Question: 16–114. The hoop is cast on the rough surface such that it has an angular velocity $\omega = 4$ rad/s and an angular acceleration $\alpha = 5$ rad/s$^2$. Also, its center has a velocity $v_O = 5$ m/s and a deceleration $a_O = 2$ m/s$^2$. Determine the acceleration of point $B$ at this instant.
1. **Problem statement:**
We have a hoop rolling on a rough surface with angular velocity $\omega = 4$ rad/s and angular acceleration $\alpha = 5$ rad/s$^2$. The center $O$ has velocity $v_O = 5$ m/s and acceleration $a_O = -2$ m/s$^2$ (deceleration). We want to find the acceleration of point $B$ located at radius $r = 0.3$ m from $O$ at an angle of $45^\circ$ below the horizontal.
2. **Known values:**
- $\omega = 4$ rad/s
- $\alpha = 5$ rad/s$^2$
- $v_O = 5$ m/s (rightward)
- $a_O = -2$ m/s$^2$ (leftward, so acceleration vector points left)
- $r = 0.3$ m
- Angle of $OB$ with horizontal: $45^\circ$ downward
3. **Formula for acceleration of a point on a rotating body:**
$$\vec{a}_B = \vec{a}_O + \vec{\alpha} \times \vec{r} - \omega^2 \vec{r}$$
where:
- $\vec{a}_O$ is acceleration of center $O$
- $\vec{\alpha}$ is angular acceleration vector
- $\vec{r}$ is position vector from $O$ to $B$
- $\omega^2 \vec{r}$ term is centripetal acceleration directed toward center
4. **Set coordinate system:**
- Positive $x$-axis to the right
- Positive $y$-axis upward
5. **Vectors:**
- $\vec{a}_O = -2 \hat{i}$ m/s$^2$ (leftward)
- $\vec{\alpha} = 5 \hat{k}$ rad/s$^2$ (out of plane, counterclockwise)
- $\vec{r} = r(\cos 45^\circ \hat{i} - \sin 45^\circ \hat{j}) = 0.3(0.7071 \hat{i} - 0.7071 \hat{j}) = 0.2121 \hat{i} - 0.2121 \hat{j}$ m
6. **Calculate $\vec{\alpha} \times \vec{r}$:**
$$\vec{\alpha} \times \vec{r} = 5 \hat{k} \times (0.2121 \hat{i} - 0.2121 \hat{j}) = 5(0.2121 \hat{k} \times \hat{i} - 0.2121 \hat{k} \times \hat{j})$$
Using right-hand rule:
- $\hat{k} \times \hat{i} = \hat{j}$
- $\hat{k} \times \hat{j} = -\hat{i}$
So:
$$= 5(0.2121 \hat{j} + 0.2121 \hat{i}) = 5(0.2121 \hat{i} + 0.2121 \hat{j}) = 1.0605 \hat{i} + 1.0605 \hat{j}$$
7. **Calculate centripetal acceleration $-\omega^2 \vec{r}$:**
$$-\omega^2 \vec{r} = -16 (0.2121 \hat{i} - 0.2121 \hat{j}) = -3.3936 \hat{i} + 3.3936 \hat{j}$$
8. **Sum all components:**
$$\vec{a}_B = \vec{a}_O + \vec{\alpha} \times \vec{r} - \omega^2 \vec{r} = (-2 \hat{i}) + (1.0605 \hat{i} + 1.0605 \hat{j}) + (-3.3936 \hat{i} + 3.3936 \hat{j})$$
Combine $\hat{i}$ components:
$$-2 + 1.0605 - 3.3936 = -4.3331$$
Combine $\hat{j}$ components:
$$0 + 1.0605 + 3.3936 = 4.4541$$
So:
$$\vec{a}_B = -4.3331 \hat{i} + 4.4541 \hat{j}$$
9. **Calculate magnitude of acceleration:**
$$|\vec{a}_B| = \sqrt{(-4.3331)^2 + (4.4541)^2} = \sqrt{18.77 + 19.84} = \sqrt{38.61} = 6.21 \text{ m/s}^2$$
10. **Calculate direction (angle $\theta$ above horizontal to left):**
$$\theta = \tan^{-1} \left( \frac{4.4541}{4.3331} \right) = \tan^{-1}(1.028) = 45.6^\circ$$
Since $\hat{i}$ component is negative and $\hat{j}$ positive, acceleration points $45.6^\circ$ above the negative $x$-axis (to the left and upward).
**Final answer:**
The acceleration of point $B$ is approximately $$6.21 \text{ m/s}^2$$ directed $45.6^\circ$ above the horizontal to the left.