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Two slender rods released, angular velocity of AB

Short answer

Central impact: line of impact passes through both mass centres, causing pure translation. Eccentric impact: line misses at least one mass centre, adding rotation. Using work-energy, gravitational work 18.72 J equals final kinetic energy of both rods; with kinematics ω_BD = ω_AB, solving gives ω_AB = 3.51 rad/s clockwise. Velocity of D = 1.80 m/s horizontally to the right.

Differentiate the central and Eccentric impact of the body. Each of the two slender rods as shown in figure below is 0.75 m long and has a mass of 6 kg. If the system is released from rest when β=50∘\beta = 50^\circ, determine (a) the angular velocity of rod "AB" when β=20∘\beta = 20^\circ (b) the velocity of point 'D' at the same instant. [Figure: two pinned slender rods AB and BD, each 0.75 m, forming an inverted V; A pinned on the ground, D on rollers on the ground; β=50∘\beta = 50^\circ at A.]

Central and eccentric impact

PointCentral impactEccentric impact
Line of impactPasses through the mass centres of both bodiesDoes not pass through the mass centre of at least one body
Motion after impactPure translation along the line of impactTranslation plus rotation
UnknownsOnly the final velocitiesFinal velocities and angular velocities
Equations usedLinear momentum and restitutionLinear and angular momentum and restitution
ExampleTwo smooth spheres colliding head-onA ball striking the end of a rod

Motion of the two rods

Rods ABAB and BDBD are identical (L=0.75L=0.75 m, m=6m=6 kg), joined by a pin at BB. AA is a fixed pin and DD slides on a smooth horizontal surface (rollers). Released from rest at β=50∘\beta=50^\circ, the system moves under gravity only, so use the work-energy principle.

          B
         / \
        /   \
       /     \
    A /_______\ D   (rollers)
       beta

Kinematics

Let ωAB\omega_{AB} be the angular velocity of ABAB. v⃗B⊥AB\vec v_B \perp AB and v⃗D\vec v_D is horizontal. The ICR II of BDBD lies on the line ABAB extended and on the vertical through DD. By symmetry of the triangle ABDABD, IB=BD=LIB = BD = L and ID=2Lsin⁡βID = 2L\sin\beta, so

ωBD=vBIB=ωABLL=ωAB=ω\omega_{BD} = \frac{v_B}{IB} = \frac{\omega_{AB}L}{L} = \omega_{AB} = \omega

(the two rods turn in opposite senses). The centre G2G_2 of BDBD is at (1.5Lcos⁡β, 0.5Lsin⁡β)(1.5L\cos\beta,\ 0.5L\sin\beta) and II is at (2Lcos⁡β, 2Lsin⁡β)(2L\cos\beta,\ 2L\sin\beta), so

(IG2L)2=0.25cos⁡2β+2.25sin⁡2β\left(\frac{IG_2}{L}\right)^2 = 0.25\cos^2\beta + 2.25\sin^2\beta

At β=20∘\beta = 20^\circ: 0.25cos⁡220∘+2.25sin⁡220∘=0.48400.25\cos^2 20^\circ + 2.25\sin^2 20^\circ = 0.4840, so IG2=0.5218IG_2 = 0.5218 m.

Kinetic energy at β=20∘\beta = 20^\circ

TAB=12(13mL2)ω2=12(1.1250) ω2T_{AB} = \tfrac12\left(\tfrac13mL^2\right)\omega^2 = \tfrac12(1.1250)\,\omega^2 TBD=12[112mL2+m(IG2)2]ω2=12(1.9146) ω2T_{BD} = \tfrac12\left[\tfrac1{12}mL^2 + m(IG_2)^2\right]\omega^2 = \tfrac12(1.9146)\,\omega^2 T2=12(1.1250+1.9146) ω2=1.5198 ω2T_2 = \tfrac12(1.1250 + 1.9146)\,\omega^2 = 1.5198\,\omega^2

Work of gravity

Heights of the mass centres: L2sin⁡β\tfrac L2\sin\beta for each rod, so the total potential energy is V=mgLsin⁡βV = mgL\sin\beta.

U1→2=mgL(sin⁡50∘−sin⁡20∘)=6(9.81)(0.75)(0.7660−0.3420)=18.72 JU_{1\to2} = mgL(\sin50^\circ - \sin20^\circ) = 6(9.81)(0.75)(0.7660 - 0.3420) = 18.72\ \text{J}

(a) Angular velocity of AB

T1+U1→2=T2:0+18.72=1.5198 ω2  ⇒  ωAB=3.51 rad/sT_1 + U_{1\to2} = T_2:\quad 0 + 18.72 = 1.5198\,\omega^2 \;\Rightarrow\; \omega_{AB} = 3.51\ \text{rad/s}

AB turns clockwise (B moving down and to the right).

(b) Velocity of D

DD is ID=2Lsin⁡20∘ID = 2L\sin20^\circ from the ICR:

vD=ωBD (ID)=3.51×2(0.75)sin⁡20∘=3.51×0.5130=1.80 m/s (→)v_D = \omega_{BD}\,(ID) = 3.51\times2(0.75)\sin20^\circ = 3.51\times0.5130 = 1.80\ \text{m/s}\ (\to)

Answer: ωAB=3.51\omega_{AB} = 3.51 rad/s clockwise; vD=1.80v_D = 1.80 m/s horizontally to the right.

✓ Answer checked by Claude Opus 5.5 (high effort)

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