
Q12
Two heaters AA and BB have power rating of 1 kW1 \mathrm{~kW} and 2 kW2 \mathrm{~kW}, respectively. Those two are first connected in series and then in parallel to a fixed power source. The ratio of power outputs for these two cases is:
A 1:11: 1
B 2:92: 9
C 1:21: 2
D 2:32: 3
Correct Answer
Option B
Solution

To find the ratio of power outputs when two heaters with different power ratings are connected first in series and then in parallel, we need to understand how the total power output varies based on the type of connection.

Heater Specifications: Power of heater A

(PA)=1kW=1000W(P_A) = 1 \, \text{kW} = 1000 \, \text{W}

Power of heater B

(PB)=2kW=2000W(P_B) = 2 \, \text{kW} = 2000 \, \text{W}

Scenario 1: Series Connection When resistors (or heaters in this case) are connected in series, the total resistance (RseriesR_{\text{series}}) is the sum of the individual resistances (RAR_A and RBR_B).

Using the formula for electrical power:

P=V2RP = \frac{V^2}{R}

, where

PP

is power,

VV

is voltage, and

RR

is resistance, we can express the resistance of each heater as:

RA=V2PAR_A = \frac{V^2}{P_A}
RB=V2PBR_B = \frac{V^2}{P_B}

Substitute the given power values:

RA=V21000R_A = \frac{V^2}{1000}
RB=V22000R_B = \frac{V^2}{2000}

Then the total resistance for the series connection is:

Rseries=RA+RB=V21000+V22000=3V22000R_{\text{series}} = R_A + R_B = \frac{V^2}{1000} + \frac{V^2}{2000} = \frac{3V^2}{2000}

The total power output in series (PseriesP_{\text{series}}) is:

Pseries=V2Rseries=V23V22000=20003WP_{\text{series}} = \frac{V^2}{R_{\text{series}}} = \frac{V^2}{\frac{3V^2}{2000}} = \frac{2000}{3} \text{W}

Scenario 2: Parallel Connection For parallel connections, the total resistance (RparallelR_{\text{parallel}}) is given by:

1Rparallel=1RA+1RB=1V21000+1V22000=32V2\frac{1}{R_{\text{parallel}}} = \frac{1}{R_A} + \frac{1}{R_B} = \frac{1}{\frac{V^2}{1000}} + \frac{1}{\frac{V^2}{2000}} = \frac{3}{2V^2}

Reformulate to find RparallelR_{\text{parallel}}:

Rparallel=2V23R_{\text{parallel}} = \frac{2V^2}{3}

And the total power output in parallel (PparallelP_{\text{parallel}}) is:

Pparallel=V2Rparallel=V22V23=3V22P_{\text{parallel}} = \frac{V^2}{R_{\text{parallel}}} = \frac{V^2}{\frac{2V^2}{3}} = \frac{3V^2}{2}

However, simplifying,

Pparallel=32V2P_{\text{parallel}} = \frac{3}{2} V^2

The ratio of powers is then:

PseriesPparallel=200033V22\frac{P_{\text{series}}}{P_{\text{parallel}}} = \frac{\frac{2000}{3}}{\frac{3V^2}{2}}

Solving and simplifying,

Ratio=200033×V22=2000×23×3×V2=40009V2\text{Ratio} = \frac{\frac{2000}{3}}{\frac{3 \times V^2}{2}} = \frac{2000 \times 2}{3 \times 3 \times V^2} = \frac{4000}{9V^2}

Given that we know one ratio of the actual power values, we simplify further.

For calculating power in simple terms, consider voltage to be normalized (taken out of the fraction):

PseriesPparallel=2000360002=2000×23×6000=400018000=29\frac{P_{\text{series}}}{P_{\text{parallel}}} = \frac{\frac{2000}{3}}{\frac{6000}{2}} = \frac{2000 \times 2}{3 \times 6000} = \frac{4000}{18000} = \frac{2}{9}

Therefore, the ratio of the power outputs when the heaters are connected first in series and then in parallel is 2:9 , which corresponds to Option B .

Q13
A certain wire A\mathrm{A} has resistance 81 Ω81 ~\Omega. The resistance of another wire B\mathrm{B} of same material and equal length but of diameter thrice the diameter of A will be :
A 81 Ω81 ~\Omega
B 9 Ω9 ~\Omega
C 729 Ω729 ~\Omega
D 243 Ω243 ~\Omega
Correct Answer
Option B
Solution
R=ρLA\mathrm{R=\frac{\rho L}{A}}

If diameter becomes thrice then cross section area will become 9 times so

R1A\mathrm{R\propto \frac{1}{A}}

Resistance will become

19\frac{1}{9}

times

R=81Ω9=9Ω\mathrm{R'=\frac{81\Omega}{9}=9\Omega}
Q14
A copper wire of radius 1 mm1 \mathrm{~mm} contains 102210^{22} free electrons per cubic metre. The drift velocity for free electrons when 10 A10 \mathrm{~A} current flows through the wire will be (Given, charge on electron =1.6×1019C=1.6 \times 10^{-19} \mathrm{C} ) :
A 6.25×104πms1\dfrac{6.25 \times 10^4}{\pi} \mathrm{ms}^{-1}
B 6.25π×103 ms1\dfrac{6.25}{\pi} \times 10^3 \mathrm{~ms}^{-1}
C 6.25πms1\dfrac{6.25}{\pi} \mathrm{ms}^{-1}
D 6.25×105πms1\dfrac{6.25 \times 10^5}{\pi} \mathrm{ms}^{-1}
Correct Answer
Option B
Solution
I=neAVdVd=IneA=101022×1.6×1019×π×106 Vd=6.25π×103 m/sec\begin{aligned} & \mathrm{I}=\mathrm{neAV_{d }} \\ & \mathrm{V}_{\mathrm{d}}=\frac{\mathrm{I}}{\mathrm{neA}}=\frac{10}{10^{22} \times 1.6 \times 10^{-19} \times \pi \times 10^{-6}} \\ & \mathrm{~V}_{\mathrm{d}}=\frac{6.25}{\pi} \times 10^3 \mathrm{~m} / \mathrm{sec} \end{aligned}
Q15
The emf of a cell having internal resistance 1Ω1 \Omega is balanced against a length of 330 cm330 \mathrm{~cm} on a potentiometer wire. When an external resistance of 2Ω2 \Omega is connected across the cell, the balancing length will be :
A 220 cm
B 330 cm
C 115 cm
D 332 cm
Correct Answer
Option A
Solution
r=(occ)R1=(330cc)×23c=660c=220 cm\begin{aligned} & \mathrm{r}=\left(\frac{\ell_{\mathrm{o}}-\ell_{\mathrm{c}}}{\ell_{\mathrm{c}}}\right) \mathrm{R} \\ & 1=\left(\frac{330-\ell_{\mathrm{c}}}{\ell_{\mathrm{c}}}\right) \times 2 \\ & 3 \ell_{\mathrm{c}}=660 \\ & \ell_{\mathrm{c}}=220 \mathrm{~cm}\end{aligned}
Q16
The magnitude and direction of the current in the following circuit is :-
A 0.5 A from AA to BB through EE
B 59A\dfrac{5}{9} A from AA to BB through EE
C 1.5 A from BB to AA through EE
D 0.2 A from BB to AA through EE
Correct Answer
Option A
Solution
i=10510=510 A\mathrm{i}=\frac{10-5}{10}=\frac{5}{10} \mathrm{~A}
=0.5 A=0.5 \mathrm{~A}

from

AA

to

BB

through

EE

.

Q17
If the galvanometer GG does not show any deflection in the circuit shown, the value of RR is given by:
A 50 Ω\Omega
B 100 Ω\Omega
C 400 Ω\Omega
D 200 Ω\Omega
Correct Answer
Option B
Solution

For no reading galvanometer. Potential across it is same.

i400Ω102400=8400=150=iR\mathrm{i}_{400 \Omega} \Rightarrow \frac{10-2}{400}=\frac{8}{400}=\frac{1}{50}=\mathrm{i}_{\mathrm{R}}
iRVRR2R=150R=100Ω\mathrm{i}_{\mathrm{R}} \Rightarrow \frac{\mathrm{V}_{\mathrm{R}}}{\mathrm{R}} \Rightarrow \frac{2}{\mathrm{R}}=\frac{1}{50} \Rightarrow \mathrm{R}=100 \Omega
Q18
Resistance of a carbon resistor determined from colour codes is (22000±5%)Ω(22000 \pm 5 \%) \Omega. The colour of third band must be :
A Green
B Orange
C Yellow
D Red
Correct Answer
Option B
Solution
R=[22×103±5%]ΩR=\left[22 \times 10^{3} \pm 5 \%\right] \Omega

Acc. to color code Third Band \to Orange (color code for digit 3 is orange)

Q19
The resistance of platinum wire at 0C0^{\circ} \mathrm{C} is 2 Ω2 ~\Omega and 6.8 Ω6.8 ~\Omega at 80C80^{\circ} \mathrm{C}. The temperature coefficient of resistance of the wire is :
A 3×103C13 \times 10^{-3} \mathrm{C}^{-1}
B 3×102C13 \times 10^{-2} \mathrm{C}^{-1}
C 3×1010C13 \times 10^{-10} \mathrm{C}^{-1}
D 3×104C13 \times 10^{-4} \mathrm{C}^{-1}
Correct Answer
Option B
Solution
RT=R0[1+α(TT0)]\mathrm{R}_{\mathrm{T}}=\mathrm{R}_{0}\left[1+\alpha\left(\mathrm{T}-\mathrm{T}_{0}\right)\right]
6.8=2[1+α(80α)]6.8=2[1+\alpha(80-\alpha)]
α=2.480=0.03/C=3×102/C\alpha=\frac{2.4}{80}=0.03 /{ }^{\circ} \mathrm{C}=3 \times 10^{-2} /{ }^{\circ} \mathrm{C}
Q20
10 resistors, each of resistance R\mathrm{R} are connected in series to a battery of emf EE and negligible internal resistance. Then those are connected in parallel to the same battery, the current is increased nn times. The value of nn is :
A 100
B 1
C 1000
D 10
Correct Answer
Option A
Solution
IS=E10R\mathrm{I}_{\mathrm{S}}=\frac{E}{10 R}

..... (1)

IP=ER/10=10ER\mathrm{I}_{\mathrm{P}}=\frac{\mathrm{E}}{\mathrm{R} / 10}=\frac{10 \mathrm{E}}{\mathrm{R}}

.... (2)

n=IPIS=100n=100\mathrm{n}=\frac{\mathrm{I}_{\mathrm{P}}}{\mathrm{I}_{\mathrm{S}}}=100 \Rightarrow \mathrm{n}=100
Ready for a full NEET mock test? Timed · full syllabus · instant results
Take a Mock Test →