16.96 Vm–1
2.25 × 10–2 Vm–1
8.48 Vm–1
6.75 × 106 Vm–1
H = 4.5 × 10–2
So B = μ0μH
Thus
E=\(\frac{c}{n}\)B
(where n ⇒ refractive index)
So
E = \(\frac{3\times10^8\times4\pi\times10{-7}\times1.61\times4.5\times10^{-2}}{\sqrt{1.61\times6.44}}\)
E = 8.48
The correct option is (A): 16.96 Vm–1
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
Transverse waves are a type of wave in which the disturbance moves perpendicular to the direction of the wave propagation. In other words, the particles of the medium through which the wave is travelling oscillate perpendicular to the direction of the wave's movement.
Examples of transverse waves include light waves, electromagnetic waves, and waves on a string or rope. In these types of waves, the oscillations are perpendicular to the direction of the wave propagation.
Transverse waves have several characteristics that define their behavior. One of these is wavelength, which is the distance between two consecutive crests or troughs in the wave. Another characteristic is frequency, which is the number of waves that pass a given point per unit time. The amplitude of a transverse wave is the maximum displacement of the particles of the medium from their equilibrium position.
Also Read: Amplitude Formula
Transverse waves can be reflected, refracted, and diffracted, just like other types of waves. They obey the laws of superposition, which means that the displacement of the medium caused by two waves passing through each other is equal to the sum of their individual displacements.
Transverse waves have many practical applications, such as in the transmission of information through fiber-optic cables, the creation of images in microscopy, and in the production of electromagnetic radiation for various uses.