The given circuit has the following elements:
- A 5 V battery in series with a 2Ω resistor.
- A 10 V battery in series with a 1Ω resistor and a 2Ω resistor.
Step 1: Assign currents to the branches:
Let the current in the branch with the 5V source and 2Ω resistor be \( I_1 \), the current in the branch with the 10V source and 1Ω resistor be \( I_2 \), and the current in the branch with the 2Ω resistor be \( I_3 \).
Step 2: Apply Kirchhoff's Voltage Law (KVL):
For loop 1 (containing the 5V source and 2Ω resistor):
\[
5 - 2I_1 = 0 \quad \Rightarrow \quad I_1 = \frac{5}{2} \, \text{A}
\]
For loop 2 (containing the 10V source, 1Ω resistor, and 2Ω resistor):
\[
10 - 1I_2 - 2I_3 = 0
\]
Apply Kirchhoff's Current Law (KCL):
At the junction where the currents meet, we have:
\[
I_1 = I_2 + I_3
\]
Substitute \( I_1 = \frac{5}{2} \) into the equation:
\[
\frac{5}{2} = I_2 + I_3
\]
Step 3: Solve the system of equations:
We have two equations:
1. \( 10 - I_2 - 2I_3 = 0 \)
2. \( \frac{5}{2} = I_2 + I_3 \)
From the first equation:
\[
I_2 = 10 - 2I_3
\]
Substitute this into the second equation:
\[
\frac{5}{2} = (10 - 2I_3) + I_3
\]
\[
\frac{5}{2} = 10 - I_3
\]
\[
I_3 = 10 - \frac{5}{2} = \frac{15}{2} \, \text{A}
\]
Now substitute \( I_3 = \frac{15}{2} \) back into \( I_2 = 10 - 2I_3 \):
\[
I_2 = 10 - 2 \times \frac{15}{2} = 10 - 15 = -5 \, \text{A}
\]
Thus, the current values are:
- \( I_1 = \frac{5}{2} \, \text{A} \)
- \( I_2 = -5 \, \text{A} \)
- \( I_3 = \frac{15}{2} \, \text{A} \)
The negative sign in \( I_2 \) indicates that the direction of current in the second branch is opposite to the assumed direction.