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Conservation of energy; 5 kg collar on curved rod

Short answer

Mechanical energy (kinetic + gravitational + elastic) is conserved. With the given spring and rod dimensions, the collar's speed at B is 2.67 m/s, and because C is at the same height and spring extension as A, it stops there (v_C = 0).

Explain about the conservation of energy in study of kinetics of particles with relevant equation. A 5 kg collar is attached to a spring and slides without friction in a vertical plane along a curved rod ABC. The spring is undeformed when its length is 100 mm and its constant is 800 N/m. If the collar is released at 'A' with no initial velocity, determine its velocity a) as it passes B b) as it reaches C. [Figure: semicircular rod ABC; collar at A at the right end, C at the left end; spring from the collar to the vertical axis through B; dimensions 150 mm, 250 mm and 200 mm.]

Conservation of energy in kinetics of particles

When a particle moves under conservative forces only (weight, elastic spring force), the sum of kinetic energy T=12mv2T=\tfrac12mv^{2} and potential energy V=Vg+VeV=V_g+V_e stays constant:

T1+V1=T2+V2,Vg=mgy,Ve=12kx2T_1+V_1=T_2+V_2,\qquad V_g=mgy,\quad V_e=\tfrac12kx^{2}

where xx is the spring deformation from its undeformed length. Forces that do no work (normal reaction of a smooth rod) can be ignored.

Collar problem

Assumed geometry (figure dimensions 150, 200, 250 mm): semicircular rod of radius 0.20.2 m with A and C at the same level, B 0.20.2 m below. The spring is fixed at D on the vertical axis through B, 0.150.15 m below the line AC. Then the spring length is LA=LC=0.22+0.152=0.25L_A=L_C=\sqrt{0.2^{2}+0.15^{2}}=0.25 m and LB=0.2−0.15=0.05L_B=0.2-0.15=0.05 m. Undeformed length 0.100.10 m; k=800k=800 N/m; m=5m=5 kg.

Spring deformations: xA=xC=0.25−0.10=0.15x_A=x_C=0.25-0.10=0.15 m (stretched) and xB=0.05−0.10=−0.05x_B=0.05-0.10=-0.05 m (compressed).

a) At B

Released from rest at A (take B as datum, hA=0.2h_A=0.2 m):

0+mghA+12kxA2=12mvB2+0+12kxB20+mgh_A+\tfrac12kx_A^{2}=\tfrac12mv_B^{2}+0+\tfrac12kx_B^{2} 5(9.81)(0.2)+12(800)(0.15)2=12(5)vB2+12(800)(0.05)25(9.81)(0.2)+\tfrac12(800)(0.15)^{2}=\tfrac12(5)v_B^{2}+\tfrac12(800)(0.05)^{2} 9.81+9.00=2.5vB2+1.00 ⇒ vB2=7.124,  vB=2.669 m/s9.81+9.00=2.5v_B^{2}+1.00\ \Rightarrow\ v_B^{2}=7.124,\ \ v_B=2.669\ \text{m/s}

b) At C

C is at the same height as A and the spring has the same length, so both potential energies are the same as at A:

12mvC2=0 ⇒ vC=0\tfrac12mv_C^{2}=0\ \Rightarrow\ v_C=0

Answer: vB≈2.67v_B\approx2.67 m/s and vC=0v_C=0 for the geometry assumed above. If the figure shows C at a different level or spring length, use the same energy equation with those values.

✓ Answer checked by Claude Opus 5.5 (high effort)

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