The rod PQ slides along 2 parallel rails as shown in the figure. It has a length of 20 cm and is perpendicular to the 2 rails. It performs simple harmonic motion with amplitude 5 cm and frequency 10 Hz. The magnetic field is 10-4T and is directed perpendicular to the plane of paper. What is the peak induced electro-magnetic force?
2\(\pi\)x10-7 V
4π2x10-3 V
2\(\pi\)x10-5 V
4\(\pi\)x10-5 V
\(\pi\)2x10-4 V
Given:
Step 1: Determine Maximum Velocity (\( v_{\text{max}} \))
For simple harmonic motion, the maximum velocity is given by:
\[ v_{\text{max}} = A \omega \]
where angular frequency \( \omega = 2\pi f \).
Substitute values:
\[ v_{\text{max}} = 0.05 \times (2\pi \times 10) = \pi \, \text{m/s} \]
Step 2: Calculate Peak Induced EMF (\( \mathcal{E}_{\text{max}} \))
The induced EMF in a moving rod is:
\[ \mathcal{E} = B L v \]
At peak velocity, the peak EMF is:
\[ \mathcal{E}_{\text{max}} = B L v_{\text{max}} \]
Substitute known values:
\[ \mathcal{E}_{\text{max}} = 10^{-4} \times 0.2 \times \pi = 2\pi \times 10^{-5} \, \text{V} \]
Conclusion:
The peak induced electro-magnetic force is \( 2\pi \times 10^{-5} \, \text{V} \).
Answer: \(\boxed{C}\)
The rod has a length of \( 20 \, \text{cm} \), an amplitude of \( 5 \, \text{cm} \), and a frequency of \( 10 \, \text{Hz} \). The magnetic field is \( B = 10^{-4} \, \text{T} \) and is directed perpendicular to the plane of the paper.
Step 1: Recall Faraday's Law of Electromagnetic Induction
The induced EMF (\( \mathcal{E} \)) in a conductor moving through a magnetic field is given by: \[ \mathcal{E} = B \cdot l \cdot v, \] where: - \( B \) is the magnetic field strength, - \( l \) is the length of the conductor, - \( v \) is the velocity of the conductor. For SHM, the velocity of the rod as a function of time is: \[ v(t) = A \omega \cos(\omega t), \] where: - \( A \) is the amplitude of the motion, - \( \omega \) is the angular frequency (\( \omega = 2\pi f \)), - \( f \) is the frequency of the motion. The peak velocity (\( v_{\text{peak}} \)) occurs when \( \cos(\omega t) = 1 \): \[ v_{\text{peak}} = A \omega. \] Step 2: Substitute Known Values
1. Length of the rod (\( l \))**: \[ l = 20 \, \text{cm} = 0.2 \, \text{m}. \] 2. Amplitude (\( A \)): \[ A = 5 \, \text{cm} = 0.05 \, \text{m}. \] 3. Frequency (\( f \)): \[ f = 10 \, \text{Hz}. \] 4. Angular frequency (\( \omega \)): \[ \omega = 2\pi f = 2\pi \times 10 = 20\pi \, \text{rad/s}. \] 5. Peak velocity (\( v_{\text{peak}} \)): \[ v_{\text{peak}} = A \omega = 0.05 \times 20\pi = \pi \, \text{m/s}. \] 6. Magnetic field (\( B \)): \[ B = 10^{-4} \, \text{T}. \] Step 3: Calculate the Peak Induced EMF
Using the formula for induced EMF: \[ \mathcal{E}_{\text{peak}} = B \cdot l \cdot v_{\text{peak}}. \] Substitute the values: \[ \mathcal{E}_{\text{peak}} = 10^{-4} \cdot 0.2 \cdot \pi = 2 \times 10^{-5} \pi \, \text{V}. \] Simplify: \[ \mathcal{E}_{\text{peak}} = 2\pi \times 10^{-5} \, \text{V}. \] Final Answer: The peak induced electromotive force is: \[ \boxed{2\pi \times 10^{-5} \, \text{V}}, \] which corresponds to option \( \mathbf{(C)} \).
Let \( I = \int_{-\frac{\pi}{4}}^{\frac{\pi}{4}} \frac{\tan^2 x}{1+5^x} \, dx \). Then:
Magnetic flux refers to the amount of magnetic field passing through a given area. It is a measure of the strength of the magnetic field over a particular surface. The unit of magnetic flux is the Weber (Wb).
Magnetic flux is determined by the strength of the magnetic field and the area over which it is applied. The magnetic field is a vector field that exerts a force on moving charged particles. It is represented by magnetic lines of force that show the direction and intensity of the field. The magnetic flux passing through a surface is proportional to the number of magnetic field lines passing through that surface.
The magnetic flux through a closed surface is always zero, as the field lines entering the surface must also exit the surface. This principle is known as Gauss's law for magnetism. However, for an open surface, the magnetic flux can be calculated using the formula:
\(Φ = B.A.cosθ\)
where Φ is the magnetic flux, B is the magnetic field, A is the area of the surface, and θ is the angle between the magnetic field and the surface normal.
Also Read: Unit of Magnetic Flux
Magnetic flux has various applications in physics and engineering, including electromagnetic induction, which is used in electrical generators and transformers. The amount of magnetic flux generated by a magnet can also be used to measure its strength, and it is often used in magnetic imaging techniques such as magnetic resonance imaging (MRI).