The two sides perpendicular to the wire would contribute net zero emf.
The electric field induced is given by: \[ \vec{E} = \vec{B} \times \vec{v} \] Using Biot-Savart Law: \[ \vec{E} = \frac{\mu_0 I}{2 \pi x} \times v \]
Therefore, the net EMF between the two sides is: \[ \text{Net emf} = \left(E_1 \cos 60^\circ - E_2 \cos 60^\circ\right) \times \text{width} \] Substituting values: \[ = \frac{1}{2} \times \frac{2}{100} \times \frac{\mu_0 I v}{2\pi} \left[\frac{1}{4} - \frac{1}{8}\right] \] Simplifying further: \[ = \frac{1}{100} \times 10^{-7} \times 2 \times 10 \times v \times 100 \times \frac{1}{8} \] \[ = 2.5 \times 10^{-7} = i \times R \] Solving for \( v \): \[ v = \frac{10 \times 10^{-6} \times 0.1}{2.5 \times 10^{-7}} = 4 \, \text{m/s} \]
Induced emf in AB = (\((\vec{V}\times \vec{B}).\vec{l}\)
\(B=\frac{l_0i}{2\pi r}=\frac{4\pi\times10^{-7}}{2\pi\times 4\times10^{-2}}=\frac{1}{2}\times10^{-4}T\)
emf in AB=e1=\(B\times\frac{1}{2}\times2\times10^{-2}\times V\)
\(\Rightarrow \frac{V}{2}\times10^{-6}\,Volt\)
Induced emf in CD = \(e_2 = B\times \frac{1}{2}\times 2\times10^{-2}\times V\)
\(\Rightarrow \frac{\mu_0}{2\pi(8\times10^{-2})}\times\frac{1}{2}\times2\times10^{-2}\times V\)
\(\Rightarrow V\times\frac{1}{4}\times10^{-6}T\)
Emf in BC and AD are equal
emf in loop = \(e_1-e_2+e-e+e-e=e_1-e_2\)
\(V\times\frac{1}{2}\times10^{-6}-\frac{1}{4}\times10^{-6}\times V\)
\(=\frac{V}{4}\times10^{-6}\)
Resistance of loop = 0.1\(\Omega\)
Current in loop = I = \(\frac{V\times10^{-6}}{4\times0.1}=\frac{10}{4}\times V\mu A\)
\(\frac{10V}{4}=10\)
\(V=4\,ms\)
Two identical concave mirrors each of focal length $ f $ are facing each other as shown. A glass slab of thickness $ t $ and refractive index $ n_0 $ is placed equidistant from both mirrors on the principal axis. A monochromatic point source $ S $ is placed at the center of the slab. For the image to be formed on $ S $ itself, which of the following distances between the two mirrors is/are correct:
The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.
Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories: