The maximum current through the Zener diode is given by:
\[ I_{\text{max}, Z} = \frac{P_Z}{V_Z} \]
Substituting \( P_Z = 2W \) and \( V_Z = 10V \):
\[ I_{\text{max}, Z} = \frac{2}{10} = 0.2A \]
The Zener diode is connected in reverse bias and maintains a constant voltage of \( V_Z = 10V \).
The normal diode is forward-biased, resulting in a voltage drop of \( V_D = 0.7V \).
The voltage across the resistance \( V_L \) is the difference between the Zener voltage \( V_Z \) and the forward voltage drop of the normal diode \( V_D \):
\[ V_L = V_Z - V_D \]
Substituting \( V_Z = 10V \) and \( V_D = 0.7V \):
\[ V_L = 10 - 0.7 = 9.3V \]
The current through the resistance \( I_L \) is given by:
\[ I_L = \frac{V_L}{R_L} \]
Substituting \( V_L = 9.3V \) and \( R_L = 2000\Omega \):
\[ I_L = \frac{9.3}{2000} = 0.00465A \]
The power dissipated across the resistor is:
\[ P_L = I_L^2 \cdot R_L \]
Substituting \( I_L = 0.00465A \) and \( R_L = 2000\Omega \):
\[ P_L = (0.00465)^2 \times 2000 \]
\[ P_L = 0.043225 \times 2000 = 86.45mW \]
This power dissipation is well within the resistor’s limit, confirming that the circuit is operating safely.
The voltage drop across the \( 2k\Omega \) resistance is approximately:
\[ 6.2V \]
Thus, the circuit operates safely with a voltage drop of approximately 6.2V across the \( 2k\Omega \) resistor.
Match the LIST-I with LIST-II
LIST-I | LIST-II |
---|---|
A. Brillouin Zone | Provides the understanding of the origin of allowed and forbidden bands in solids. |
B. Extended Zone Scheme | The electrons in a crystal behave like free electrons for most of the \( k \) values except when it approaches \( n\pi/a \). |
C. Periodic Zone Scheme | The E-k curve for several values of \( n \) reduced into the first zone for a simple cubic lattice with vanishing potential. |
D. Reduced Zone Scheme | The E-K curve is not continuous and has discontinuities at \( k = \pm n\pi/a \), where \( n=1,2,3,\dots \). |
Choose the correct answer from the options given below:
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/m³, which is dimensionally incorrect for a spectral density. The correct unit J/(m³·Hz) or J·s/m³ is used here for the solution.)