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Coriolis acceleration; rod AB and BD velocity

Short answer

Coriolis acceleration is the additional acceleration 2ω×v_rel experienced by a point moving relative to a rotating body, e.g., a collar sliding on a rotating arm. From velocity analysis: ω_AB = 3.20 rad/s clockwise; velocity of midpoint of BD is 1.26 m/s.

Define Coriolis acceleration of a rigid body in general plane motion. For the figure shown knowing that at the instant shown the velocity of point D is 2.4 m/s upward, determine (a) the angular velocity of rod AB, (b) the velocity of the midpoint of rod BD. [Figure: rod AB vertical with slider A at the top; rod BD inclined from B down to D, D on a horizontal slider E; vertical dimensions 0.2 m and 0.25 m; horizontal dimensions 0.2 m and 0.6 m.]

Coriolis acceleration is the extra acceleration a point has when it moves relative to a rotating (moving) frame or body. If a point PP moves with relative velocity v⃗rel\vec v_{rel} on a body rotating with angular velocity ω⃗\vec\omega, then

a⃗P=a⃗P′+a⃗rel+2ω⃗×v⃗rel\vec a_P = \vec a_{P'} + \vec a_{rel} + 2\vec\omega\times\vec v_{rel}

where a⃗P′\vec a_{P'} is the acceleration of the coincident point of the rotating frame. The term a⃗c=2ω⃗×v⃗rel\vec a_c = 2\vec\omega\times\vec v_{rel} is the Coriolis acceleration. Its magnitude is 2ωvrel2\omega v_{rel} and its direction is that of v⃗rel\vec v_{rel} rotated through 90∘90^\circ in the sense of ω\omega. It exists only when the point slides on the rotating body (for example a collar sliding on a rotating arm, or a slider in a slotted rotating link); it is zero for two points fixed in the same rigid body, such as the crank pin and piston pin of a connecting rod.

Velocity analysis

The figure is not fully legible, so I assume: ABAB is a vertical rod of length 0.250.25 m pinned at the top end AA to a fixed support; BDBD runs from BB down to DD with horizontal projection 0.60.6 m and drop 0.20.2 m; and DD is constrained to move vertically (given vD=2.4v_D = 2.4 m/s upward). Take xx to the right, yy up.

r⃗D/B=(0.6 i^−0.2 j^) m,v⃗D=2.4 j^ m/s\vec r_{D/B} = (0.6\,\hat i - 0.2\,\hat j)\ \text{m}, \qquad \vec v_D = 2.4\,\hat j\ \text{m/s}

Rod ABAB rotates about AA, so v⃗B=ωABk^×(−0.25j^)=0.25 ωAB i^\vec v_B = \omega_{AB}\hat k\times(-0.25\hat j) = 0.25\,\omega_{AB}\,\hat i is horizontal.

For rod BDBD:

v⃗D=v⃗B+ωBDk^×r⃗D/B=vBi^+ωBD(0.2 i^+0.6 j^)\vec v_D = \vec v_B + \omega_{BD}\hat k\times\vec r_{D/B} = v_{B}\hat i + \omega_{BD}(0.2\,\hat i + 0.6\,\hat j) j^:2.4=0.6 ωBD  ⇒  ωBD=4.00 rad/s (ccw)i^:0=vB+0.2(4.00)  ⇒  vB=−0.80 m/s\begin{aligned} \hat j:&\quad 2.4 = 0.6\,\omega_{BD} \;\Rightarrow\; \omega_{BD} = 4.00\ \text{rad/s (ccw)}\\ \hat i:&\quad 0 = v_B + 0.2(4.00) \;\Rightarrow\; v_B = -0.80\ \text{m/s} \end{aligned}

(a) Angular velocity of AB

ωAB=vB0.25=−0.800.25=−3.20 rad/s\omega_{AB} = \frac{v_B}{0.25} = \frac{-0.80}{0.25} = -3.20\ \text{rad/s}

so ∣ωAB∣=3.20|\omega_{AB}| = 3.20 rad/s, clockwise (the sign shows that BB moves to the left).

(b) Velocity of the midpoint of BD

v⃗M=v⃗B+ωBDk^×(12r⃗D/B)=(−0.80 i^)+4.00(0.1 i^+0.3 j^)=(−0.40 i^+1.20 j^) m/s\vec v_M = \vec v_B + \omega_{BD}\hat k\times\left(\tfrac12\vec r_{D/B}\right) = (-0.80\,\hat i) + 4.00(0.1\,\hat i + 0.3\,\hat j) = (-0.40\,\hat i + 1.20\,\hat j)\ \text{m/s} vM=1.26 m/sv_M = 1.26\ \text{m/s}

Answer: ωAB=3.20\omega_{AB} = 3.20 rad/s clockwise; vM=1.26v_M = 1.26 m/s.

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