Start with a question
How can a turning handle make a block slide back and forth?
Machines often need to change one kind of movement into another. A turning handle can drive a pump that pushes and pulls in a straight line.
Before you start: No mechanics knowledge is needed. First meet three parts, then follow one movement. The model shows motion; it does not simulate a running engine.
Your goal: Explain how the turning arm, connecting rod and straight guide make the piston move out and back.
A turn and a slide are different movements
A point on a turning arm travels around its fixed center. A sliding block moves along a straight path. Joining them needs a link that can change its angle while staying the same length.
Meet the three working parts
The crank is the turning arm. A pin near its end joins it to the connecting rod. The rod’s other end joins the piston, the sliding block. Both joints let the rod pivot, like a hinge, instead of forcing the piston to follow a circle.
The guide keeps the piston on one path
The cylinder is the fixed guide around the piston. It keeps the piston moving along one straight line. Because the rod does not stretch, the changing position of the crank pin makes the piston move closer to the crank and then farther away.
Words you’ll see
- Crank
- The arm that turns about a fixed center; its outer pin travels around that center.
- Connecting rod
- A rigid link that joins the turning pin to the piston. Its joints let it tilt.
- Piston
- The block that slides inside the cylinder. One trip from one end of its path to the other is called a stroke.
Now match the three numbered parts to their names. Follow the guided turn, make a prediction, then explore the controls if you want to try a different movement.
Watch the connection
Find the turning arm, the link and the sliding block
Match the numbers on the model to the names below it: 1 is the crank, 2 is the connecting rod, and 3 is the piston. The short crank turns about its fixed center. Start by watching its outer pin.
Guided first turn · 1 of 4
A full turn is 360°. A quarter turn is 90°. The distance unit mm means millimetres.
Reduced motion is on. Use Step or the angle control to inspect still positions.
Experiment: change how far the crank reaches
A crank’s radius is the distance from its fixed center to the outer pin. A stroke is one trip between the piston’s two end positions. Keep the rod’s length unchanged and compare the stroke with a different radius.
Crank radiusKeep the 110 mm rod fixed. Compare the stroke with a different crank radius.
Saved front-section drawings show the same quarter-turn positions. Use Step to follow the mechanism.
How far does the piston move?
A stroke is one trip between the piston’s two end positions. The crank’s radius is the distance from its center to its outer pin. We measure distance in millimetres, written mm.
At one end, the crank pin reaches one radius toward the piston. Half a turn later, it points one radius in the other direction. Those positions are two radii apart. The rod has the same length at both ends, so the piston’s stroke is twice the crank radius. A larger radius makes a longer stroke in this straight, in-line arrangement.
Worked example: a 30 mm crank radius gives a 30 + 30 = 60 mm stroke. A full turn gives one 60 mm inward trip and one 60 mm return trip: two strokes, with 120 mm of total travel.
0° · Farthest from the crank
180° · Closest to the crank
Optional: the geometry and model assumptions
You do not need this equation for the lesson. L is the rod length (110 mm), r is the crank radius, θ is the crank’s turn angle, and x is the distance along the piston’s path from the shaft center to the piston’s joint.
The rod’s horizontal reach is √(L² − r² sin² θ). Adding the crank pin’s horizontal position gives x = r cos θ + √(L² − r² sin² θ). At the two ends, x is L + r and L − r, so the difference is 2r. The drawing and readout use this geometry.
An ideal in-line slider–crank with a rigid 110 mm connecting rod. Playback is deliberately slow. The cutaway exposes the joints; this lesson models motion, not combustion, friction, forces, inertia, or manufacturing tolerances.
Reference: MIT OpenCourseWare · Machine Elements, slider–crank kinematics (PDF).
