Concept:
In a slider crank-mechanism,
The piston displacement: \({x_p} = r\left( {1 - \cos θ } \right)\)
Piston velocity: \({v_p} = \omega r\left( {\sin θ + \frac{{\sin 2θ }}{{2n}}} \right)\)
Piston acceleration: \({a_p} = {\omega ^2}r\left( {\cos θ + \frac{{\cos 2θ }}{n}} \right)\), where n is equal to l/r
l length of connecting rod in m and r is crank radius in m.
for maximum acceleration, θ = 0° \({a_{max}} = {\omega ^2}r\left( {1 + \frac{1}{n}} \right)\)
Calculation:
Given, l = r = 300 mm = 0.3 m, ω = 14 rad/s
\({a_{max}} = {\omega ^2}r\left( {1 + \frac{1}{n}} \right)\)
n = 1, as l = r = 0.3 m
thus, \({a_{max}} = {\omega ^2}r\left( {1 + \frac{1}{1}} \right) = 2{\omega ^2}r\)
\({a_{max}} = 2 \times {14^2} \times 0.3 = 117.6\;m/{s^2}\)