King Fahd University of Petroleum & Minerals

Slides:



Advertisements
Similar presentations
MAE 242 Dynamics – Section I Dr. Kostas Sierros. Problem 1.
Advertisements

“Dynamics by Hibbeler,” Dr. S. Nasseri, MET Department, SPSU Today’s Objectives: Students will be able to: 1.Apply the three equations of motion for a.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 9.
RIGID BODY MOTION: TRANSLATION & ROTATION (Sections )
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 3.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 25.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 40.
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 7.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 16.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 27.
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 21.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 6.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 39.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 32.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 8.
ENGR 215 ~ Dynamics Sections 16.1 – Rigid Body Motion When all the particles of a rigid body move along paths which are equidistant from a fixed.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 17.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 38.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 29.
KINETIC ENERGY, WORK, PRINCIPLE OF WORK AND ENERGY
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 27.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 35.
Plane Motion of Rigid Bodies: Forces and Accelerations
MAE 242 Dynamics – Section I Dr. Kostas Sierros.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 13.
King Fahd University of Petroleum & Minerals
5.Kinematics of Particles
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 5.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 30.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 18.
EQUATIONS OF MOTION: ROTATION ABOUT A FIXED AXIS Today’s Objectives: Students will be able to: 1.Analyze the planar kinetics of a rigid body undergoing.
Apply the three equations of motion for a rigid body in planar motion. Analyze problems involving translational motion. PLANAR KINETIC EQUATIONS OF MOTION:
Today’s Objectives: Students will be able to: a)Apply the three equations of motion for a rigid body in planar motion. b)Analyze problems involving translational.
KINETIC ENERGY, WORK, PRINCIPLE OF WORK AND ENERGY
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 21.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 15.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 10.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 37.
King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 28.
Chapter 17 Rigid Body Dynamics. Unconstrained Motion: 3 Equations for x, y, rotation.
KINETIC ENERGY, WORK, PRINCIPLE OF WORK AND ENERGY Today’s Objectives: Students will be able to: 1.Define the various ways a force and couple do work.
KINETICS of PARTICLES Newton’s 2nd Law & The Equation of Motion
ROTATION ABOUT A FIXED AXIS
ROTATION ABOUT A FIXED AXIS
King Fahd University of Petroleum & Minerals
ดร. พิภัทร พฤกษาโรจนกุล
KINETIC ENERGY, WORK, PRINCIPLE OF WORK AND ENERGY
King Fahd University of Petroleum & Minerals
PLANAR KINETIC EQUATIONS OF MOTION:
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
MEE 214 (Dynamics) Tuesday
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
PLANAR KINETIC EQUATIONS OF MOTION:
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
King Fahd University of Petroleum & Minerals
Presentation transcript:

King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 33

General Application of the Equations of Motion Summation of moment in FBD = summation of the kinetic moment in K.D

Rectilinear Translation

Curvilinear Translation

Example mm=125 kg mR= 75 kg a= ? NB=? FB=? ms=? Minimum to Lift front wheel

Problem m = 80 kg mB= 0.8 NA= ? NB= ? When rear wheel locks for break a = ? Deceleration aG mBNB NA NB

Problem m= 80 kg mB= ? NA=? NB=? a =? When traveling at constant velocity and no break was applied NA NB mBNB a = 0

Problem m= 80 kg NA=? NB=? a =? mk=? minimum When rider applies the front break and back wheel start to lift off the ground NA NB=0 mkNA

Example mBD=100kg mAB=mCD= Neglect q = 30o w = 6 rad/s TA= ? TD= ? aG=?

Rotation About a Fixed Axis

Pin Reaction Horizontal Reaction Vertical Reaction OR Normal Reaction Tangential Reaction If G&O are same use horizontal and vertical If G&O are not same use normal and tangential On Ot Ox On Oy Ot

Example 17-9 Start from rest m = 30 kg w=20rad/s Pin reaction? q=? Number

Example 17-10 m= 20 kg

Example 17-11 m=60 kg Radius of gyration kO=0.25 mb=20 kg a=? Drum a=?

Example 17-12 W=50 Ib kG=0.6 ft w= 8 rad/s Pin reaction =?

Thank you