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Current Electricity — NEET Physics MCQs with Solutions

Free NEET Physics Current Electricity MCQs with step-by-step solutions covering Conductors, Combination of Resistors, Kirchhoff's Laws, Instruments. Practise online on Prepizo — no login needed.

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Sample questions with solutions

Q1 — Conductors · easy · numerical
Current of 4.8 amperes is flowing through a conductor. The number of electrons per second will be
A. $3 \times 10^{19}$  ✓ Correct
B. $3 \times 10^{20}$
C. $7.68 \times 10^{21}$
D. $7.68 \times 10^{20}$
Solution: Number of electrons per second $n = i/e = 4.8 / (1.6 \times 10^{-19}) = 3 \times 10^{19}$.
Q2 — Conductors · easy · numerical
Every atom makes one free electron in copper. If 1.1 ampere current is flowing in the wire of copper having 1 mm diameter, then the drift velocity (approx.) will be (Density of copper $= 9 \times 10^{3}\ kg\ m^{-3}$ and atomic weight = 63)
A. $0.2\ mm/sec$
B. $0.3\ mm/sec$
C. $0.2\ cm/sec$
D. $0.1\ mm/sec$  ✓ Correct
Solution: Electron density $n = (6 \times 10^{23} / 63 \times 10^{-3}) \times 9 \times 10^{3} = 8.5 \times 10^{28}\ m^{-3}$. With $A = \pi (0.5 \times 10^{-3})^2$, drift velocity $v_d = i/(neA) = 1.1/(8.5 \times 10^{28} \times 1.6 \times 10^{-19} \times 7.85 \times 10^{-7}) \approx 0.1\ mm/s$.
Q3 — Conductors · easy · theory
Which one is not the correct statement
A. $1\ volt \times 1\ coulomb = 1\ joule$
B. $1\ volt \times 1\ ampere = 1\ joule/second$
C. $1\ volt \times 1\ watt = 1\ H.P.$  ✓ Correct
D. Watt-hour can be expressed in eV
Solution: Volt $\times$ watt is not a unit of power at all, so it cannot equal 1 H.P. The other three relations are dimensionally correct.
Q4 — Conductors · easy · numerical
The temperature coefficient of resistance for a wire is $0.00125\ /^{\circ}C$. At 300 K its resistance is 1 ohm. The temperature at which the resistance becomes 2 ohm is
A. $1154\ K$
B. $1400\ K$
C. $1127\ K$  ✓ Correct
D. $1100\ K$
Solution: Using $R_1/R_2 = (1 + \alpha t_1)/(1 + \alpha t_2)$ with $t_1 = 27^{\circ}C$: $1/2 = (1 + 0.00125 \times 27)/(1 + 0.00125\,t_2)$, giving $t_2 = 854^{\circ}C = 1127\ K$.
Q5 — Conductors · easy · theory
Ohm's law is true
A. For diode when current flows
B. For metallic conductors at low temperature  ✓ Correct
C. For electrolytes when current passes through them
D. For metallic conductors at high temperature
Solution: At high temperature the resistance of a metal changes appreciably and the V–i graph becomes non-linear; electrolytes and diodes are non-ohmic. So Ohm's law holds for metallic conductors at low temperature.
Q6 — Conductors · easy · theory
The example for non-ohmic resistance is
A. Tungston wire
B. Copper wire
C. Diode  ✓ Correct
D. Carbon resistance
Solution: A diode has a non-linear V–i characteristic, so it is a non-ohmic resistance.
Q7 — Conductors · easy · theory
Drift velocity $v_d$ varies with the intensity of electric field as per the relation
A. $v_d \propto \dfrac{1}{E}$
B. $v_d \propto E$  ✓ Correct
C. $v_d = $ constant
D. $v_d \propto E^{2}$
Solution: From $v_d = (e\tau/m)E$, the drift velocity is directly proportional to the electric field, i.e. $v_d \propto E$.
Q8 — Conductors · easy · theory
On increasing the temperature of a conductor, its resistance increases because
A. Electron density decreases
B. Mass of the electrons increases
C. None of the above
D. Relaxation time decreases  ✓ Correct
Solution: Resistance $R = ml/(ne^{2}\tau A)$. Heating increases the vibration of lattice ions, so the relaxation time $\tau$ decreases and $R$ increases.
Q9 — Conductors · easy · numerical
In a conductor 4 coulombs of charge flows for 2 seconds. The value of electric current will be
A. 2 volts
B. 2 amperes  ✓ Correct
C. 4 amperes
D. 4 volts
Solution: Current $i = q/t = 4/2 = 2\ A$.
Q10 — Conductors · easy · numerical
The specific resistance of a wire is $\rho$, its volume is $3\ m^{3}$ and its resistance is 3 ohms, then its length will be
A. $\rho\sqrt{\dfrac{1}{3}}$
B. $\dfrac{1}{\rho}\sqrt{3}$
C. $\dfrac{3}{\sqrt{\rho}}$  ✓ Correct
D. $\sqrt{\dfrac{1}{\rho}}$
Solution: Volume $V = lA = 3$, so $A = 3/l$. Then $R = \rho l/A = \rho l^{2}/3 = 3$, giving $l^{2} = 9/\rho$ and $l = 3/\sqrt{\rho}$.
Q11 — Conductors · easy · numerical
$62.5 \times 10^{18}$ electrons per second are flowing through a wire of area of cross-section $0.1\ m^{2}$, the value of current flowing will be
A. 10 A  ✓ Correct
B. 1 A
C. 0.11 A
D. 0.1 A
Solution: $i = ne = 62.5 \times 10^{18} \times 1.6 \times 10^{-19} = 10\ A$. The area is not needed.
Q12 — Conductors · easy · theory
A certain wire has a resistance $R$. The resistance of another wire identical with the first except having twice its diameter is
A. $2\,R$
B. $0.25\,R$  ✓ Correct
C. $0.5\,R$
D. $4\,R$
Solution: $R \propto 1/d^{2}$. Doubling the diameter makes the area four times larger, so the resistance becomes $R/4 = 0.25R$.
Q13 — Conductors · easy · numerical
In hydrogen atom, the electron makes $6.6 \times 10^{15}$ revolutions per second around the nucleus in an orbit of radius $0.5 \times 10^{-10}\ m$. It is equivalent to a current nearly
A. $1\ A$
B. $1\ mA$  ✓ Correct
C. $1\ \mu A$
D. $1.6 \times 10^{-19}\ A$
Solution: $i = e \times f = 1.6 \times 10^{-19} \times 6.6 \times 10^{15} \approx 1.06 \times 10^{-3}\ A \approx 1\ mA$.
Q14 — Conductors · easy · numerical
A wire of length 5 m and radius 1 mm has a resistance of 1 ohm. What length of the wire of the same material at the same temperature and of radius 2 mm will also have a resistance of 1 ohm
A. $1.25\ m$
B. $2.5\ m$
C. $10\ m$
D. $20\ m$  ✓ Correct
Solution: $R \propto l/r^{2}$. For $R$ to stay the same when $r$ doubles (area $\times 4$), the length must also become four times: $l = 4 \times 5 = 20\ m$.
Q15 — Conductors · easy · theory
When there is an electric current through a conducting wire along its length, then an electric field must exist
A. Inside the wire but parallel to it  ✓ Correct
B. Outside the wire but parallel to it
C. Outside the wire but normal to it
D. Inside the wire but normal to it
Solution: The current is driven by the field inside the conductor, and it is directed along the length of the wire, i.e. inside the wire and parallel to it.
Q16 — Conductors · easy · theory
Through a semiconductor, an electric current is due to drift of
A. Free electrons
B. Positive and negative ions
C. Free electrons and holes  ✓ Correct
D. Protons
Solution: In a semiconductor both electrons (in the conduction band) and holes (in the valence band) act as charge carriers.
Q17 — Conductors · easy · numerical
In an electrolyte $3.2 \times 10^{18}$ bivalent positive ions drift to the right per second while $3.6 \times 10^{18}$ monovalent negative ions drift to the left per second. Then the current is
A. 1.6 amp to the left
B. 0.45 amp to the left
C. 0.45 amp to the right
D. 1.6 amp to the right  ✓ Correct
Solution: Positive ions moving right give $3.2 \times 10^{18} \times 2e = 1.024\ A$ to the right; negative ions moving left also give a current $3.6 \times 10^{18} \times e = 0.576\ A$ to the right. Total $= 1.6\ A$ to the right.
Q18 — Conductors · easy · theory
A metallic block has no potential difference applied across it, then the mean velocity of free electrons is ($T$ = absolute temperature of the block)
A. Finite but independent of temperature
B. Zero
C. Proportional to $T$
D. Proportional to $\sqrt{T}$  ✓ Correct
Solution: With no external field the electrons have only random thermal motion, for which $\tfrac{1}{2}mv_{rms}^{2} = \tfrac{3}{2}kT$, so the speed is proportional to $\sqrt{T}$.
Q19 — Conductors · easy · theory
The specific resistance of all metals is most affected by
A. Pressure
B. Applied magnetic field
C. Temperature  ✓ Correct
D. Degree of illumination
Solution: The specific resistance (resistivity) of a metal rises appreciably with temperature; the other factors have a negligible effect.
Q20 — Conductors · easy · theory
The positive temperature coefficient of resistance is for
A. Germanium
B. Copper  ✓ Correct
C. Carbon
D. An electrolyte
Solution: Metals such as copper have a positive temperature coefficient of resistance; carbon, semiconductors and electrolytes have negative coefficients.
Q21 — Conductors · easy · theory
The fact that the conductance of some metals rises to infinity at some temperature below a few Kelvin is called
A. Superconductivity  ✓ Correct
B. Thermal conductivity
C. Magnetic conductivity
D. Optical conductivity
Solution: Below a critical temperature the resistance drops to zero (conductance becomes infinite); this phenomenon is superconductivity.
Q22 — Conductors · easy · numerical
Dimensions of a block are $1\ cm \times 1\ cm \times 100\ cm$. If specific resistance of its material is $3 \times 10^{-7}\ ohm-m$, then the resistance between the opposite rectangular faces is
A. $3 \times 10^{-9}\ ohm$
B. $3 \times 10^{-3}\ ohm$
C. $3 \times 10^{-7}\ ohm$  ✓ Correct
D. $3 \times 10^{-5}\ ohm$
Solution: For the opposite rectangular faces, $l = 1\ cm = 10^{-2}\ m$ and $A = 1\ cm \times 100\ cm = 10^{-2}\ m^{2}$. So $R = \rho l/A = 3 \times 10^{-7} \times 10^{-2}/10^{-2} = 3 \times 10^{-7}\ \Omega$.
Q23 — Conductors · easy · numerical
There is a current of 20 amperes in a copper wire of $10^{-6}$ square metre area of cross-section. If the number of free electrons per cubic metre is $10^{29}$, then the drift velocity is
A. $1.25 \times 10^{-3}\ m/sec$  ✓ Correct
B. $125 \times 10^{-3}\ m/sec$
C. $12.5 \times 10^{-3}\ m/sec$
D. $1.25 \times 10^{-4}\ m/sec$
Solution: $v_d = i/(neA) = 20/(10^{29} \times 1.6 \times 10^{-19} \times 10^{-6}) = 1.25 \times 10^{-3}\ m/s$.
Q24 — Conductors · easy · theory
The electric intensity $E$, current density $j$ and specific resistance $k$ are related to each other by the relation
A. $E = jk$  ✓ Correct
B. $k = jE$
C. $E = j/k$
D. $E = k/j$
Solution: From $j = \sigma E$ and $\sigma = 1/k$, we get $E = jk$.
Q25 — Conductors · easy · theory
The resistance of a wire of uniform diameter $d$ and length $L$ is $R$. The resistance of another wire of the same material but diameter $2d$ and length $4L$ will be
A. $R/4$
B. $2R$
C. $R$  ✓ Correct
D. $R/2$
Solution: $R \propto l/d^{2}$. Here the length is 4 times and $d^{2}$ is also 4 times, so the resistance is unchanged: $R$.
Q26 — Conductors · easy · numerical
There is a current of 1.344 amp in a copper wire whose area of cross-section normal to the length of the wire is $1\ mm^{2}$. If the number of free electrons per $cm^{3}$ is $8.4 \times 10^{22}$, then the drift velocity would be
A. $1.0\ mm/sec$
B. $1.0\ m/sec$
C. $0.01\ mm/sec$
D. $0.1\ mm/sec$  ✓ Correct
Solution: Here $n = 8.4 \times 10^{22}\ cm^{-3} = 8.4 \times 10^{28}\ m^{-3}$ and $A = 10^{-6}\ m^{2}$, so $v_d = i/(neA) = 1.344/(8.4 \times 10^{28} \times 1.6 \times 10^{-19} \times 10^{-6}) = 10^{-4}\ m/s = 0.1\ mm/s$.
Q27 — Conductors · easy · theory
It is easier to start a car engine on a hot day than on a cold day. This is because the internal resistance of the car battery
A. Decreases with a fall in temperature
B. Increases with rise in temperature
C. Does not change with a change in temperature
D. Decreases with rise in temperature  ✓ Correct
Solution: The battery is an electrolytic cell, and the resistance of an electrolyte falls as the temperature rises, so more current is available on a hot day.
Q28 — Conductors · easy · numerical
5 amperes of current is passed through a metallic conductor. The charge flowing in one minute in coulombs will be
A. 5
B. 1/12
C. 300  ✓ Correct
D. 12
Solution: $q = it = 5 \times 60 = 300\ C$.
Q29 — Conductors · easy · theory
Two wires of the same material are given. The first wire is twice as long as the second and has twice the diameter of the second. The resistance of the first will be
A. Equal to the second
B. Four times of the second
C. Twice of the second
D. Half of the second  ✓ Correct
Solution: $R \propto l/d^{2}$. With $l$ doubled and $d^{2}$ four times, $R_1/R_2 = 2/4 = 1/2$, so the first has half the resistance.
Q30 — Conductors · easy · theory
An electric wire is connected across a cell of e.m.f. $E$. The current $I$ is measured by an ammeter of resistance $R$. According to ohm's law
A. $E = I/R$
B. $E = I^{2}R$
C. $E = IR$  ✓ Correct
D. $E = R/I$
Solution: Ohm's law states that the potential difference equals current times resistance, i.e. $E = IR$.