The induced electric field \( E(r) \) at a distance \( r \) from the axis of a solenoid is obtained from Faradayโs law of electromagnetic induction:
\[ \oint \mathbf{E} \cdot d\mathbf{l} = -\frac{d\Phi_B}{dt} \]
where \( \Phi_B \) is the magnetic flux through the solenoid.
The magnetic flux through a circle of radius \( r \) inside the solenoid is:
\[ \Phi_B = B(t) \cdot \pi r^2 \]
The magnetic flux through the solenoid remains constant and is determined by its radius \( R \):
\[ \Phi_B = B(t) \cdot \pi R^2 \]
For \( r = 0.07m > R =0.05m \), the induced electric field \( E(r) \) is given by:
\[ E(r) \cdot 2\pi r = -\frac{d}{dt} \left( B(t) \cdot \pi R^2 \right) \]
Substituting \( B(t) = B_0 \sin(\omega t) \), the time derivative is:
\[ \frac{dB}{dt} = B_0 \omega \cos(\omega t) \]
Thus, the induced electric field is:
\[ E(r) = \frac{R^2}{2r} \cdot B_0 \omega \]
\[ E(r) = \frac{(0.05)^2}{2 \times 0.07} \times 0.98 \times 100 \]
\[ E(r) = \frac{0.0025}{0.14} \times 98 \]
\[ E(r) = 1.71 \text{ V/m} \]
The amplitude of the induced electric field is 1.71 V/m.
At a particular temperature T, Planck's energy density of black body radiation in terms of frequency is \(\rho_T(\nu) = 8 \times 10^{-18} \text{ J/m}^3 \text{ Hz}^{-1}\) at \(\nu = 3 \times 10^{14}\) Hz. Then Planck's energy density \(\rho_T(\lambda)\) at the corresponding wavelength (\(\lambda\)) has the value \rule{1cm}{0.15mm} \(\times 10^2 \text{ J/m}^4\). (in integer)
[Speed of light \(c = 3 \times 10^8\) m/s]
(Note: The unit for \(\rho_T(\nu)\) in the original problem was given as J/mยณ, which is dimensionally incorrect for a spectral density. The correct unit J/(mยณยทHz) or Jยทs/mยณ is used here for the solution.)