Peaucellier-Lipkin Linkage: Exact Straight-Line Inversor

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The Peaucellier-Lipkin linkage transforms a circular arc into a straight path through geometric inversion. A rhombus of equal links and two longer links keep the product of two distances constant. Explore the motion and calculate its line offset and ideal stroke.

Peaucellier-Lipkin Exact-Closure Explorer

Set the two cell-link lengths, the driver-circle radius and angular sweep. Every bar remains rigid while inverse point Q traces the exact output line.

0°

Inversion constant
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Exact line offset
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Ideal output stroke
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Input-circle diameter
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Equation Used

k=a^2-b^2=OP times OQ; xQ=k/(2c); strokeQ=2xQ tan(alpha/2)
The driver point P moves on a circle of radius c centered c from O. Because that circle passes through O, its inverse Q has constant x-coordinate k/(2c).
  • The two links from fixed center O to opposite cell pivots are equal length a.
  • The four rhombus links are equal length b, with a greater than b.
  • The driver link CP and fixed spacing OC both equal c.
  • All links are ideal rigid planar members with perfect pivots.
  • Force, stress, clearance, tolerance, friction, speed, interference and safety are excluded.

The input point moves on a circle through the inversion center, giving a straight path for the output point. Results assume ideal links and pivots; folded positions where P and Q coincide need a separate singularity check.

Eight rigid links form an exact geometric inversor

Cornell's Reuleaux collection identifies the Peaucellier-Lipkin mechanism as an eight-link exact straight-line linkage. Four equal links form the rhombus cell, and two equal longer links connect its side pivots to fixed inversion center O.

The cell enforces OP times OQ equals a squared minus b squared. Constraining P to a circle through O therefore constrains inverse point Q to one exact straight line.

Historical exact straight-line motion

Cornell records applications in steam-engine pressure indicators and machine tools. The linkage is historically important because it produces mathematically exact straight-line motion from revolute joints.

This explorer demonstrates ideal geometry; it does not size an actuator, machine joint or loaded mechanism.

Inversion constant and line position

k=a^2-b^2=OP times OQ; xQ=k/(2c)

For a driver circle of radius c whose center is c from O, OP squared equals 2c times the horizontal coordinate of P. Inversion sends P to Q=kP/OP squared, so Q has constant horizontal coordinate k/(2c).

Declared exact example

For a=280 mm, b=200 mm and c=140 mm, k=38,400 mm squared and the exact output line is 137.143 mm from O. A plus-or-minus 65-degree driver swing gives 174.74 mm of ideal straight-line output stroke.

Exact ideal theorem, separate real tolerances

The mathematical result is exact only for rigid links of exact length and perfect planar pivots. A real design needs a configuration-dependent tolerance, stiffness, bearing, interference and load analysis.

Calculating departure from a straight line requires the actual link and pivot errors and their effect through the stroke. This explorer reports ideal geometric results and does not check singularity avoidance.

Peaucellier-Lipkin questions

Why is the output exact?

The linkage makes Q the geometric inverse of P, and inversion maps a circle through O to a straight line.

What stays constant?

OP times OQ equals a squared minus b squared.

Do any bars stretch?

No. All six cell links and the circular driver remain rigid in the animation.

Does exact theory predict manufacturing error?

No. Real error requires a separate tolerance and compliance model.

Peaucellier-Lipkin references

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