Question 15.11: The crane shown rotates with a constant angular velocity V1 ......

The crane shown rotates with a constant angular velocity \text V_1 of 0.30 rad/s. Simultaneously, the boom is being raised with a constant angular velocity \text V_2 of 0.50 rad/s relative to the cab. Knowing that the length of the boom OP is l = 12 m, determine (a) the angular velocity V of the boom, (b) the angular acceleration A of the boom, (c) the velocity v of the tip of the boom, (d) the acceleration a of the tip of the boom.

15.11.1
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a. Angular Velocity of Boom. Adding the angular velocity \text V_1 of the cab and the angular velocity \text V_2 of the boom relative to the cab, we obtain the angular velocity V of the boom at the instant considered:

\mathrm{V}=\mathrm{V}_{1}+\mathrm{V}_{2} \quad\quad\quad \mathrm{V}=(0.30 ~\mathrm{rad} / \mathrm{s}) {j}+(0.50~ \mathrm{rad} / \mathrm{s}){k}

b. Angular Acceleration of Boom. The angular acceleration A of the boom is obtained by differentiating V. Since the vector \text V_1 is constant in magnitude and direction, we have

\mathrm{A}=\mathrm{\dot V}=\mathrm{\dot V}_{1}+\mathrm{\dot V}_{2}=0+\mathrm{\dot V}_{2}

where the rate of change \mathrm{\dot V}_2 is to be computed with respect to the fixed frame OXYZ. However, it is more convenient to use a frame Oxyz attached to the cab and rotating with it, since the vector \text V_2 also rotates with the cab and therefore has zero rate of change with respect to that frame. Using Eq. (15.31) with Q = \text V_2 and Ω = \text V_1, we write

\begin{aligned}(\dot{{Q}})_{\text {OXYZ }} & =(\dot{{Q}})_{\text {Oxyz }}+{\Omega} \times {Q} \\\left(\mathrm{\dot V}_{2}\right)_{\text {OXYZ }} & =\left(\mathrm{\dot V}_{2}\right)_{\text {Oxyz }}+\mathrm{V}_{1} \times \mathrm{V}_{2} \\\mathrm{~A}=\left(\mathrm{\dot V}_{2}\right)_{\text {OXYZ }} & =0+(0.30~ \mathrm{rad} / \mathrm{s}) {j} \times(0.50~ \mathrm{rad} / \mathrm{s}) {k}\end{aligned}

A = (0.15 rad/s²)i

c. Velocity of Tip of Boom. Noting that the position vector of point P is r = (10.39 m)i + (6 m)j and using the expression found for V in part a, we write

\begin{aligned}\mathrm{v}=\mathrm{V} \times {r}=\left|\begin{array}{ccc}{i} & {j} & {k} \\0 & 0.30~ \mathrm{rad} / \mathrm{s} & 0.50 ~\mathrm{rad} / \mathrm{s} \\10.39 \mathrm{~m} & 6 \mathrm{~m} & 0\end{array}\right| \\\mathrm{v}=-(3 \mathrm{~m} / \mathrm{s}){i}+(5.20 \mathrm{~m} / \mathrm{s}){j}-(3.12 \mathrm{~m} / \mathrm{s}){k}\end{aligned}

d. Acceleration of Tip of Boom. Recalling that v = V × r, we write

\begin{aligned}{a} & =\mathrm{A} \times {r}+\mathrm{V} \times(\mathrm{V} \times {r})={A} \times {r}+\mathrm{V} \times \mathrm{v} \\{a} & =\left|\begin{array}{ccc}{i} & {j} & {k} \\0.15 & 0 & 0 \\10.39 & 6 & 0\end{array}\right|+\left|\begin{array}{ccc}{i} & {j} &{k} \\0 & 0.30 & 0.50 \\-3 & 5.20 & -3.12\end{array}\right| \\& =0.90 {k}-0.94 {i}-2.60 {i}-1.50 {j}+0.90{k} \\& \mathbf{a}=-\left(3.54 \mathrm{~m} / \mathrm{s}^{2}\right) {i}-\left(1.50 \mathrm{~m} / \mathrm{s}^{2}\right) {j}+\left(1.80 \mathrm{~m} / \mathrm{s}^{2}\right) {k}\end{aligned}
15.11.2
15.11.3
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