| Hello everyone, 👋 Welcome back to Motion Monday! This time for real 😁 , Recently I saw an interesting kinematic combination — the inverted slider crank in series with a slider crank — and thought of sharing a quick note on it.
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In this mechanism, there are 4 rigid links, 3 lower pairs (surface contact), and 2 higher pairs (point or line contact).
Using Gruebler’s equation for planar mechanisms:
DOF=3(n−1)−2L−H
| DOF=3(n−1)−2L−H |
where
- n = number of links
- L = number of lower pairs
- H = number of higher pairs
Substituting the values:
| DOF=3(4−1)−2(3)−2 |
| DOF=9−6−2 |
| DOF=1 |
This means the mechanism has one degree of freedom, and its motion can be completely controlled by a single input, i.e. the rotation of the crank.
Motion transformation in the mechanism:
- Input: Rotary motion (360 Degrees, 100 rpm)
- Intermediate: Oscillatory motion (angular displacement θ=61.78 degrees)
- Output: Reciprocating motion (slider displacement 154.5mm)
To Play with the motion yourself you can download SOLIDWORKS file from below.
