class 12th physics 2025 paper leak 10 que leak
1. Gauss's Theorem and Application to an Infinitely Long Charged Wire
Gauss's Theorem: The total electric flux through a closed surface is equal to \frac{1}{\varepsilon_0}times the total charge enclosed.
\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\varepsilon_0}Application to an Infinitely Long Charged Wire
For a wire with charge density \lambda (charge per unit length) at a distance r , using a cylindrical Gaussian surface:
E \cdot (2\pi r L) = \frac{\lambda L}{\varepsilon_0}Solving for E :
E = \frac{\lambda}{2\pi \varepsilon_0 r}📌 The field is radially outward if \lambda > 0 and inward if \lambda < 0 .
2. Potential Energy of a System of Two Point Charges
The electrostatic potential energy of two point charges q_1and q_2separated by distance r :
U = \frac{1}{4\pi \varepsilon_0} \frac{q_1 q_2}{r}✅ If q_1and q_2have the same sign → U > 0 (repulsion).
✅ If q_1and q_2have opposite signs → U < 0 (attractions).
3. Kirchhoff's Laws
(i) Kirchhoff's Current Law (KCL):
At any junction, the total incoming current equals the total outgoing current:
\sum I_{\text{in}} = \sum I_{\text{out}}(ii) Kirchhoff's Voltage Law (KVL):
The algebraic sum of all potential differences in a closed loop is zero:
\sum V = 0🔹 Example: In a circuit with resistors and batteries, the sum of EMFs equals the sum of potential drops.
4. Biot-Savart Law and Magnetic Field at the Center of a Circular Loop
Biot-Savart Law: The magnetic field dB due to a small current element Idl at distance r is:
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For a current-carrying circular loop of radius R , the field at the center is:
B = \frac{\mu_0 I}{2R}📌 The field follows the right-hand thumb rule .
5. Magnetic Field on the Axial Line of a Magnetic Dipole
For a bar magnet or small magnetic dipole , the field at an axial distance from the center:
B = \frac{\mu_0}{4\pi} \frac{2M}{r^3}where M = m \cdot 2l is the magnetic dipole moment.
✅ Direction: Along the axis of the dipole.
✅ Behavior: Decrease with \frac{1}{r^3}.
6. Faraday's Laws of Electromagnetic Induction
(i) First Law:
A changing magnetic flux induces an EMF in a coil.
(ii) Second Law:
The induced EMF is proportional to the rate of change of flux:
\mathcal{E} = -\frac{d\Phi_B}{dt}(🔹 Negative sign indicates Lenz's Law , opposing the cause of induction.)
7. Impedance and Resonance in an LCR Circuit
Impedance (Z):
Total opposition to AC in an LCR circuit:
Z = \sqrt{R^2 + (X_L - X_C)^2}where X_L = \omega L and X_C = \frac{1}{\omega C}.
Resonance Condition:
When X_L = X_C, impedance is minimum and current is maximum:
f_r = \frac{1}{2\pi \sqrt{LC}}8. Displacement Current and Maxwell's Equations
🔹 Displacement Current ( I_d) : Accounts for a changing electric field in capacitors.
I_d = \varepsilon_0 \frac{d\Phi_E}{dt}📌 It completes Ampere's Law , leading to Maxwell's equations .
9. Lens Maker's Formula
For a thin lens with refractive index , radius R_1, R_2:
\frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right)✅ Used for convex and concave lenses.
10. Young's Double-Slit Experiment and Fringe Width
For two slits separated by distance d , wavelength \lambda , and screen distance D :
\text{Fringe width} \quad w = \frac{\lambda D}{d}✅ Bright fringes : Constructive interference.
✅ Dark fringes : Destructive interference.
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