MASS MOMENT OF INERTIA (Section 10.9) Today’s Objectives:

Slides:



Advertisements
Similar presentations
MOMENT OF INERTIA Today’s Objectives: Students will be able to:
Advertisements

Today’s Objectives: Students will be able to:
1 ME 302 DYNAMICS OF MACHINERY Dynamic Force Analysis Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.
ENGR 215 ~ Dynamics Section 17.1
MASS MOMENT OF INERTIA (Section 10.9) Today’s Objectives:
I G is the “mass moment of inertia” for a body about an axis passing through the body’s mass center, G. I G is defined as: I G =  r 2 dm Units: kg-m 2.
Thursday, Oct. 23, 2014PHYS , Fall 2014 Dr. Jaehoon Yu 1 PHYS 1443 – Section 004 Lecture #17 Thursday, Oct. 23, 2014 Dr. Jaehoon Yu Torque & Vector.
MOMENT OF INERTIA Today’s Objectives: Students will be able to:
Copyright © 2010 Pearson Education South Asia Pte Ltd
PHYS 1441 – Section 002 Lecture #21 Monday, April 15, 2013 Dr. Jaehoon Yu Moment of Inertia Torque and Angular Acceleration Rotational Kinetic Energy Today’s.
MOMENT OF INERTIA Today’s Objectives: Students will be able to: 1.Determine the mass moment of inertia of a rigid body or a system of rigid bodies. In-Class.
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.
Physics.
9 rad/s2 7 rad/s2 13 rad/s2 14 rad/s2 16 rad/s2
Spring 2002 Lecture #13 Dr. Jaehoon Yu 1.Rotational Energy 2.Computation of Moments of Inertia 3.Parallel-axis Theorem 4.Torque & Angular Acceleration.
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.
CHAPTER 6 PLANAR KINETICS OF A RIGID BODY: FORCE AND ACCELERATION.
Wednesday, Nov. 14, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #20 Wednesday, Nov. 14, 2007 Dr. Jae Yu Moment of Inertia.
Center of Gravity The balance point of an object.
MASS MOMENT OF INERTIA (Section 17.1) Today’s Objectives: Students will be able to Determine the mass moment of inertia of a rigid body or a system of.
Wednesday, Nov. 10, 2004PHYS , Fall 2004 Dr. Jaehoon Yu 1 1.Moment of Inertia 2.Parallel Axis Theorem 3.Torque and Angular Acceleration 4.Rotational.
EQUATIONS OF MOTION: ROTATION ABOUT A FIXED AXIS
MOMENT OF INERTIA Today’s Objectives: Students will be able to:
Statics, Fourteenth Edition R.C. Hibbeler Copyright ©2016 by Pearson Education, Inc. All rights reserved. In-Class Activities: Check homework, if any Reading.
Theoretical Mechanics DYNAMICS * Navigation: Right (Down) arrow – next slide Left (Up) arrow – previous slide Esc – Exit Notes and Recommendations:
Monday, Nov. 4, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #14 Monday, Nov. 4, 2002 Dr. Jaehoon Yu 1.Parallel Axis Theorem.
Mechanics for Engineers: Dynamics, 13th SI Edition R. C. Hibbeler and Kai Beng Yap © Pearson Education South Asia Pte Ltd All rights reserved. MOMENT.
PHYS 1443 – Section 002 Lecture #19
What is Moment of Inertia ( MoI )?
Causes of Rotation Sum the Torques.
COMPOSITE BODIES (Section 9.3)
MOMENTS OF INERTIA FOR AREAS
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
PHYS 1441 – Section 002 Lecture #21
MOMENT ABOUT AN AXIS Today’s Objectives:
MOMENT ABOUT AN AXIS Today’s Objectives:
PHYS 1443 – Section 001 Lecture #14
ROTATION ABOUT A FIXED AXIS
Rotational Inertia.
ROTATION ABOUT A FIXED AXIS
PHYS 1443 – Section 002 Lecture #18
Today’s Objectives: Students will be able to:
COMPOSITE BODIES Today’s Objective:
REDUCTION OF A SIMPLE DISTRIBUTED LOADING
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
MOMENT OF A FORCE SCALAR FORMULATION, CROSS PRODUCT, MOMENT OF A FORCE VECTOR FORMULATION, & PRINCIPLE OF MOMENTS Today’s Objectives : Students will be.
Statics Course Code: CIVL211 Dr. Aeid A. Abdulrazeg
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
PLANAR KINETICS OF A RIGID BODY: CONSERVATION OF ENERGY
Spring 2002 Lecture #15 Dr. Jaehoon Yu Mid-term Results
COMPOSITE BODIES Today’s Objective:
PHYS 1441 – Section 002 Lecture #21
ENGINEERING MECHANICS
CENTER OF GRAVITY, CENTER OF MASS AND CENTROID FOR A BODY
Today’s Objectives: Students will be able to:
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Students will be able to a) define a couple, and,
PLANAR RIGID BODY MOTION: TRANSLATION & ROTATION
MOMENT OF A COUPLE Today’s Objectives: Students will be able to
REDUCTION OF A SIMPLE DISTRIBUTED LOADING
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
MOMENTS OF INERTIA FOR AREAS
MOMENT OF INERTIA Today’s Objectives: Students will be able to:
PHYS 1443 – Section 003 Lecture #14
Students will be able to: a) understand and define moment, and,
MOMENT OF A COUPLE Today’s Objectives: Students will be able to
MOMENT OF A FORCE (Section 4.1)
REDUCTION OF DISTRIBUTED LOADING
EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS
Presentation transcript:

MASS MOMENT OF INERTIA (Section 10.9) Today’s Objectives: Students will be able to : a) Explain the concept of the mass moment of inertia (MMI). b) Determine the MMI of a composite body. In-Class Activities: Check homework, if any Reading quiz Applications MMI: concept and definition Determining the MMI Concept quiz Group problem solving Attention quiz Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

2. The parallel-axis theorem can be applied to determine ________ . READING QUIZ 1. The formula definition of the mass moment of inertia about an axis is ___________ . A)  r dm B)  r2 dm C)  m dr D)  m2 dr 2. The parallel-axis theorem can be applied to determine ________ . A) only the MoI B) only the MMI C) both the MoI and MMI D) None of the above. Note: MoI is the moment of inertia of an area and MMI is the mass moment inertia of a body Answers : 1.B 2.C Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

APPLICATIONS The large flywheel in the picture is connected to a large metal cutter. The flywheel is used to provide a uniform motion to the cutting blade. What property of the flywheel is most important for this use? How can we determine a value for this property? Why is most of the mass of the flywheel located near the flywheel’s circumference? Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

APPLICATIONS (continued) If a torque M is applied to a fan blade which is initially at rest, its angular speed begins to increase. On which property (P) of the fan blade does the angular acceleration () depend? How can we determine a value for P? What is the relationship between M, P, and ? Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

· CONCEPT OF THE MMI G T Consider a rigid body with a center of mass at G. It is free to rotate about the z axis, which passes through G. Now, if we apply a torque T about the z axis to the body, the body begins to rotate with an angular acceleration . T and  are related by the equation T = I  . In this equation, I is the mass moment of inertia (MMI) about the z axis. The MMI of a body is a property that measures the resistance of the body to angular acceleration. This is similar to the role of mass in the equation F = m a. The MMI is often used when analyzing rotational motion (done in dynamics). Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

DEFINITION OF THE MMI p Consider a rigid body and the arbitrary axis p shown in the figure. The MMI about the p axis is defined as I = m r2 dm, where r, the “moment arm,” is the perpendicular distance from the axis to the arbitrary element dm. The MMI is always a positive quantity and has a unit of kg ·m2 or slug · ft2. Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

p’ · RELATED CONCEPTS Parallel-Axis Theorem: Just as with the MoI for an area, the parallel-axis theorem can be used to find the MMI about a parallel axis p’ that is a distance d from the axis through the body’s center of mass G. The formula is Ip’ = IG + (m) (d)2 (where m is the mass of the body). d p’ G · m The radius of gyration is similarly defined as k = (I / m) Finally, the MMI can be obtained by integration or by the method for composite bodies. The latter method is easier for many practical shapes. Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

Plan: Follow steps similar to finding the MoI for a composite area. q EXAMPLE Given: The wheel consists of a thin ring with a mass 10 kg and four spokes (slender rods) with a mass 2 kg each. Find: The wheel’s MMI about an axis perpendicular to the screen and passing through point A. Plan: Follow steps similar to finding the MoI for a composite area. q r p Solution: 1. The wheel can be divided into a thin ring (p) and two slender rods (q and r). Will both rods be treated the same? Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

IAq = IAr = (1/12) (4) (1)2 + 4 (0.5)2 = 1.333 kg·m2 EXAMPLE (continued) p q r 2. The center of mass for each of the three pieces is at point O, 0.5 m from Point A. 3. The MMI data for a thin ring and slender rod are given on the inside back cover of the textbook. Using those data and the parallel-axis theorem, calculate the following. O IA = IO + (m) (d) 2 IAp = 10 (0.5)2 + 10 (0.5)2 = 5.0 kg·m2 IAq = IAr = (1/12) (4) (1)2 + 4 (0.5)2 = 1.333 kg·m2 4. Now add the three MMIs about point A. IA = IAp + IAq + IAr = 7.67 kg·m2 Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

1. Consider a particle of mass 1 kg CONCEPT QUIZ 1. Consider a particle of mass 1 kg located at point P, whose coordinates are given in meters. Determine the MMI of that particle about the z axis. A) 9 kg·m2 B) 16 kg·m2 C) 25 kg·m2 D) 36 kg·m2 z x y ·P(3,4,6) 2. Consider a rectangular frame made of four slender bars with four axes (zP, zQ, zR and zS) perpendicular to the screen and passing through the points P, Q, R, and S respectively. About which of the four axes will the MMI of the frame be the largest? A) zP B) zQ C) zR D) zS E) Not possible to determine. P • S • Q • R Answers: 1.C 2.B Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

Find: The radius of gyration of the pendulum about an axis GROUP PROBLEM SOLVING R Given: The pendulum consists of a 24 lb plate and a slender rod weighing 8 lb. Find: The radius of gyration of the pendulum about an axis perpendicular to the screen and passing through point O. P Plan: Determine the MMI of the pendulum using the method for composite bodies. Then determine the radius of gyration using the MMI and mass values (check units!!). Solution 1. Separate the pendulum into a square plate (P) and a slender rod (R). Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

2. The center of mass of the plate and rod are 3.5 ft and 0.5 ft from GROUP PROBLEM SOLVING P R 2. The center of mass of the plate and rod are 3.5 ft and 0.5 ft from point O, respectively. 3. The MMI data on plates and slender rods are given on the inside cover of the textbook. Using those data and the parallel-axis theorem, IP = (1/12) (24/32.2) (12 + 12) + (24/32.2) (3.5)2 = 9.254 slug·ft2 IR = (1/12) (8/32.2) (5)2 + (8/32.2) (0.5)2 = 0.5797 slug·ft2 4. IO = IP + IR = 9.254 + 0.5797 = 9.834 slug·ft2 5. Total mass (m) equals (24+8)/32.2 = 0.9938 slug Radius of gyration k = IO / m = 3.15 ft Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

2. Consider a rectangular frame made of four ATTENTION QUIZ 1. A particle of mass 2 kg is located 1 m down the y-axis. What are the MMI of the particle about the x, y, and z axes, respectively? A) (2, 0, 2) B) (0, 2, 2) C) (0, 2, 2) D) (2, 2, 0) • 1 m x y z 2. Consider a rectangular frame made of four slender bars and four axes (zP, zQ, zR and zS) perpendicular to the screen and passing through points P, Q, R, and S, respectively. About which of the four axes will the MMI of the frame be the lowest? A) zP B) zQ C) zR D) zS E) Not possible to determine. P • S • Q • R Answers : 1.A 2.D Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9

End of the Lecture Let Learning Continue Statics:The Next Generation Mehta & Danielson Lecture Notes for Section 10.9