Oblique Disc Motion: Hiscox Rod-and-Roller Mechanism

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An oblique disc fixed to a rotating shaft drives a guided rod through a roller. Moving the roller farther from the centre increases the stroke. Explore the arrangement in Hiscox item 1085 and calculate ideal stroke, peak rod speed and revolution period.

Ideal Oblique-Disc Rod Travel

Enter declared roller radius from the disc centre, disc tilt and shaft speed. The worksheet reports the ideal plane-intersection stroke, peak speed and period only; it does not size a swashplate, follower, bearing, pump or compressor.

0°

Ideal full stroke
--
Ideal half-stroke
--
Ideal peak rod speed
--
Shaft revolution period
--

Equation Used

h=R tan(theta); x(phi)=h sin(phi); S=2h; vmax=h(2 pi n/60); trev=60/n
Hiscox establishes variable rectilinear motion by changing roller radius but gives no dimensions. The formula assumes an ideal flat disc plane, constant tilt, continuous contact and axial guidance.
  • The disc is an ideal rigid plane fixed at the declared tilt to a straight rotating shaft.
  • The roller contact lies at declared radius R and the rod is constrained to move only along the shaft axis.
  • Continuous contact is assumed and the motion is sinusoidal at constant shaft speed.
  • Disc thickness, roller radius, preload, friction, slip, Hertz contact, lubrication, wear, bearings, runout, deflection, loads, torque, strength, pump displacement, pressure and safety are excluded.

The ideal rotating-plane model makes stroke proportional to roller distance from the centre. Tilt changes the stroke, while shaft speed changes the calculated velocity and revolution period.

A tilted disc drives a guided rod through a roller

Hiscox item 1085 fixes a disc obliquely on the end of a rotating shaft. A roller follows the disc face while its rod is constrained to rectilinear motion.

Moving the roller farther from the disc centre increases travel. The side projection illustrates the rod and roller following the disc; the calculation assumes continuous contact.

A historical rotary-to-rectilinear mechanism

The mechanism illustrates conversion from rotary to reciprocating motion with adjustable travel. This ideal motion calculation does not determine the loads or contact design needed for a particular machine.

Ideal rotating-plane displacement

h=R tanθ; x(φ)=h sinφ; S=2h; vmax=h(2πn/60); trev=60/n

The result is kinematic only and assumes continuous roller contact with a perfectly flat disc.

Declared geometry example

For R=50 mm, θ=15° and n=20 rpm, ideal half-stroke is 13.40 mm, full stroke is 26.79 mm, peak rod speed is 28.05 mm/s, and one shaft revolution takes 3.000 s.

Motion calculations and contact design

The stroke relation describes an ideal rotating plane and continuously guided contact. A working follower also needs adequate contact force, suitable roller and disc geometry, and support for the applied loads. Those requirements, and any pump or compressor performance, are outside this motion calculation.

Oblique disc-motion questions

Does changing roller radius change stroke?

Yes, linearly in this ideal plane model.

Does the calculator size a pump or compressor?

No.

Is animation speed the entered rpm?

No. The display is slowed for inspection; the numeric velocity and period use the entered rpm.

Oblique disc-motion reference

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