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Static force analysis of slider crank

Short answer

A two-force member has forces at only two points, equal, opposite and collinear. A three-force member has three coplanar, concurrent forces summing to zero. For the slider-crank: connecting rod force = 2032.0 N, guide reaction = 359.2 N, crank torque = 166.8 N m.

Define two-force member and three-force member and state the conditions of equilibrium for each. In a slider crank mechanism the crank is 100 mm long and the connecting rod is 400 mm long. When the crank makes 45 degrees with the line of stroke, a force of 2000 N acts on the slider along the line of stroke, tending to push it towards the crank. Neglecting weights, inertia and friction, find (a) the force in the connecting rod, (b) the normal reaction of the guide on the slider, (c) the torque on the crank required to keep the mechanism in equilibrium, and verify the torque by the principle of virtual work.

Force members

  • Two-force member: a member acted upon by forces at only two points (no couple). For equilibrium the two forces are equal, opposite and collinear (along the line joining the points). The connecting rod (with pin joints at both ends and no load between) is a two-force member.
  • Three-force member: a member with forces at three points. For equilibrium the three forces must be coplanar, their lines of action must meet at one point (concurrent) and their vector sum must be zero (a closed force triangle). The slider block (force PP, guide reaction FNF_N, rod force FQF_Q) is a three-force member.

Geometry

sin⁡ϕ=rsin⁡θl=sin⁡45∘4=0.1768⇒ϕ=10.18∘\sin\phi = \frac{r\sin\theta}{l} = \frac{\sin45^\circ}{4} = 0.1768 \Rightarrow \phi = 10.18^\circ

Free-body of the slider

          F_N (guide reaction, perpendicular)
            ^
            |
   P  <-----[]----- F_Q (rod force)

The rod is a two-force member, so FQF_Q acts along the rod, at angle ϕ\phi to the line of stroke. Equilibrium of the slider:

FQcos⁡ϕ=P⇒FQ=2000cos⁡10.18∘=2032.0 NF_Q\cos\phi = P \Rightarrow F_Q = \frac{2000}{\cos 10.18^\circ} = 2032.0\ \text{N} FN=FQsin⁡ϕ=Ptan⁡ϕ=2000tan⁡10.18∘=359.2 NF_N = F_Q\sin\phi = P\tan\phi = 2000\tan 10.18^\circ = 359.2\ \text{N}

Torque on the crank

The rod force FQF_Q acts on the crank pin along the rod. The perpendicular distance from the crank centre O to the line of the rod is rsin⁡(θ+ϕ)r\sin(\theta + \phi). So

T=FQ rsin⁡(θ+ϕ)=2032.0×0.1×sin⁡55.18∘=166.8 N mT = F_Q\, r\sin(\theta + \phi) = 2032.0 \times 0.1 \times \sin 55.18^\circ = 166.8\ \text{N m}

(The radial component on the crank pin, FQcos⁡(θ+ϕ)=1160.2F_Q\cos(\theta+\phi) = 1160.2 N, only loads the bearing.)

Check by virtual work

Slider position from O: x=rcos⁡θ+l2−r2sin⁡2θx = r\cos\theta + \sqrt{l^2 - r^2\sin^2\theta}. For a virtual displacement δθ\delta\theta of the crank, the work of the input torque equals the work done against PP:

T δθ=P δx⇒T=P∣dxdθ∣=Pr[sin⁡θ+sin⁡2θ2n2−sin⁡2θ]T\,\delta\theta = P\,\delta x \Rightarrow T = P\left|\frac{dx}{d\theta}\right| = P r\left[\sin\theta + \frac{\sin2\theta}{2\sqrt{n^2 - \sin^2\theta}}\right] T=2000×0.1[0.7071+1.00002×3.937]=166.8 N mT = 2000 \times 0.1\left[0.7071 + \frac{1.0000}{2 \times 3.937}\right] = 166.8\ \text{N m}

It agrees with the free-body result.

Answer: FQ=2032.0F_Q = 2032.0 N, FN=359.2F_N = 359.2 N, T=166.8T = 166.8 N m.

✓ Answer checked by Claude Opus 5.5 (high effort)

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