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King Fahd University of Petroleum & Minerals

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Presentation on theme: "King Fahd University of Petroleum & Minerals"— Presentation transcript:

1 King Fahd University of Petroleum & Minerals
Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 26

2 Examples of relative motions “motion of one part lead to the
motion of other parts” (pin-connected rigid body)

3 Relative-Motion Analysis :
Relative Velocity Instantaneous Center of Zero Velocity Relative Acceleration

4 Examples of Non-Relative-Motions
)sliding connections and has two independent motion)

5 Position Rotating axes

6 Rotating axes & translating object
Velocity Rotating axes & translating object wr + v

7 Velocity VC = Velocity of the Collar, measured from
the X, Y, Z reference VO = Velocity of the origin O of the x,y,z reference measured from the X,Y,Z reference (VC/O)xyz = relative velocity of “C with respect to O” observer attached to the rotating x,y,z reference = angular velocity of the x,y,z reference, measured from the X,Y,Z reference rC/O = relative position of “C with respect to O”

8 Rotating axes & translating object
Acceleration Acceleration is the time derivative of velocity Rotating axes & translating object (wr + v)

9 Rotating axes & translating object (wr + v)
Acceleration of origin Acceleration of the object w2 r Normal acceleration a r Tangential acceleration Coriolis acceleration

10 Coriolis acceleration
Whenever a point is moving on a path and the path is rotating, there is an extra component of the acceleration due to coupling between the motion of the point on the path and the rotation of the path. This component is called Coriolis acceleration. First measured by the French engineer G.C. Coriolis Important in studying the effect “force and acceleration” of earth rotation on the rockets and long-range projectiles

11

12 In a cylindrical coordinate
Rearrange Compare !

13

14 Recall – Cylindrical coordinate
Coriolis acceleration

15 Example 16-20

16 Thank You


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