Step 1: Recall the force on a current-carrying wire segment.
The magnetic force on a straight wire of length $\vec{l}$ carrying current $I$ in a uniform field $\vec{B}$ is:
\[
\vec{F} = I(\vec{l} \times \vec{B})
\]
Step 2: Consider the concept of net displacement vector for the whole loop.
For the entire closed triangular loop, the sum of all the displacement vectors $\vec{l}_i$ (for each side, going around the loop) must equal zero, because the loop returns to the starting point.
Step 3: Write the total force on the closed loop.
Since the field $\vec{B}$ is uniform (does not depend on position), we can take it outside the sum:
\[
\vec{F}_\text{net} = I \left(\sum_i \vec{l}_i\right) \times \vec{B}
\]
Step 4: Evaluate the sum of displacement vectors.
For a closed loop, the vector sum of all side lengths (with direction) is zero:
\[
\sum_i \vec{l}_i = \vec{0}
\]
Step 5: Compute the net force.
\[
\vec{F}_\text{net} = I(\vec{0}) \times \vec{B} = \vec{0}
\]
Step 6: State the answer.
No matter what the shape of the closed loop, the net force in a uniform magnetic field is always zero.
\[
\boxed{0}
\]