The energy density of an EM wave is proportional to the square of the electric f ield. Squaring a sinusoidal function doubles the frequency.
The energy density of the wave is given by:
\( \text{Energy density} = \frac{1}{2} \varepsilon_0 E_{\text{net}}^2 \)
Substitute \( E_{\text{net}} = E_0 \sin(\omega t - kx) \):
\[ \text{Energy density} = \frac{1}{2} \varepsilon_0 E_0^2 \sin^2(\omega t - kx) \]
Using the trigonometric identity \( \sin^2 x = \frac{1}{2}(1 - \cos 2x) \):
\[ \sin^2(\omega t - kx) = \frac{1}{2}(1 - \cos(2\omega t - 2kx)) \]
Substitute this into the energy density formula:
\[ \text{Energy density} = \frac{1}{2} \varepsilon_0 E_0^2 \cdot \frac{1}{2}(1 - \cos(2\omega t - 2kx)) \]
Simplify the expression:
\[ \text{Energy density} = \frac{1}{4} \varepsilon_0 E_0^2 (1 - \cos(2\omega t - 2kx)) \]
The energy density of the wave is:
\( \frac{1}{4} \varepsilon_0 E_0^2 (1 - \cos(2\omega t - 2kx)) \)
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 : \(A_2 \rightleftharpoons 2A\)