The problem describes a radially slotted arm whose rotation is governed by $\theta = 0.2t + 0.02t^2$. The distance of a slider B from point O is given by $r = 0.2 + 0.04t^2$. We are asked to calculate the magnitudes of the velocity and acceleration of the slider at time $t = 3$ s. $\theta$ is in radians and $r$ is in meters.

Applied MathematicsKinematicsPolar CoordinatesDerivativesVelocityAccelerationEngineering Mechanics
2025/7/1

1. Problem Description

The problem describes a radially slotted arm whose rotation is governed by θ=0.2t+0.02t2\theta = 0.2t + 0.02t^2. The distance of a slider B from point O is given by r=0.2+0.04t2r = 0.2 + 0.04t^2. We are asked to calculate the magnitudes of the velocity and acceleration of the slider at time t=3t = 3 s. θ\theta is in radians and rr is in meters.

2. Solution Steps

First, we calculate the first and second derivatives of θ\theta and rr with respect to time.
θ=0.2t+0.02t2\theta = 0.2t + 0.02t^2
θ˙=dθdt=0.2+0.04t\dot{\theta} = \frac{d\theta}{dt} = 0.2 + 0.04t
θ¨=d2θdt2=0.04\ddot{\theta} = \frac{d^2\theta}{dt^2} = 0.04
r=0.2+0.04t2r = 0.2 + 0.04t^2
r˙=drdt=0.08t\dot{r} = \frac{dr}{dt} = 0.08t
r¨=d2rdt2=0.08\ddot{r} = \frac{d^2r}{dt^2} = 0.08
Next, we evaluate these derivatives at t=3t = 3 s.
θ˙(3)=0.2+0.04(3)=0.2+0.12=0.32 rad/s\dot{\theta}(3) = 0.2 + 0.04(3) = 0.2 + 0.12 = 0.32 \text{ rad/s}
θ¨(3)=0.04 rad/s2\ddot{\theta}(3) = 0.04 \text{ rad/s}^2
r(3)=0.2+0.04(32)=0.2+0.04(9)=0.2+0.36=0.56 mr(3) = 0.2 + 0.04(3^2) = 0.2 + 0.04(9) = 0.2 + 0.36 = 0.56 \text{ m}
r˙(3)=0.08(3)=0.24 m/s\dot{r}(3) = 0.08(3) = 0.24 \text{ m/s}
r¨(3)=0.08 m/s2\ddot{r}(3) = 0.08 \text{ m/s}^2
Now, we calculate the radial and transverse components of velocity and acceleration.
vr=r˙v_r = \dot{r}
vθ=rθ˙v_\theta = r\dot{\theta}
ar=r¨rθ˙2a_r = \ddot{r} - r\dot{\theta}^2
aθ=rθ¨+2r˙θ˙a_\theta = r\ddot{\theta} + 2\dot{r}\dot{\theta}
At t=3t=3 s,
vr(3)=r˙(3)=0.24 m/sv_r(3) = \dot{r}(3) = 0.24 \text{ m/s}
vθ(3)=r(3)θ˙(3)=0.56(0.32)=0.1792 m/sv_\theta(3) = r(3)\dot{\theta}(3) = 0.56(0.32) = 0.1792 \text{ m/s}
ar(3)=r¨(3)r(3)θ˙(3)2=0.080.56(0.32)2=0.080.56(0.1024)=0.080.057344=0.022656 m/s2a_r(3) = \ddot{r}(3) - r(3)\dot{\theta}(3)^2 = 0.08 - 0.56(0.32)^2 = 0.08 - 0.56(0.1024) = 0.08 - 0.057344 = 0.022656 \text{ m/s}^2
aθ(3)=r(3)θ¨(3)+2r˙(3)θ˙(3)=0.56(0.04)+2(0.24)(0.32)=0.0224+0.1536=0.176 m/s2a_\theta(3) = r(3)\ddot{\theta}(3) + 2\dot{r}(3)\dot{\theta}(3) = 0.56(0.04) + 2(0.24)(0.32) = 0.0224 + 0.1536 = 0.176 \text{ m/s}^2
Finally, we calculate the magnitudes of the velocity and acceleration.
v=vr2+vθ2=(0.24)2+(0.1792)2=0.0576+0.03211264=0.089712640.2995 m/sv = \sqrt{v_r^2 + v_\theta^2} = \sqrt{(0.24)^2 + (0.1792)^2} = \sqrt{0.0576 + 0.03211264} = \sqrt{0.08971264} \approx 0.2995 \text{ m/s}
a=ar2+aθ2=(0.022656)2+(0.176)2=0.0005133+0.030976=0.03148930.1775 m/s2a = \sqrt{a_r^2 + a_\theta^2} = \sqrt{(0.022656)^2 + (0.176)^2} = \sqrt{0.0005133 + 0.030976} = \sqrt{0.0314893} \approx 0.1775 \text{ m/s}^2

3. Final Answer

The magnitude of the velocity of the slider at t=3t=3 s is approximately 0.29950.2995 m/s.
The magnitude of the acceleration of the slider at t=3t=3 s is approximately 0.17750.1775 m/s2^2.

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