For the given circuit, the value of base current $I_b$ of the npn transistor is ........... mA. ($\beta$ is the current gain and assume the Op-Amp as ideal.) (Specify your answer in mA up to two digits after decimal.) 
Step 1: Understand Op-amp behavior.
The Op-Amp keeps the inverting and non-inverting terminals at the same voltage (ideal Op-Amp). Both nodes thus stay at $+5\,\text{V}$.
Step 2: Compute current through 1k resistor.
The emitter resistor is 1k and bottom node is grounded, so emitter current flows through 1k from +10V:
$I_e = \frac{10 - 5}{1k} = 5\,\text{mA}$.
Step 3: Relate emitter and base currents.
For transistor: $I_e = I_b + I_c$ and $I_c = \beta I_b$.
Thus, $I_e = (\beta + 1)I_b = 51 I_b$.
Step 4: Compute base current.
$I_b = \frac{5\,\text{mA}}{51} \approx 0.098\,\text{mA} \approx 0.10\,\text{mA}$.




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.)