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This lecture covers the application of equations of translation and rotation motion, center of mass role, slipping vs. tipping scenarios, and practical examples. Discusses concepts like wheely vs. non-wheely and provides detailed examples on motion problems.
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King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 31
Objectives • Apply the Equation of Translation motion • Rectilinear Translation • Curvilinear Translation • Apply the equation of Rotation motion • The roll of the center of mass G • Discuss the slipping Vs. Tipping • Discuss the slipping Vs. freely rotating • Discuss the “wheely” Vs. Non-wheely
General Application of the Equations of Motion Summation of moment in FBD = summation of the kinetic moment in K.D
x N slipping Vs. Tipping If x > 1.5 ft tipping If x < 1.5 ft slipping
Slipping Vs. Freely rotating Front wheel Vs Back wheel drive Vs Four wheel drive mg FA=msNA NA NB slipping Freely Rotating
“Wheely” Vs. Non-Wheely Wheely : lift the front wheel off the ground NB=0
Example mk=0.2 a= ? Flip Or Tipp? If x > 0.5 m tipping will take place
Example mm=125 kg mR= 75 kg a= ? NB=? FB=? ms=? Minimum to Lift front wheel
Problem aG mBNB NA NB m = 80 kg mB= 0.8 NA= ? NB= ? When rear wheel locks for break a = ? Deceleration
Problem a = 0 mBNB NA NB m= 80 kg mB= ? NA=? NB=? a =? When traveling at constant velocity and no break was applied
Problem mkNA NA NB=0 m= 80 kg NA=? NB=? a =? mk=? minimum When rider applies the front break and back wheel start to lift off the ground
Example mBD=100kg mAB=mCD= Neglect q = 30o w = 6 rad/s TA= ? TD= ? aG=?