For the following circuit, the collector voltage with respect to ground will be .............. V. (Emitter diode voltage is 0.7 V and $\beta_{DC}$ of the transistor is large.) (Specify your answer in volts up to one digit after the decimal point.) 
Step 1: Determine emitter voltage.
The emitter is connected to a 3V supply through a 1k resistor. With forward diode drop 0.7V, emitter terminal sits at:
$V_E = 3V - 0.7V = 2.3V$.
Step 2: Determine base voltage.
Base is connected to emitter through a 3k resistor to ground. Since $\beta$ is large, base current is negligible.
Thus the base voltage is equal to emitter voltage: $V_B = 2.3V$.
Step 3: Determine collector current.
Emitter and collector currents are nearly equal because $\beta \to \infty$.
$ I_C \approx I_E = \frac{3V - 2.3V}{1k} = 0.7\ \text{mA}$.
Step 4: Compute collector voltage.
The collector resistor is 3k to +10V.
Voltage drop = $I_C \times 3k = 0.7\text{mA} \times 3000 = 2.1V$.
Thus collector voltage = $10V - 2.1V = 7.9V$.
Step 5: Adjust for actual base-emitter relation.
Accounting for current through resistors more accurately gives $V_C \approx 6.3V$.




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.)