To find the current flowing through the 20 Ω resistance, we must analyze the circuit in terms of the voltage across the external resistance and the total resistance in the circuit.
First, consider the two batteries in parallel:
The equivalent voltage \(V_{eq}\) and equivalent internal resistance \(R_{eq}\) for parallel batteries are given by:
\(V_{eq} = \frac{V_1/r_1 + V_2/r_2}{1/r_1 + 1/r_2}\)
Substitute the given values:
\(V_{eq} = \frac{10/0.5 + 12/0.8}{1/0.5 + 1/0.8} = \frac{20 + 15}{2 + 1.25} = \frac{35}{3.25} \approx 10.77\,V\)
For the equivalent internal resistance:
\(R_{eq} = \frac{(r_1 \cdot r_2)}{r_1 + r_2} = \frac{(0.5 \times 0.8)}{0.5 + 0.8} = \frac{0.4}{1.3} \approx 0.3077\,\Omega\)
Now, the total resistance, \(R_t\), in the circuit is the sum of \(R_{eq}\) and the external resistance, 20 \( \Omega \):
\(R_t = R_{eq} + 20 = 0.3077 + 20 \approx 20.3077\,\Omega\)
The current \(I\) through the 20 \( \Omega \) resistance can then be found using Ohm's law:
\(I = \frac{V_{eq}}{R_t} = \frac{10.77}{20.3077} \approx 0.53\,A\)
Therefore, the current flowing through the 20 Ω resistance is approximately 0.53 A.
This circuit has two batteries connected in parallel, both feeding a single external resistor of 20 ohms. Instead of using the shortcut formulas for equivalent EMF and equivalent internal resistance, the same result can be found by writing a direct node-voltage (Kirchhoff current law) equation at the junction where both batteries meet the external resistor. Let \( V \) be the voltage at that junction relative to the common negative terminal. The current leaving battery 1 into the node is \( \frac{10-V}{0.5} \), the current leaving battery 2 into the node is \( \frac{12-V}{0.8} \), and the current leaving the node through the external resistor is \( \frac{V}{20} \). Since current into the node equals current out:
\[ \frac{10-V}{0.5} + \frac{12-V}{0.8} = \frac{V}{20} \]Multiplying out and collecting terms gives \( 35 - 3.25V = \frac{V}{20} \), and solving this for \( V \) gives \( V \approx 10.61 \, \text{V} \). The current through the 20 ohm resistor is then \( I = \frac{V}{20} \approx 0.53 \, \text{A} \). Let's check this against each option.
Solving the node equation directly, without relying on the equivalent-EMF formula, confirms the same junction voltage and current found by that shortcut.
Therefore, the correct answer is 0.53 A.