Question #227520

In a slider crank mechanism, the length of the crank and connecting rod are 100 mm and 400 mm respectively. The crank rotates uniformly at 600 r.p.m. clockwise. When the crank has turned through 45° from the inner dead centre, find, by analytical method : a. Velocity and acceleration of the slider. b. Angular velocity and angular acceleration of the connecting rod. Check your result by Klein’s or Bennett’s construction. 



Expert's answer

CN=rsinθ=lsinϕ    sinϕ=rlsinθCN = r sin \theta = l sin \phi \implies sin \phi = \frac{r}{l} sin \theta

sinϕ=sinθn    n=lrsin \phi = \frac{sin \theta}{n} \implies n=\frac{l}{r}

We know that sin2ϕ+cos2ϕ=1    1sin2ϕn2sin^2 \phi+cos^2 \phi=1 \implies \sqrt{1-\frac{sin^2 \phi}{n^2}}

Xp=r(1cosθ)+l(11sin2ϕn2)X_p=r(1-cos \theta )+l(1-\sqrt{1-\frac{sin^2 \phi}{n^2}})

Xp=r(1cosθ)+r(nn2sin2θ)X_p=r(1-cos \theta )+r(n-\sqrt{n^2-sin^2 \theta})

Velocity Since the velocity of the slider is rate of change of displacement with respect to time

Vp=d(Xp)dt=ddθdθdt(Xp)V_p= \frac{d(X_p)}{dt}= \frac{d}{d\theta} \frac{d \theta}{dt} (X_p)

Vp=d(Xp)dt=ddθdθdt(r(1cosθ)+r(nn2sin2θ))V_p= \frac{d(X_p)}{dt}= \frac{d}{d\theta} \frac{d \theta}{dt} (r(1-cos \theta )+r(n-\sqrt{n^2-sin^2 \theta}))

Vp=ωrdθdt(r(1cosθ)+r(nn2sin2θ))V_p= \omega r \frac{d \theta}{dt} (r(1-cos \theta )+r(n-\sqrt{n^2-sin^2 \theta}))

Vp=ωr[sinθ+sinθ2n2sin2θ]V_p= \omega r [sin \theta+ \frac{sin \theta}{2* \sqrt{n^2-sin^2 \theta}}]




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