Applied Mechanics Embracing Strength And Elasticity of Materials Theory And De

Cover Applied Mechanics Embracing Strength And Elasticity of Materials Theory And De
Applied Mechanics Embracing Strength And Elasticity of Materials Theory And De
David Allan Low
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The Angular Velocity J Time Curve.
BD = Cd=Ce =FE = BE B D = Angular Veloaty\ of Connecting - rod J FIG, 477.
different values of > corresponding to different values of are readily obtained by the construction shown, and which may be briefly described as follows. With C as centre, and radius equal to the length of the connecting-rod, measured on the linear scale, describe the arc 0'3'. Let CB be one position of the crank. Draw BB' parallel to CO' to meet 0'3' at B'. Join CB', then angle B'CO' =
... >. Draw BD parallel to B'C to meet the perpendicular to CO' from C at D. Then BD represents the angular velocity of the connecting-rod when the crank is at CB. Make, on B'C, B"E = BD. Then E is a point on a polar curve of angular velocity of connecting-rod. If Cd = BD be marked off on B'C from C as a pole, then d is a point on another polar curve of angular velocity of connecting-rod. Observe that when BD is positive B'E is measured from the arc 0'3' on the side opposite to C, and when negative it is measured from the arc 0'3' towards C.

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