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Collar on arm: velocity and relative acceleration

Short answer

At θ=45°, t=1.023 s. v_r=−0.614 m/s, v_θ=1.053 m/s, total v=1.219 m/s. a_r=−2.216 m/s², a_θ=−0.856, total a=2.376 m/s². Relative acceleration a_rel = r̈ = −0.6 m/s², toward O.

Rotation of the arm about O is defined by θ=0.75t2\theta = 0.75t^2 where θ\theta is in radians and tt in seconds. Collar B slides along the arm such that r=1−0.3t2r = 1 - 0.3t^2 where rr is in meters. After the arm has rotated through 45∘45^\circ, determine (a) the total velocity of the collar, (b) the total acceleration of the collar and (c) the relative acceleration of the collar with respect to the arm. [Figure: arm OA rotating about O at angle θ\theta, collar B at distance rr from O.]

Time when θ=45∘\theta=45^\circ

θ=45∘=0.7854 rad=0.75t2 ⇒ t2=1.0472, t=1.0233 s\theta=45^\circ=0.7854\ \text{rad}=0.75t^{2}\ \Rightarrow\ t^{2}=1.0472,\ t=1.0233\ \text{s}

Quantities at this instant

r=1−0.3t2=0.6858 mr˙=−0.6t=−0.6140 m/s,r¨=−0.6 m/s2θ˙=1.5t=1.5350 rad/s,θ¨=1.5 rad/s2\begin{aligned} r&=1-0.3t^{2}=0.6858\ \text{m}\\ \dot r&=-0.6t=-0.6140\ \text{m/s},\qquad \ddot r=-0.6\ \text{m/s}^2\\ \dot\theta&=1.5t=1.5350\ \text{rad/s},\qquad \ddot\theta=1.5\ \text{rad/s}^2 \end{aligned}

(a) Total velocity

vr=r˙=−0.6140 m/svθ=rθ˙=0.6858(1.5350)=1.0528 m/sv=vr2+vθ2=1.219 m/s\begin{aligned} v_r&=\dot r=-0.6140\ \text{m/s}\\ v_\theta&=r\dot\theta=0.6858(1.5350)=1.0528\ \text{m/s}\\ v&=\sqrt{v_r^{2}+v_\theta^{2}}=1.219\ \text{m/s} \end{aligned}

The velocity makes 120.3∘120.3^\circ with e^r\hat e_r, that is, 59.8∘59.8^\circ with the direction along the arm towards O.

(b) Total acceleration

ar=r¨−rθ˙2=−0.6−0.6858(1.5350)2=−2.216 m/s2aθ=rθ¨+2r˙θ˙=0.6858(1.5)+2(−0.6140)(1.5350)=−0.856 m/s2a=2.2162+0.8562=2.376 m/s2\begin{aligned} a_r&=\ddot r-r\dot\theta^{2}=-0.6-0.6858(1.5350)^{2}=-2.216\ \text{m/s}^2\\ a_\theta&=r\ddot\theta+2\dot r\dot\theta=0.6858(1.5)+2(-0.6140)(1.5350)=-0.856\ \text{m/s}^2\\ a&=\sqrt{2.216^{2}+0.856^{2}}=2.376\ \text{m/s}^2 \end{aligned}

(c) Acceleration relative to the arm

The collar moves along the arm, so relative to the arm (a rotating frame) its motion is rectilinear along rr:

arel=r¨=−0.6 m/s2a_{rel}=\ddot r=-0.6\ \text{m/s}^2

That is, 0.60.6 m/s2^2 directed towards O along the arm.

Answer: (a) v=1.219v=1.219 m/s; (b) a=2.376a=2.376 m/s2^2; (c) arel=0.6a_{rel}=0.6 m/s2^2 towards O.

✓ Answer checked by Claude Opus 5.5 (high effort)

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