In: Physics
Knowing that at the instant shown the angular velocity of rod BE is 4 rad/s counterclockwise, determine (a) the angular velocity of rod AD, (b) the velocity of collar D, (c) the velocity of point A.
Concepts and reason Equations of motion:
Equation of motions refers to the equations which describe the attributes of a moving object in terms of displacement, velocity, and acceleration. Vector:
Vector form is used to represent a quantity in terms of magnitude and direction. This form is expressed as magnitude multiplied by direction in terms of \(\mathbf{i}, \mathbf{j}\) and \(\mathbf{k}\) representing the three perpendicular axes \(x, y\) and \(z\) respectively of a quantity. Angular displacement:
Angular displacement is the angle through which an object moves on a circular path. It is denoted by \(\boldsymbol{\theta}\) Angular velocity:
The rate of change of angular displacement of a body with respect to time is angular velocity. It is denoted by \(\omega\) and its unit is \(\mathrm{rad} / \mathrm{s}\)
Relative velocity It is defined as the velocity measurement of a moving object with reference as a translating frame or another moving object. The relative velocity between points \(\mathrm{B}\) and \(\mathrm{D}\) can be used to obtain the angular velocity of the link and the velocity of point \(\mathrm{D}\). Then relative velocity between points \(\mathrm{B}\) and \(\mathrm{A}\) can be used to calculate the velocity of point \(\mathrm{A} .\)
Fundamentals
\(A(x, y, z)\)
For a point with coordinates as \( {A}(x, y, 2) \) in motion, the position vector with respect to the origin is expressed as \(\mathbf{r}=x \mathbf{i}+y \mathbf{j}+z \mathbf{k}\)
Here, the position vector is \(\mathbf{r}\).
Write the relation for velocity and angular velocity \((\omega)\)
\(v=r \omega\)
Here, the constant velocity is \(v\) and the radius of the circular path is \(r\) \(\left(v_{B / A}\right)\)
The formula to calculate the relative velocity \( \left(V_{B / A}\right) \) of point \(\mathrm{B}\) with respect to point \(\mathrm{A}\) of an object is as follows:
\( v_{B / A}=v_{B}-v_{A} \)
Here, velocity of object \(\mathrm{B}\) is \( {v_{B}} \) and velocity of object \(\mathrm{A}\) is \( {v_A} \). From the angular velocity definition, the expression can also be written as follows:
\(v_{B / A}=\omega r_{B / A}\)
\(v_{B}-v_{A}=\omega r_{B / A}\)
Here, relative position of \(\mathrm{B}\) with respect to \(\mathrm{A}\) is \(\boldsymbol{r}_{B / A}\). The velocity of B with respect to origin A from the observer measurement can be rewritten in vector form as follows:
\(\mathbf{v}_{B}=\mathbf{v}_{A}-\boldsymbol{\omega} \times \mathbf{r}_{B / A}\)
Cross product rule of vectors:
\(\mathbf{i} \times \mathbf{i}=\mathbf{0}\)
\(\mathbf{j} \times \mathbf{j}=\mathbf{0}\)
\(\mathbf{k} \times \mathbf{k}=\mathbf{0}\)
\(\mathbf{i} \times \mathbf{j}=\mathbf{k}\)
\(\mathbf{j} \times \mathbf{k}=\mathbf{i}\)
\(\mathbf{k} \times \mathbf{i}=\mathbf{j}\)
\(\mathbf{j} \times \mathbf{i}=-\mathbf{k}\)
\(\mathbf{k} \times \mathbf{j}=-\mathbf{i}\)
\(\mathbf{i} \times \mathbf{k}=-\mathbf{j}\)
Calculate the linear velocity \(\left(v_{B}\right)\) of point \(\mathrm{B}\).
\(v_{B}=r_{B E} \omega_{B E}\)
Here, the distance BE is \(r_{B E}\) and the angular velocity of \(\mathrm{BE}\) is \(\omega_{B E}\).
Substitute \(0.192 \mathrm{~m}\) for \(r_{B E}\) and \(4 \mathrm{rad} / \mathrm{s}\) for \(\omega_{B E}\).
\(v_{B}=0.192 \mathrm{~m} \times 4 \mathrm{rad} / \mathrm{s}\)
\(v_{B}=0.768 \mathrm{~m} / \mathrm{s}\)
Write the velocity of point \(\mathrm{B}\) in Cartesian vector form. \(\mathbf{v}_{B}=0.768 \mathbf{i} \mathrm{m} / \mathrm{s}\)
The velocity of point B acts along only in the horizontal direction. Thus the velocity of point B is calculated as the product of radius and angular velocity of link BE.
(A)
Write the position vector for \(\mathrm{BD}\left(\mathbf{r}_{B D}\right)\).
\(\mathbf{r}_{B D}=\left(0.36 \cos 30^{\circ} \mathbf{i}-0.36 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m}\)
Write the expression for relative velocity between points \(B\) and D for link AD.
\(\mathbf{v}_{D}=\mathbf{v}_{B}-\omega_{A D} \mathbf{k} \times \mathbf{r}_{B D}\)
Here, the velocity of point \(\mathrm{D}\) is \(v_{D}\), and the angular velocity of link \(\mathrm{AD}\) is \(\omega_{A D}\).
Substitute \(-v_{D} \mathbf{j}_{\text {for }} \mathbf{v}_{D}, 0.768 \mathbf{i} \mathrm{m} / \mathrm{s}\) for \(\mathbf{v}_{B}\), and \(\left(0.36 \cos 30^{\circ} \mathbf{i}-0.36 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m}_{\text {for }} \mathbf{r}_{B D}\).
\(\begin{aligned}-v_{D} \mathbf{j} &=0.768 \mathbf{i} \mathrm{m} / \mathrm{s}-\omega_{A D} \mathbf{k} \times\left(0.36 \cos 30^{\circ} \mathbf{i}-0.36 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m} \\ &=0.768 \mathbf{i}-\left(0.36 \cos 30^{\circ}\right) \omega_{A D} \mathbf{j}-\left(0.36 \sin 30^{\circ}\right) \omega_{A D} \mathbf{i} \\-v_{D} \mathbf{j} &=\left[0.768-\left(0.36 \sin 30^{\circ}\right) \omega_{A D}\right] \mathbf{i}-\left(0.36 \cos 30^{\circ}\right) \omega_{A D} \mathbf{j} \end{aligned}\)
Equate the coefficients of \(\mathbf{i}\) from Equation (1).
\(0.768-\left(0.36 \sin 30^{\circ}\right) \omega_{A D}=0\)
\(\omega_{A D}=4.267 \mathrm{rad} / \mathrm{s}\)
The position vector for the link BD is obtained. Then the expression for the relative velocity between points B and D is used to obtain the equation (1). Then i components are equated on both sides of equation (1) to calculate the angular velocity of the link AD.
(B) Rewrite the Equation (1).
\(-v_{D} \mathbf{j}=\left[0.768-\left(0.36 \sin 30^{\circ}\right) \omega_{A D}\right] \mathbf{i}-\left(0.36 \cos 30^{\circ}\right) \omega_{A D} \mathbf{j}\)
Equate the components of \(\mathrm{j}\)
\(-v_{D}=-\left(0.36 \cos 30^{\circ}\right) \omega_{A D}\)
Substitute \(4.267 \mathrm{rad} / \mathrm{s}\) for \(\omega_{A D}\).
\(v_{D}=0.360 \cos 30^{\circ} \times 4.267\)
\(v_{D}=1.33 \mathrm{~m} / \mathrm{s}\)
Equation (1) obtained for the velocity of D in vector form is considered. Then components of j are equated on both sides of the expression to calculate the velocity of collar D.
(c)
Write the position vector for \(\mathrm{AB}\left(\mathbf{r}_{A B}\right)\).
\(\mathbf{r}_{A B}=\left(0.24 \cos 30^{\circ} \mathbf{i}-0.24 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m}\)
Write the expression for relative velocity between points \(A\) and \(B\) for link \(A B\).
\(\mathbf{v}_{A}=\mathbf{v}_{B}+\omega_{A D} \mathbf{k} \times \mathbf{r}_{A B}\)
Here, velocity of point \(\mathrm{A}\) is \(\boldsymbol{v}_{A}\).
Substitute \(0.768 \mathbf{i} \mathrm{m} / \mathrm{s}\) for \(\mathbf{v}_{B}, 4.267 \mathrm{rad} / \mathrm{s}\) for \(\omega_{A D, \text { and }}\left(0.24 \cos 30^{\circ} \mathbf{i}-0.24 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m}_{\text {for }} \mathbf{r}_{A B}\).
\(\begin{aligned} \mathbf{v}_{A} &=0.768 \mathrm{i} \mathrm{m} / \mathrm{s}+(4.267 \mathrm{rad} / \mathrm{s}) \mathbf{k} \times\left(0.24 \cos 30^{\circ} \mathbf{i}-0.24 \sin 30^{\circ} \mathbf{j}\right) \mathrm{m} \\ &=(1.28 \mathbf{i}+0.887 \mathbf{j}) \mathrm{m} / \mathrm{s} \end{aligned}\)
Calculate the magnitude of velocity of point \(A\).
\(v_{A}=\sqrt{(1.28)^{2}+(0.887)^{2}}\)
\(=1.557 \mathrm{~m} / \mathrm{s}\)
The position vector for the link AB is obtained. Then the expression for the relative velocity between points B and A is used to obtain the velocity of A in vector form.
Part A
The angular velocity of rod AD \(\left(\omega_{A D}\right)\) is \(4.267 \mathrm{rad} / \mathrm{s}\).
Part B
The velocity of collar D \(\left(v_{D}\right)\) is \(1.33 \mathrm{~m} / \mathrm{s}\).
Part C
The velocity of point \(A\left(v_{A}\right)\) is \(1.557 \mathrm{~m} / \mathrm{s}\)