A body initially at rest undergoes linear motion with constant acceleration under the action of a constant force. Then the power delivered to the body at time \(t\) is proportional to
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For constant force, power increases linearly with velocity.
Concept:
Power:
\[
P = F \cdot v
\]
Step 1: Velocity under constant acceleration.
\[
v = at
\]
Step 2: Substitute in power.
\[
P = F \cdot at
\]
Since \(F\) and \(a\) are constants:
\[
P \propto t
\]