The figure shows a circuit containing two diodes \(D_1\) and \(D_2\) with threshold voltages \(V_{TH}\) of 0.7 V and 0.3 V, respectively. Considering the simplified diode model, which assumes diode I–V characteristics as shown in the plot on the right, the current through the resistor \(R\) is ......... µA. 
Step 1: Analyze the diode configuration.
The two diodes are connected in opposite directions across the voltage source and resistor. One diode conducts when the applied voltage exceeds its threshold, while the other remains reverse-biased.
Step 2: Determine the effective voltage across the resistor.
When \(D_1\) (0.7 V) is forward-biased, \(D_2\) (0.3 V) will be reverse-biased since their orientation is opposite.
Hence, total voltage drop across both diodes is approximately:
\[
V_{D1} + V_{D2} = 0.7 + 0.3 = 1.0 \, \text{V}
\]
Effective voltage across the resistor:
\[
V_R = 10 - 1.0 = 9.0 \, \text{V}
\]
Step 3: Calculate current through the resistor.
\[
I = \frac{V_R}{R} = \frac{9.0}{100 \times 10^3} = 90 \, \mu\text{A}
\]
However, since both diodes don't conduct simultaneously (only one forward conducts), the actual current corresponds to one conduction path:
\[
I = \frac{(10 - 0.7 - 0.3)}{100 \times 10^3} = \frac{9}{100000} = 90 \, \mu\text{A}
\]
Step 4: Conclusion.
Thus, the current through the resistor is \(90 \, \mu\text{A}\).

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.)