Step 1: Assign potentials to the circuit nodes.
Let the right terminal be at zero potential:
\[
V_R=0
\]
The left terminal is connected to a \(10\,\text{V}\) battery, so
\[
V_L=10\,\text{V}
\]
Let the potentials of the top and bottom junctions of the bridge be \(V_T\) and \(V_B\) respectively.
The central battery is of \(4\,\text{V}\), so
\[
V_T-V_B=4
\]
Step 2: Apply Kirchhoff's current law to the supernode.
For the supernode containing \(V_T\) and \(V_B\),
\[
\frac{V_T-10}{2}+\frac{V_T-0}{1}+\frac{V_B-10}{1}+\frac{V_B-0}{4}=0
\]
\[
\frac{V_T-10}{2}+V_T+V_B-10+\frac{V_B}{4}=0
\]
Solving this with
\[
V_T-V_B=4
\]
we get
\[
V_T=\frac{80}{11}\,\text{V}
\]
and
\[
V_B=\frac{36}{11}\,\text{V}
\]
Step 3: Calculate \(I_1\).
Current through the \(2\,\Omega\) resistor is
\[
I_1=\frac{10-V_T}{2}
\]
\[
I_1=\frac{10-\frac{80}{11}}{2}
\]
\[
I_1=\frac{15}{11}
\]
\[
I_1=1.364\,\text{A}
\]
Step 4: Calculate \(I_2\).
Current through the \(1\,\Omega\) resistor in the lower left branch is
\[
I_2=\frac{10-V_B}{1}
\]
\[
I_2=10-\frac{36}{11}
\]
\[
I_2=\frac{74}{11}
\]
\[
I_2=6.727\,\text{A}
\]
Step 5: Calculate \(I_3\).
Using current balance at the top junction,
\[
I_3= \frac{V_T}{1}-I_1
\]
\[
I_3=\frac{80}{11}-\frac{15}{11}
\]
\[
I_3=\frac{65}{11}
\]
\[
I_3=5.91\,\text{A}
\]
Step 6: Final conclusion.
Therefore,
\[
\boxed{I_1=1.364\,\text{A},\ I_2=6.727\,\text{A},\ I_3=5.91\,\text{A}}
\]