Force on the Bent Wire
Step 1: Use the property of uniform magnetic field.
For a wire carrying current in a uniform magnetic field,
\[
\vec F
=
I(\vec L\times\vec B),
\]
where \(\vec L\) is the displacement vector joining the initial and final points.
Step 2: Determine the effective length vector.
From the figure,
horizontal displacement
\[
=50\,\text{cm}=0.50\,m.
\]
Vertical displacement
\[
=-20\,\text{cm}=-0.20\,m.
\]
Therefore
\[
\vec L
=
0.50\hat i-0.20\hat j.
\]
Step 3: Calculate \(\vec L\times\vec B\).
Given
\[
\vec B=-0.50\hat k.
\]
Hence
\[
\vec L\times\vec B
=
(0.50\hat i-0.20\hat j)\times(-0.50\hat k).
\]
Using
\[
\hat i\times\hat k=-\hat j,
\qquad
\hat j\times\hat k=\hat i,
\]
\[
\vec L\times\vec B
=
0.25\hat j+0.10\hat i.
\]
Step 4: Calculate force vector.
\[
\vec F
=
I(\vec L\times\vec B).
\]
Since
\[
I=2.0\,A,
\]
\[
\vec F
=
0.20\hat i+0.50\hat j.
\]
Step 5: Find magnitude.
\[
F
=
\sqrt{(0.20)^2+(0.50)^2}.
\]
\[
F
=
\sqrt{0.29}.
\]
\[
F
=
0.538\,N.
\]
Therefore,
\[
\boxed{
F\approx0.54\,N
}
\]