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
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
Current passing through a wire as function of time is given as $I(t)=0.02 \mathrm{t}+0.01 \mathrm{~A}$. The charge that will flow through the wire from $t=1 \mathrm{~s}$ to $\mathrm{t}=2 \mathrm{~s}$ is:
In the figure shown below, a resistance of 150.4 $ \Omega $ is connected in series to an ammeter A of resistance 240 $ \Omega $. A shunt resistance of 10 $ \Omega $ is connected in parallel with the ammeter. The reading of the ammeter is ______ mA.
Match List-I with List-II: List-I