\(Ey=60sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{j}Vm^{−1}\)
\(Bz=2sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{k}T\)
\(Ey=60sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{j}Vm^{−1}\)
\(Bz=2× 10^{-7} sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{k}T\)
\(Ey=2× 10^{-7}sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{j}Vm^{−1}\)
\(Bz=60 sin[\frac{π}{4}×10^3(x−3×10^8t)]\hat{k}T\)
\(Ey=2× 10^{-7}sin[\frac{π}{4}×10^4(x−4×10^8t)]\hat{j}Vm^{−1}\)
\(Bz=60 sin[\frac{π}{4}×10^4(x−4×10^8t)]\hat{k}T\)
In first 3 options speed of light is 3 × 108 m/sec and in the fourth option it is 4 × 108 m/sec.
Using E = CB
We can check the option is B.
If AB is incident plane wave front, then refracted wave front is (n\(_1\) → n\(_2\))
If $10 \sin^4 \theta + 15 \cos^4 \theta = 6$, then the value of $\frac{27 \csc^6 \theta + 8 \sec^6 \theta}{16 \sec^8 \theta}$ is:
If the area of the region $\{ (x, y) : |x - 5| \leq y \leq 4\sqrt{x} \}$ is $A$, then $3A$ is equal to
Let $A = \begin{bmatrix} \cos \theta & 0 & -\sin \theta \\ 0 & 1 & 0 \\ \sin \theta & 0 & \cos \theta \end{bmatrix}$. If for some $\theta \in (0, \pi)$, $A^2 = A^T$, then the sum of the diagonal elements of the matrix $(A + I)^3 + (A - I)^3 - 6A$ is equal to
Let $A = \{ z \in \mathbb{C} : |z - 2 - i| = 3 \}$, $B = \{ z \in \mathbb{C} : \text{Re}(z - iz) = 2 \}$, and $S = A \cap B$. Then $\sum_{z \in S} |z|^2$ is equal to
Let $C$ be the circle $x^2 + (y - 1)^2 = 2$, $E_1$ and $E_2$ be two ellipses whose centres lie at the origin and major axes lie on the $x$-axis and $y$-axis respectively. Let the straight line $x + y = 3$ touch the curves $C$, $E_1$, and $E_2$ at $P(x_1, y_1)$, $Q(x_2, y_2)$, and $R(x_3, y_3)$ respectively. Given that $P$ is the mid-point of the line segment $QR$ and $PQ = \frac{2\sqrt{2}}{3}$, the value of $9(x_1 y_1 + x_2 y_2 + x_3 y_3)$ is equal to
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: