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Gauss' Law & Applications — MH-CET Physics MCQs with Solutions

Free MH-CET Physics Gauss' Law & Applications MCQs with step-by-step solutions (21 questions). Part of Electrostatics. Practise online on Prepizo — no login needed.

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Questions with solutions

Q1 — Gauss' Law & Applications · easy · theory
Gauss' law states that the total electric flux through a closed surface equals:
A. The charge enclosed divided by $\varepsilon_0$  ✓ Correct
B. Zero in all cases
C. The total charge in the universe divided by $\varepsilon_0$
D. The charge enclosed multiplied by $\varepsilon_0$
Solution: $\oint \vec{E}\cdot d\vec{A} = \dfrac{q_{enc}}{\varepsilon_0}$, where only charges inside the surface contribute.
Q2 — Gauss' Law & Applications · medium · theory
The electric flux through a closed surface enclosing a given charge depends on:
A. The shape of the surface
B. Only the magnitude of the enclosed charge  ✓ Correct
C. The position of the charge inside the surface
D. The size of the surface
Solution: Gauss' law makes the flux independent of the geometry, which is what makes it such a powerful shortcut.
Q3 — Gauss' Law & Applications · medium · theory
The electric field due to an infinite plane sheet of surface charge density $\sigma$ is:
A. Zero
B. $\dfrac{\sigma}{2\varepsilon_0 r^2}$
C. $\dfrac{\sigma}{2\varepsilon_0}$, independent of distance  ✓ Correct
D. $\dfrac{\sigma}{\varepsilon_0 r}$
Solution: A Gaussian cylinder gives a uniform field on both sides, which does not weaken with distance from the sheet.
Q4 — Gauss' Law & Applications · easy · theory
The electric field at any point inside a uniformly charged conducting spherical shell is:
A. Zero  ✓ Correct
B. $\dfrac{kQ}{R^2}$
C. Infinite at the centre
D. $\dfrac{kQ}{r^2}$
Solution: A Gaussian surface drawn inside encloses no charge, so the field must vanish everywhere within.
Q5 — Gauss' Law & Applications · medium · theory
The electric field outside a uniformly charged spherical shell of total charge $Q$ at distance $r$ from the centre is:
A. Zero
B. $\dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{r^3}$
C. $\dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{r^2}$  ✓ Correct
D. $\dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{R^2}$
Solution: Outside the shell the field is exactly as though all the charge were concentrated at the centre.
Q6 — Gauss' Law & Applications · medium · theory
The electric field due to an infinitely long straight charged wire of linear charge density $\lambda$ at distance $r$ is proportional to:
A. $r$
B. $\dfrac{1}{r^2}$
C. $\dfrac{1}{r^3}$
D. $\dfrac{1}{r}$  ✓ Correct
Solution: A cylindrical Gaussian surface gives $E = \dfrac{\lambda}{2\pi\varepsilon_0 r}$.
Q7 — Gauss' Law & Applications · easy · theory
The net electric flux through a closed surface that encloses no net charge is:
A. Infinite
B. Always negative
C. Zero  ✓ Correct
D. Always positive
Solution: Whatever flux enters the surface must leave it, so the net flux is zero even if the field inside is not.
Q8 — Gauss' Law & Applications · easy · theory
Electric flux is a:
A. Vector quantity
B. Scalar quantity  ✓ Correct
C. Dimensionless quantity
D. Tensor quantity
Solution: It is defined by the scalar product $\vec{E}\cdot d\vec{A}$, and its unit is $\text{N}\cdot\text{m}^2/\text{C}$.
Q9 — Gauss' Law & Applications · medium · numerical
A charge of $8.85 \times 10^{-12}\text{ C}$ is enclosed by a closed surface. The total flux through it is:
A. $1\text{ N}\cdot\text{m}^2/\text{C}$  ✓ Correct
B. $10^{-12}\text{ N}\cdot\text{m}^2/\text{C}$
C. $8.85\text{ N}\cdot\text{m}^2/\text{C}$
D. Zero
Solution: $\Phi = \dfrac{q}{\varepsilon_0} = \dfrac{8.85 \times 10^{-12}}{8.85 \times 10^{-12}} = 1\text{ N}\cdot\text{m}^2/\text{C}$.
Q10 — Gauss' Law & Applications · hard · numerical
A uniform field $E = 2000\text{ N/C}$ passes through a rectangular surface $10\text{ cm} \times 20\text{ cm}$ whose normal makes $60^\circ$ with the field. The flux is:
A. $10\text{ N}\cdot\text{m}^2/\text{C}$
B. $20\text{ N}\cdot\text{m}^2/\text{C}$  ✓ Correct
C. $34.6\text{ N}\cdot\text{m}^2/\text{C}$
D. $40\text{ N}\cdot\text{m}^2/\text{C}$
Solution: $\Phi = EA\cos\theta = 2000 \times 0.02 \times \cos 60^\circ = 40 \times 0.5 = 20\text{ N}\cdot\text{m}^2/\text{C}$.
Q11 — Gauss' Law & Applications · medium · numerical
A point charge $q$ is placed at the centre of a cube. The flux through one face of the cube is:
A. $\dfrac{q}{24\varepsilon_0}$
B. $\dfrac{q}{\varepsilon_0}$
C. $\dfrac{q}{8\varepsilon_0}$
D. $\dfrac{q}{6\varepsilon_0}$  ✓ Correct
Solution: The total flux $\dfrac{q}{\varepsilon_0}$ is shared equally among the six identical faces.
Q12 — Gauss' Law & Applications · hard · numerical
An infinite sheet carries a surface charge density of $8.85 \times 10^{-12}\text{ C/m}^2$. The field near it is:
A. $8.85\text{ N/C}$
B. $1\text{ N/C}$
C. $0.5\text{ N/C}$  ✓ Correct
D. $2\text{ N/C}$
Solution: $E = \dfrac{\sigma}{2\varepsilon_0} = \dfrac{8.85 \times 10^{-12}}{2 \times 8.85 \times 10^{-12}} = 0.5\text{ N/C}$.
Q13 — Gauss' Law & Applications · hard · numerical
An infinitely long wire has a linear charge density of $10^{-6}\text{ C/m}$. The field at $0.1\text{ m}$ from it is:
A. $9 \times 10^4\text{ N/C}$
B. $9 \times 10^5\text{ N/C}$
C. $1.8 \times 10^5\text{ N/C}$  ✓ Correct
D. $1.8 \times 10^4\text{ N/C}$
Solution: $E = \dfrac{2k\lambda}{r} = \dfrac{2 \times 9 \times 10^9 \times 10^{-6}}{0.1} = 1.8 \times 10^5\text{ N/C}$.
Q14 — Gauss' Law & Applications · hard · numerical
A spherical shell of radius $0.1\text{ m}$ carries a charge of $1\,\mu\text{C}$. The field at a point $0.2\text{ m}$ from its centre is:
A. $9 \times 10^5\text{ N/C}$
B. Zero
C. $2.25 \times 10^5\text{ N/C}$  ✓ Correct
D. $4.5 \times 10^5\text{ N/C}$
Solution: Outside the shell it behaves as a point charge: $E = \dfrac{9 \times 10^9 \times 10^{-6}}{(0.2)^2} = 2.25 \times 10^5\text{ N/C}$.
Q15 — Gauss' Law & Applications · easy · numerical
A spherical shell carries a charge $Q$. The electric field at a point inside the shell is:
A. $\dfrac{kQ}{r^2}$
B. Zero  ✓ Correct
C. Infinite
D. $\dfrac{kQ}{R^2}$
Solution: A Gaussian sphere drawn inside encloses no charge, so by symmetry the field is zero everywhere within.
Q16 — Gauss' Law & Applications · medium · numerical
A closed surface encloses charges of $+2\,\mu\text{C}$ and $-2\,\mu\text{C}$. The total flux through it is:
A. $2.26 \times 10^5\text{ N}\cdot\text{m}^2/\text{C}$
B. $4.52 \times 10^5\text{ N}\cdot\text{m}^2/\text{C}$
C. Zero  ✓ Correct
D. Infinite
Solution: The net enclosed charge is zero, so by Gauss' law the total flux is zero.
Q17 — Gauss' Law & Applications · easy · numerical
A uniform field of $100\text{ N/C}$ passes normally through an area of $2\text{ m}^2$. The flux is:
A. $100\text{ N}\cdot\text{m}^2/\text{C}$
B. Zero
C. $50\text{ N}\cdot\text{m}^2/\text{C}$
D. $200\text{ N}\cdot\text{m}^2/\text{C}$  ✓ Correct
Solution: $\Phi = EA\cos 0^\circ = 100 \times 2 = 200\text{ N}\cdot\text{m}^2/\text{C}$.
Q18 — Gauss' Law & Applications · hard · numerical
The flux through a closed surface is $100\text{ N}\cdot\text{m}^2/\text{C}$. The charge enclosed is:
A. $1.13 \times 10^{10}\text{ C}$
B. $8.85 \times 10^{-10}\text{ C}$  ✓ Correct
C. $100\text{ C}$
D. $8.85 \times 10^{-12}\text{ C}$
Solution: $q = \varepsilon_0\Phi = 8.85 \times 10^{-12} \times 100 = 8.85 \times 10^{-10}\text{ C}$.
Q19 — Gauss' Law & Applications · medium · numerical
A charge is enclosed by a spherical Gaussian surface. If the radius of the sphere is doubled, the flux through it:
A. Doubles
B. Becomes four times
C. Remains unchanged  ✓ Correct
D. Becomes one-fourth
Solution: Gauss' law makes the flux depend only on the enclosed charge, not on the size of the surface.
Q20 — Gauss' Law & Applications · hard · numerical
A spherical shell of radius $0.2\text{ m}$ carries a charge of $4\,\mu\text{C}$. The field just outside its surface is:
A. $1.8 \times 10^6\text{ N/C}$
B. $4.5 \times 10^5\text{ N/C}$
C. Zero
D. $9 \times 10^5\text{ N/C}$  ✓ Correct
Solution: $E = \dfrac{9 \times 10^9 \times 4 \times 10^{-6}}{(0.2)^2} = \dfrac{3.6 \times 10^4}{0.04} = 9 \times 10^5\text{ N/C}$.
Q21 — Gauss' Law & Applications · hard · numerical
A point charge $q$ is placed at one corner of a cube. The flux through one face not containing that corner is:
A. $\dfrac{q}{24\varepsilon_0}$  ✓ Correct
B. $\dfrac{q}{6\varepsilon_0}$
C. $\dfrac{q}{8\varepsilon_0}$
D. $\dfrac{q}{\varepsilon_0}$
Solution: Eight such cubes surround the corner, so this cube receives $\dfrac{q}{8\varepsilon_0}$. That is shared equally by the three faces away from the corner, giving $\dfrac{q}{24\varepsilon_0}$ each.