Slider-Crank Mechanism - Part 3

Consider the mechanism shown in the figure. The system comprises two rigid rods named 1 1 and 2 2 respectively. The point mass numbered as 3 3 can only translate along the X-axis. The bodies are linked by using appropriate hinges and joints.

O A = 0.15 m OA = 0.15 \ m A B = 0.4 m AB = 0.4 \ m A O B = θ \angle AOB = \theta

The centers of mass of rods lie at their geometric center. At the following instant: θ = π 3 r a d \theta = \frac{\pi}{3} \: rad θ ˙ = 12 π r a d / s \dot{\theta} = -12\pi \: rad/s

The solver is required to find the point on body 2 2 which has minimum speed. Enter your answer as the distance from point A A along the length of the rod A B AB .

Note:

  • The small circles and triangles just indicate joints between bodies.
  • The negative sign of θ ˙ \dot{\theta} indicates a clockwise rotation of body 1 about O.
  • Body 3, even though depicted as a rectangle is just a point mass.
  • The motion of the system is confined to the X-Y plane.


The answer is 0.1450.

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1 solution

Steven Chase
Sep 10, 2019

Let ( x , y ) (x,y) be a point on rod 2 2 . The following relation generally holds:

x = x A + α ( x B x A ) y = y A + α ( y B y A ) 0 α 1 x = x_A + \alpha(x_B - x_A) \\ y = y_A + \alpha(y_B - y_A) \\ 0 \leq \alpha \leq 1

Time-differentiating gives:

x ˙ = x ˙ A + α ( x ˙ B x ˙ A ) y ˙ = y ˙ A + α ( y ˙ B y ˙ A ) 0 α 1 \dot{x} = \dot{x}_A + \alpha(\dot{x}_B - \dot{x}_A) \\ \dot{y} = \dot{y}_A + \alpha(\dot{y}_B - \dot{y}_A) \\ 0 \leq \alpha \leq 1

The speed is:

v = x ˙ 2 + y ˙ 2 v = \sqrt{\dot{x}^2 + \dot{y}^2}

For point A A :

x A = O A cos θ y A = O A sin θ x ˙ A = O A sin θ θ ˙ y ˙ A = O A cos θ θ ˙ x_A = OA \, \cos \theta \\ y_A = OA \, \sin \theta \\ \dot{x}_A = -OA \, \sin \theta \, \dot{\theta} \\ \dot{y}_A = OA \, \cos \theta \, \dot{\theta}

For point B B (from the previous problem):

x ˙ B 5.868 y ˙ B = 0 \dot{x}_B \approx 5.868 \\ \dot{y}_B = 0

So we know the velocities of the two ends points. All that remains is to sweep the parameter α \alpha and see which value yields the smallest speed. As it turns out, α 0.3625 \alpha \approx 0.3625 yields the smallest speed, corresponding to a length of 0.145 \approx 0.145 from point A A .

Thanks for the solution. Another way in which this can be approached is by computing the square of the speed as a function of α \alpha and equating its derivative (with respect to α \alpha ) to zero. This would be an analytical method.

Karan Chatrath - 1 year, 9 months ago

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Indeed, I considered that. But laziness prevailed, as it often does. This has turned into a nice problem series

Steven Chase - 1 year, 9 months ago

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I understand, and thanks! I am still contemplating whether I should post a dynamics variant of this. Thinking of something insightful and yet not too tedious in terms of calculations. I'll post one when I do have an idea.

Karan Chatrath - 1 year, 9 months ago

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