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 1 ε 0 \frac{1}{\varepsilon_0}times the total charge enclosed.

E d A = Q enc ε 0 ​​\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 λ \lambda (charge per unit length) at a distance r r , using a cylindrical Gaussian surface:

E ( 2 π r L ) = λ L ε 0 E \cdot (2\pi r L) = \frac{\lambda L}{\varepsilon_0}

Solving for E E :

E = λ 2 π ε 0 r E = \frac{\lambda}{2\pi \varepsilon_0 r}

📌 The field is radially outward if λ > 0 \lambda > 0 and inward if λ < 0 \lambda < 0 .


2. Potential Energy of a System of Two Point Charges

The electrostatic potential energy of two point charges q 1 q_1and q 2 q_2separated by distance r r :

U = 1 4 π ε 0 q 1 q 2 r U = \frac{1}{4\pi \varepsilon_0} \frac{q_1 q_2}{r}

✅ If q 1 q_1and q 2 q_2have the same sign → U > 0 U > 0 (repulsion).
✅ If q 1 q_1and q 2 q_2have opposite signs → U < 0 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:

I in = I out \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:

V = 0 \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 d B dB due to a small current element I d l Idl at distance r r is:

d B

style="vertical-align: inherit;">= μ 0 4 π I d l sin θ r 2 dB = \frac{\mu_0}{4\pi} \frac{I \, dl \sin\theta}{r^2}

For a current-carrying circular loop of radius R R , the field at the center is:

B = μ 0 I 2 R 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 r from the center:

B = μ 0 4 π 2 M r 3 B = \frac{\mu_0}{4\pi} \frac{2M}{r^3}

where M = m 2 l M = m \cdot 2l is the magnetic dipole moment.

Direction: Along the axis of the dipole.
Behavior: Decrease with 1 r 3 \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:

E = d Φ B d t \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 = R 2 + ( X LX C ) 2 Z = \sqrt{R^2 + (X_L - X_C)^2}

where X L = ω L X_L = \omega L and X C = 1 ω C X_C = \frac{1}{\omega C}.

Resonance Condition:

When X L = X C X_L = X_C, impedance is minimum and current is maximum:

f r = 1 2 π L C f_r = \frac{1}{2\pi \sqrt{LC}}

8. Displacement Current and Maxwell's Equations

🔹 Displacement Current ( I d I_d) : Accounts for a changing electric field in capacitors.

I d = ε 0 d Φ E d t 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 n , radius R 1 R_1, R 2 R_2:

1 f = ( n 1 ) ( 1 R 11 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 d , wavelength λ \lambda , and screen distance D D :

Fringe widthw = λ D d \text{Fringe width} \quad w = \frac{\lambda D}{d}

Bright fringes : Constructive interference.
Dark fringes : Destructive interference.



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