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Spring force and contact force on cam follower

Short answer

During SHM rise, maximum inertia force is m a_max = 70.18 N. Minimum spring stiffness to prevent jump: (70.18 - 15)/0.025 = 2207 N/m. Maximum cam force at start = 85.2 N. A spring is needed because a disc cam only pushes; deceleration inertia would otherwise cause follower to lose contact.

A disc cam rotating at 400 rpm moves a horizontal translating roller follower of mass 0.8 kg through a lift of 25 mm with simple harmonic motion in 90 degrees of cam rotation. A return spring is preloaded with a force of 15 N when the follower is at its lowest position. Neglecting friction and the mass of the roller, find (a) the maximum inertia force during the rise, (b) the minimum spring stiffness required to prevent the follower from losing contact with the cam (jump) at the end of the rise, and (c) the maximum force exerted by the cam on the follower during the rise, taking this stiffness. Explain why the spring is needed.

Why a spring is needed

A disc cam can push the follower, but it cannot pull it back. During the second half of the rise the follower decelerates, and its inertia tends to carry it forward, away from the cam. A spring (or a positive-drive groove) must keep it in contact; otherwise the follower jumps and the intended motion is lost.

Follower acceleration (SHM rise)

a=π2hω22β2cos⁡πθβa = \frac{\pi^2 h\omega^2}{2\beta^2}\cos\frac{\pi\theta}{\beta}

Data: m=0.8m = 0.8 kg, h=0.025h = 0.025 m, β=90∘=π/2\beta = 90^\circ = \pi/2, ω=2π×40060=41.888\omega = \dfrac{2\pi \times 400}{60} = 41.888 rad/s, ω2=1754.6\omega^2 = 1754.6.

amax=π2hω22β2=π2(0.025)(1754.6)2(π/2)2=87.73 m/s2a_{max} = \frac{\pi^2 h\omega^2}{2\beta^2} = \frac{\pi^2 (0.025)(1754.6)}{2(\pi/2)^2} = 87.73\ \text{m/s}^2

(Here π2/(2β2)=2\pi^2/(2\beta^2) = 2, so amax=2hω2=2×0.025×1754.6a_{max} = 2h\omega^2 = 2 \times 0.025 \times 1754.6. The same value can be written as h2(πβ)2ω2\dfrac{h}{2}\left(\dfrac{\pi}{\beta}\right)^2\omega^2.)

(a) Maximum inertia force

FI,max=m amax=0.8×87.73=70.18 NF_{I,max} = m\,a_{max} = 0.8 \times 87.73 = 70.18\ \text{N}

It occurs at the beginning of the rise (positive acceleration, so the cam must push) and at the end of the rise (negative acceleration, so the follower tends to leave the cam).

(b) Minimum spring stiffness

At the end of the rise the spring is compressed by the lift hh, and its force there must be at least equal to the inertia force:

F0+k h≥m amaxF_0 + k\,h \ge m\,a_{max} k≥70.18−150.025=2207 N/m≈2.21 N/mmk \ge \frac{70.18 - 15}{0.025} = 2207\ \text{N/m} \approx 2.21\ \text{N/mm}

In practice, a margin of 20 to 50 percent is added.

(c) Maximum force from the cam

At the start of the rise, the spring force is just the preload F0F_0, and the cam must supply the spring force plus the inertia force:

Fcam=mamax+F0=70.18+15=85.2 NF_{cam} = m a_{max} + F_0 = 70.18 + 15 = 85.2\ \text{N}

At any angle, the cam force is N=ma+F0+ksN = m a + F_0 + k s. With the stiffness found above, this reduces to N=42.6(1+cos⁡x)N = 42.6(1 + \cos x) N, where x=πθ/βx = \pi\theta/\beta. So the force falls from its maximum at the start to zero (just touching) at the end of the rise. The spring force at the end of the rise is 70.2 N, equal to the inertia force.

Answer: (a) FI,max=70.18F_{I,max} = 70.18 N; (b) kmin=2207k_{min} = 2207 N/m; (c) Fcam,max=85.2F_{cam,max} = 85.2 N (at the start of the rise).

✓ Answer checked by Claude Opus 5.5 (high effort)

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