Relative Velocity & Acceleration - Statics and Dynamics

  1. Using the velocity loop equation vB=vA+ωAB×rB/A\mathbf{v}_B = \mathbf{v}_A + \boldsymbol{\omega}_{AB}\times\mathbf{r}_{B/A}, combined with the constraint that B moves perpendicular to O₂B (i.e., B's velocity is horizontal at this instant), find ωAB\omega_{AB} (angular velocity of the coupler AB).
    Answer: ωAB=−43 rad/s≈−2.31 rad/s\omega_{AB} = -\frac{4}{\sqrt{3}}\,\text{rad/s} \approx -2.31\,\text{rad/s} (CW), obtained by enforcing the constraint that vBy=0v_{By} = 0 and solving the j^\hat{j}-component of the relative velocity equation. When analyzing four-bar linkage velocities, your strategy should be to write the vector loop equation, express each cross product in component form, then apply kinematic constraints to isolate unknowns — one equation per unknown. Here, the coupler AB makes 30° above horizontal, so rB/A=0.5cos⁡30° i^+0.5sin⁡30° j^=34i^+14j^\mathbf{r}_{B/A} = 0.5\cos30°\,\hat{i} + 0.5\sin30°\,\hat{j} = \frac{\sqrt{3}}{4}\hat{i} + \frac{1}{4}\hat{j} m. With ωAB=ωABk^\boldsymbol{\omega}_{AB} = \omega_{AB}\hat{k}, the cross product gives ωAB×rB/A=ωAB(−14i^+34j^)\boldsymbol{\omega}_{AB}\times\mathbf{r}_{B/A} = \omega_{AB}(-\frac{1}{4}\hat{i} + \frac{\sqrt{3}}{4}\hat{j}). Since O₂B is vertical, B can only move horizontally, meaning vBy=0v_{By} = 0. Applying the j^\hat{j}-component of vB=vA+ωAB×rB/A\mathbf{v}_B = \mathbf{v}_A + \boldsymbol{\omega}_{AB}\times\mathbf{r}_{B/A}: 0=2+ωAB⋅340 = 2 + \omega_{AB}\cdot\frac{\sqrt{3}}{4}, which yields ωAB=−83⋅12=−43≈−2.31 rad/s\omega_{AB} = -\frac{8}{\sqrt{3}} \cdot \frac{1}{2} = -\frac{4}{\sqrt{3}} \approx -2.31\,\text{rad/s}. The negative sign confirms clockwise rotation. This is answer A, the correct choice. Answer B reaches the same magnitude but positive, reflecting a sign error — typically from reversing rB/A\mathbf{r}_{B/A} to point from B to A instead of A to B, which flips the cross product components incorrectly. Answer C uses only the i^\hat{i}-component without enforcing vBy=0v_{By} = 0, leaving one equation with two unknowns (ωAB\omega_{AB} and vBxv_{Bx}) and guessing a value — a fundamental setup error. Answer D simply divides ∣vA∣|\mathbf{v}_A| by the coupler length, ignoring both the angle of the coupler and the kinematic constraint on B's motion entirely. Your key takeaway: always apply the geometric constraint on B's velocity direction before solving — it's what makes the system determinate.

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