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An electric dipole of mass m, charge q, and length l is placed in a uniform electric field vecmathrmE = mathrmE_0hatmathrmi . When the dipole is rotated slightly from its equilibrium position and released, the time period of its oscillations will be: [cite: 1, 5]

Solution & Explanation

### Related Formula tau = -pE sin theta I = 2 m left(fracl2right)^2 = fracml^22 ### Core Logic Restoring torque for small angle theta is given by: tau = -q l E_0 theta Equating with rotational inertia dynamics: I omega^2 theta = q l E_0 theta fracm l^22 omega^2 = q l E_0 implies omega^2 = frac2 q E_0m l [cite: 618, 620] ### Step 1: Compute Time Period T = frac2piomega = 2pi sqrtfracml2qE_0 ### Pattern Recognition For a two-particle system pivoting about midpoint, total moment of inertia drops to ml^2/2, scaling the period by a factor of sqrt2[cite: 618, 622]. ### Chapter Mix Class 12 Physics: Electrostatics

Reference Study Guides

More Electrostatics Previous-Year Questions — Page 6

Q21 2025 Gauss's Law and Electric Flux
A square loop of sides a = 1 m is held normally in front of a point charge q = 1C The flux of the electric field through the shaded region is frac5p times frac1varepsilon_0 fracNm^2C , where the value of p is .
Gauss's Law and Electric Flux diagram for Q21 - JEE Main 2025 Morning
The diagram illustrates a square loop divided into 8 symmetric parts with a point charge positioned in front of its center.
Numerical Answer. Answer: 48 to 48

Solution

### Related Formula By Gauss's Law, the total flux emitted by a point charge q through a completely enclosing symmetric cube container surface is: Phitexttotal = fracqepsilon0 ### Core Logic Assuming the charge resides at a symmetric center distance fraca2 relative to the loop face [cite: 784, 786], this square loop represents one of the six identical faces of an enclosing cube system. Thus, the flux passing through the entire square loop face is[cite: 775, 776]: Phitextsquare = frac16 Phitexttotal = fracq6epsilon0 ### Step 1: Symmetric Partitioning As shown in the solution schematic
Gauss's Law and Electric Flux diagram for Q21 - JEE Main 2025 Morning
The diagram illustrates a square loop divided into 8 symmetric parts with a point charge positioned in front of its center.
, the square face can be divided into 8 identical symmetric right-angled triangle sections by drawing its diagonals and medians[cite: 771, 777]. Each individual part intercepts an equal portion of the flux field : Phitextpart = frac18 Phitextsquare = frac18 left(fracq6epsilon_0 ight) = fracq48epsilon_0 The shaded region covers exactly 5 of these individual triangle parts [cite: 779, 780]: Phi_textshaded = 5 times Phi_textpart = frac548 times fracqepsilon_0 Comparing this result with the given expression frac5p times frac1epsilon_0 , we find: p = 48 ### Pattern Recognition Exploit geometric symmetry to break solid angles down into equal fractions, avoiding complex surface integration. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electrostatics
Q2 2025 Energy Density in Capacitors
A parallel plate capacitor of capacitance 1mu mathrmF is charged to a potential difference of 20mathrmV. The distance between plates is 1mu mathrmm. The energy density between plates of capacitor is:
  • A. 1.8 times 10^3 \, mathrmJ/m^3
  • B. 2 times 10^-4 \, mathrmJ/m^3
  • C. 2 times 10^2 mathrm~J / mathrmm^3
  • D. 1.8 times 10^5 mathrm~J / mathrmm^3

Solution

### Related Formula The electric field E between the plates of a parallel plate capacitor is given by : E = fracVd The electrostatic energy density U in a medium is given by: U = frac12 epsilon_0 E^2 ### Core Logic Given values [cite: 662, 664, 665]: * Capacitance, C = 1 \ mutextF * Potential difference, V = 20 text V * Plate separation, d = 1 \ mutextm = 10^-6 text m First, calculate the electric field E : E = frac2010^-6 = 20 times 10^6 text V/m Now, calculate the energy density U using epsilon_0 approx 8.85 times 10^-12 text F/m : U = frac12 times (8.85 times 10^-12) times (20 times 10^6)^2 U = frac12 times 8.85 times 10^-12 times 400 times 10^12 U = 8.85 times 200 = 1770 text J/m^3 = 1.77 times 10^3 text J/m^3 Rounding to the nearest matching option gives 1.8 times 10^3 text J/m^3. ### Pattern Recognition Notice that energy density is completely independent of the total capacitance value C if the voltage and spacing are directly provided. Always check for redundant parameters included to distract candidates. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electrostatics
Q22 2025 Electric Dipole
An electric dipole of dipole moment 6 times 10^-6 mathrmCm is placed in uniform electric field of magnitude 10^6 mathrm~V/m. Initially, the dipole moment is \parallel to electric field. The work that needs to be done on the dipole to make its dipole moment opposite to the field, will be ______ J.
Numerical Answer. Answer: 12

Solution

### Related Formula The potential energy of an electric dipole aligned at an \angle theta inside a uniform electric field is given by: U = -p E cos theta The work done by an external agent to rotate the dipole equals its change in potential energy: W = Delta U = -pE (cos theta_f - cos theta_i) ### Core Logic Given parameters [cite: 805, 806]: * Dipole moment, p = 6 times 10^-6 text Cm * Electric field, E = 10^6 text V/m * Initial \angle (\parallel state), theta_i = 0^circ * Final \angle (opposite state), theta_f = 180^circ Substitute the values into the work equation [cite: 807, 808]: W = -pE (cos 180^circ - cos 0^circ) W = -pE (-1 - 1) = 2 p E quad text W = 2 times (6 times 10^-6) times 10^6 = 12 text J quad text ### Pattern Recognition Rotating a dipole from its most stable configuration (\parallel, theta=0^circ) to its most unstable position (anti-\parallel, theta=180^circ) always requires a maximum work value of exactly 2pE. ### Evaluation Rubric / Model Answer null ### Chapter Mix Class 12 Physics: Electrostatics
Q18 2025 Gauss\'s Law
Match List-I with List-II.
List-IList-II
(A) Electric field inside (distance r > 0 from center) of a uniformly charged spherical shell with surface charge density σ, and radius R.(I) sigma / epsilon_0
(B) Electric field at distance r > 0 from a uniformly charged infinite plane sheet with surface charge density σ.(II) sigma / 2epsilon_0
(C) Electric field outside (distance r > 0 from center) of a uniformly charged spherical shell with surface charge density σ, and radius R(III) 0
(D) Electric field between 2 oppositely charged infinite plane parallel sheets with uniform surface charge density σ.(IV) sigma R^2 / epsilon_0 r^2
Choose the correct answer from the options given below: [cite: 1, 2]
  • A. (A)-(IV), (B)-(I), (C)-(III), (D)-(II)
  • B. (A)-(IV), (B)-(II), (C)-(III), (D)-(I)
  • C. (A)-(II), (B)-(I), (C)-(IV), (D)-(III)
  • D. (A)-(III), (B)-(II), (C)-(IV), (D)-(I)

Solution

### Core Logic Mapping electrostatics equations via Gauss\'s law applications : * (A) Inside a shell, enclosed charge is zero implies E = 0 (III) . * (B) Near an infinite sheet, E = fracsigma2epsilon_0 (II) . * (C) Outside a shell, E = frackQr^2 = fracsigma R^2epsilon_0 r^2 (IV) . * (D) Between opposite sheets, fields add up: fracsigma2epsilon_0 + fracsigma2epsilon_0 = fracsigmaepsilon_0 (I) . Hence, the proper combination sequence is (A)-(III), (B)-(II), (C)-(IV), (D)-(I). ### Chapter Mix Class 12 Physics: Electrostatics

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