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ME321 Kinematics and Dynamics of Machines

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Presentation on theme: "ME321 Kinematics and Dynamics of Machines"— Presentation transcript:

1 ME321 Kinematics and Dynamics of Machines
Steve Lambert Mechanical Engineering, U of Waterloo 9/23/2018

2 Kinematics and Dynamics
Position Analysis Velocity Analysis Acceleration Analysis Force Analysis We will concentrate on four-bar linkages 9/23/2018

3 Velocity Analysis Can use vector methods or instantaneous centres
Vector equations can be expressed in general form, or specialized for planar problems Graphical Solutions Vector Component Solutions Complex Number Solutions 9/23/2018

4 Vector Equations 9/23/2018

5 Vector Equations for Velocity
Differentiate Position Vector with respect to Time 9/23/2018

6 Vector Velocity Equation
Where: = Total absolute velocity of point = Absolute velocity of local origin = Relative velocity in local system = Angular velocity of Local System = Position of point in local system 9/23/2018

7 Planar Velocity Equations
Assume: Motion is restricted to the XY plane Local frame is aligned with and fixed to link Therefore:  becomes the angular velocity of the link 9/23/2018

8 Planar Velocity Equations
Becomes: 9/23/2018

9 Application to Four-Bar Linkages
9/23/2018

10 Graphical Solution 9/23/2018

11 Velocity Image A’B’ is the velocity image of link AB
And then the velocity of point C, VC, can be obtained directly from the figure as the vector O’C’ 9/23/2018

12 Vector Component Solution
But: and Giving: or: 9/23/2018

13 Instant Centres An instant centre is a point at which there is no relative velocity between two links in a mechanism, at a particular instant in time 9/23/2018

14 Kennedy’s Theorem Kennedy’s theorem states: the three instant centres of three bodies moving relative to one another must lie along a straight line. 9/23/2018

15 Kennedy’s Theorem 9/23/2018

16 Instant Centre Velocity Analysis
9/23/2018


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