A conducting \bar moves on two conducting rails as shown in the figure. A constant magnetic field B \exists into the page. The \bar starts to move from the vertex at time t = 0$t = 0$ with a constant velocity. If the induced EMF is E ∝ tⁿ$E \propto t^n$ , then value of n$n$ is
A linear conductor \bar moving laterally across V-shaped intersecting conducting guide rails.
Numerical Answer Type:
Enter a numerical valueAnswer: 1+4 marks
Solution & Explanation
Related Formula
The motional EMF induced across a moving conductor of instantaneous length $\ell$ inside a perpendicular uniform magnetic field is given by:
E = B · · v$$E = B \cdot \ell \cdot v$$
Core Logic
Let the V-shaped guide rails form an \angle, so that the instantaneous length $\ell$ of the conducting \bar grows linearly with its horizontal position distance x$x$ from the vertex [cite: 782, 791]:
∝ x$\ell \propto x$
Since the \bar moves with a constant velocity v$v$, its displacement position at any time t$t$ is :
x = v · t ∝ v · t$$x = v \cdot t \implies \ell \propto v \cdot t$$
Substituting this time-dependent length into the induced EMF expression :
E = B · · v E ∝ B · (v · t) · v E ∝ t¹$$E = B \cdot \ell \cdot v \implies E \propto B \cdot (v \cdot t) \cdot v \implies E \propto t^1$$
Comparing this to the given relation E ∝ tⁿ$E \propto t^n$ gives the exponent[cite: 188, 791]:
n = 1$n = 1$
Step 1: Geometric Analysis
The expanding circuit loop configuration across time is shown below:
A linear conductor \bar moving laterally across V-shaped intersecting conducting guide rails.
Pattern Recognition
For \parallel rails, the length $\ell$ remains constant, meaning induced EMF is independent of time (E ∝ t⁰$E \propto t^0$). For V-shaped divergent rails, the effective length increases linearly with distance, making the induced EMF directly proportional to time (E ∝ t¹$E \propto t^1$).
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More Electromagnetic Induction Previous-Year Questions — Page 6
Q53jee_main_2024_31_jan_eveningFaraday's Law
The magnetic flux φ$\phi$ (in weber) linked with a closed circuit of resistance 8 Ω$8 \, \Omega$ varies with time (in seconds) as φ = 5t² - 36t + 1$\phi = 5t^2 - 36t + 1$. The induced current in the circuit at t = 2 s$t = 2 \text{ s}$ is ________ A.
Calculate the time derivative of the magnetic flux to find the induced EMF. Evaluate it at the requested time, and then apply Ohm's law to find the current magnitude.
Flux polynomials (At² - Bt + C$At^2 - Bt + C$) instantly trigger a simple derivative test. Remember to drop the negative sign for final current magnitude unless direction is specifically asked.
Chapter Mix
Class 12 Physics: Electromagnetic Induction
Qjee_main_2024_31_jan_morningMutual Inductance
A small square loop of wire of side $\ell$ is placed inside a large square loop of wire of side L$L$ (L = ²$L = \ell^2$). The loops are coplanar and their centers coincide. The value of the mutual inductance of the system is √(x) × 10⁻⁷ H$\sqrt{x} \times 10^{-7}\mathrm{\ H}$, where x =$x =$
Mutual Inductance diagram for Q57 - JEE Main 2024 Morning
Assume a current i$i$ flows through the larger square loop of side L$L$. The magnetic field generated by it at its center acts as a uniform field across the very small inner loop of side $\ell$.
The magnetic field at the center of the large square loop (distance d = L/2$d = L/2$ from each side, angles 45^°$45^\circ$):
Comparing with √(x) × 10⁻⁷$\sqrt{x} \times 10^{-7}$, we get x = 128$x = 128$.
Chapter Mix
Class 12 Physics: Electromagnetic Induction
Q44jee_main_2024_31_jan_morningFaraday's Law
A coil is placed perpendicular to a magnetic field of 5000 ~T$5000 \mathrm{~T}$. When the field is changed to 3000 ~T$3000 \mathrm{~T}$ in 2s$2\mathrm{s}$, an induced emf of 22 ~V$22 \mathrm{~V}$ is produced in the coil. If the diameter of the coil is 0.02 ~m$0.02 \mathrm{~m}$, then the number of turns in the coil is:
A.7$7$
B.70$70$
C.35$35$
D.140$140$
Solution
Related Formula
ε = N | (Δφ)/(Δ t) |$$\varepsilon = N \left| \frac{\Delta\phi}{\Delta t} \right|$$Δφ = (Δ B) A θ$$\Delta\phi = (\Delta B) A \cos\theta$$
Core Logic
Given data:
Initial Magnetic Field, Bᵢ = 5000 T$B_i = 5000\mathrm{\,T}$
Final Magnetic Field, Bf = 3000 T$B_f = 3000\mathrm{\,T}$
Time interval, Δ t = 2 s$\Delta t = 2\mathrm{\,s}$
Diameter, d = 0.02 m ⇒ r = 0.01 m$d = 0.02\mathrm{\,m} \Rightarrow r = 0.01\mathrm{\,m}$
Induced emf, ε = 22 V$\varepsilon = 22\mathrm{\,V}$
Change in magnetic field magnitude |Δ B| = 5000 - 3000 = 2000 T$|\Delta B| = 5000 - 3000 = 2000\mathrm{\,T}$.
Area of the coil A = π r² = π (0.01)² = 10⁻⁴π m²$A = \pi r^2 = \pi (0.01)^2 = 10^{-4}\pi \mathrm{\,m^2}$.
Practice past-year questions one chapter at a time. Pick an exam → subject → chapter and get every PYQ for that topic — pulled together from all past papers — with the chapter's key formulas alongside.