A force of \(10\text{ N}\) acting at an angle on a particle produces a displacement of
\[
(3\hat{i}-4\hat{j})\text{ m}
\]
due to this force. If the kinetic energy of the particle is decreased by \(25\text{ J}\), then the angle between the force and the displacement is
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If work done is negative, the angle between force and displacement is obtuse because
\[
\cos\theta\lt 0.
\]
Step 1: Apply the work-energy theorem. Net work done $= \Delta KE$. Since KE decreases by 25 J: $W = -25$ J. Step 2: Find the magnitude of the displacement vector. $\vec{s} = 3\hat{i} - 4\hat{j}$ m: \[ |\vec{s}| = \sqrt{9 + 16} = 5 \text{ m} \] Step 3: Use $W = F s \cos\theta$. \[ -25 = 10 \times 5 \times \cos\theta \Rightarrow \cos\theta = -\frac{1}{2} \] Step 4: Solve for $\theta$. \[ \theta = \cos^{-1}\!\left(-\frac{1}{2}\right) = 120^\circ \] The obtuse angle confirms the force has a component opposing displacement, decreasing KE. Step 5: Verify physically. Force component along displacement: $10\cos 120^\circ = -5$ N. Work $= -5 \times 5 = -25$ J. Confirmed. Step 6: State the final answer. \[ \boxed{\theta = 120^\circ} \]