King Fahd University of Petroleum Minerals Mechanical Engineering

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King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr.

King Fahd University of Petroleum & Minerals Mechanical Engineering Dynamics ME 201 BY Dr. Meyassar N. Al-Haddad Lecture # 35

Objective • • Moment of Inertia of a body Parallel Axis Theorem Radius of

Objective • • Moment of Inertia of a body Parallel Axis Theorem Radius of Gyration Moment of Inertia of Composite Bodies

Parallel Axis Theorem • The moment of inertia about any axis parallel to and

Parallel Axis Theorem • The moment of inertia about any axis parallel to and at distance d away from the axis that passes through the centre of mass is: • Where – IG= moment of inertia for mass centre G – m = mass of the body – d = perpendicular distance between the parallel axes.

Radius of Gyration

Radius of Gyration

Mass Center Example

Mass Center Example

Objectives • Apply the Equation of Translation motion – Rectilinear Translation – Curvilinear Translation

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

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

Rectilinear Translation

Rectilinear Translation

Curvilinear Translation

Curvilinear Translation

Discuss the slipping Vs. Tipping If x > 1. 5 ft tipping If x

Discuss the slipping Vs. Tipping If x > 1. 5 ft tipping If x < 1. 5 ft slipping x N

Slipping Vs. Freely rotating mg FA=ms. NA NA NB

Slipping Vs. Freely rotating mg FA=ms. NA NA NB

“Wheely” Vs. Non-Wheely : lift the front wheel off the ground NB=0

“Wheely” Vs. Non-Wheely : lift the front wheel off the ground NB=0

Example 17 -5

Example 17 -5

Example 17 -8 m. BD=100 kg m. AB=m. CD= Neglect q = 30 o

Example 17 -8 m. BD=100 kg m. AB=m. CD= Neglect q = 30 o w = 6 rad/s TA= ? TB= ? a. G=?

Problem 17 -43 m= 80 kg m. B=0. 8 NA=? NB=? When rear wheel

Problem 17 -43 m= 80 kg m. B=0. 8 NA=? NB=? When rear wheel locks for break a =? Deceleration a. G m. BNB NA NB

Problem 17 -43 m= 80 kg m. B=0. 8 NA=? NB=? a =? When

Problem 17 -43 m= 80 kg m. B=0. 8 NA=? NB=? a =? When traveling at constant velocity and no break was applied a=0 m. BNB NA NB

Problem 17 -44 m= 80 kg NA=? NB=? a =? mk=? minimum When rider

Problem 17 -44 m= 80 kg NA=? NB=? a =? mk=? minimum When rider applies the front break and back wheel start to lift off the ground mk NA NA NB=0

Rotation About a Fixed Axis

Rotation About a Fixed Axis

Rotation About a Fixed Axis

Rotation About a Fixed Axis

Horizontal Reaction Vertical Reaction OR Normal Reaction Tangential Reaction Pin Reaction Ox On Oy

Horizontal Reaction Vertical Reaction OR Normal Reaction Tangential Reaction Pin Reaction Ox On Oy On Ot Ot

Example 17 -9 Start from rest q=? Number w=20 rad/s Pine reaction

Example 17 -9 Start from rest q=? Number w=20 rad/s Pine reaction

Example 17 -10

Example 17 -10

Example 17 -11 m=60 kg Radius of gyration k. O=0. 25 mb=20 kg a=?

Example 17 -11 m=60 kg Radius of gyration k. O=0. 25 mb=20 kg a=? Drum a=?

Example 17 -12 W=50 Ib k. G=0. 6 ft w= 8 rad/s Pin reaction

Example 17 -12 W=50 Ib k. G=0. 6 ft w= 8 rad/s Pin reaction =?

Frictional Rolling Problems - rolls without slipping - slides as it rolls

Frictional Rolling Problems - rolls without slipping - slides as it rolls

Example 17 -14 m = 8 Kg radius of gyration k. G=0. 3 m.

Example 17 -14 m = 8 Kg radius of gyration k. G=0. 3 m. a=? .

Example 17 -15 W= 50 -lb radius of gyration k. G=0. 70 ft. a.

Example 17 -15 W= 50 -lb radius of gyration k. G=0. 70 ft. a. G=? .

Example 17 -16 m=100 kg IG=75 kg. m 2 a=? The pole at rest

Example 17 -16 m=100 kg IG=75 kg. m 2 a=? The pole at rest

Example 17 -17

Example 17 -17