Given Data:
RD1 = 1.5 kΩ, RL = 2.5 kΩ, V = 15 V, VD1 = 0.3 V, VD2 = 0.7 V.
The voltage across the resistive portion of the circuit can be found by subtracting the voltage drops across the two diodes from the applied voltage:
Vresistive = V - (VD1 + VD2).
Substituting the values:
Vresistive = 15 V - (0.3 V + 0.7 V) = 14 V.
The total resistance in the resistive portion of the circuit is the sum of RD1 and RL:
Rtotal = RD1 + RL = 1.5 kΩ + 2.5 kΩ = 4.0 kΩ.
Using Ohm’s Law, the total current i in the circuit is given by:
i = \(\frac{V_{resistive}}{R_{total}}\).
Substituting the values:
i = \(\frac{14 \text{ V}}{4.0 \text{ k}\Omega}\) = \(\frac{14}{4000}\) A = 0.0035 A = 3.5 mA.
The voltage across the load resistance RL, denoted as VL, is given by Ohm’s Law:
VL = i × RL.
Substituting the values:
VL = 3.5 mA × 2.5 kΩ = 0.0035 A × 2500 Ω = 8.75 V.
Final Result: The voltage across the load resistance RL is:
VL = 8.75 V
A constant voltage of 50 V is maintained between the points A and B of the circuit shown in the figure. The current through the branch CD of the circuit is :
The current passing through the battery in the given circuit, is:
Let \( S = \left\{ m \in \mathbb{Z} : A^m + A^m = 3I - A^{-6} \right\} \), where
\[ A = \begin{bmatrix} 2 & -1 \\ 1 & 0 \end{bmatrix} \]Then \( n(S) \) is equal to ______.