The base voltage \( V_B \) is determined by the voltage divider formed by the 20kΞ© and 5kΞ© resistors:
\[ V_B = V_{CC} \cdot \frac{5k\Omega}{20k\Omega + 5k\Omega} \]
Substituting \( V_{CC} = 15V \):
\[ V_B = 15 \cdot \frac{5}{25} \]
\[ V_B = 3.0V \]
The emitter voltage \( V_E \) is related to the base voltage by:
\[ V_E = V_B - V_{BE} \]
Substituting \( V_{BE} = 0.7V \):
\[ V_E = 3.0 - 0.7 = 2.3V \]
The emitter current \( I_E \) is determined by the 2kΞ© resistor:
\[ I_E = \frac{V_E}{2k\Omega} \]
Substituting \( V_E = 2.3V \):
\[ I_E = \frac{2.3}{2000} \]
\[ I_E = 1.15mA \]
The collector current \( I_C \) is related to the emitter current \( I_E \) by:
\[ I_C = \frac{\beta}{\beta + 1} I_E \]
Substituting \( \beta = 100 \):
\[ I_C = \frac{100}{101} \times 1.15 \]
\[ I_C \approx 1.14mA \]
Thus, the collector current \( I_C \) is approximately 1.14mA.
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/mΒ³, which is dimensionally incorrect for a spectral density. The correct unit J/(mΒ³Β·Hz) or JΒ·s/mΒ³ is used here for the solution.)