180 likes | 189 Vues
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.
E N D
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=?