1 ME 302 DYNAMICS OF MACHINERY Dynamic Force Analysis III Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.

Slides:



Advertisements
Similar presentations
Lectures D25-D26 : 3D Rigid Body Dynamics
Advertisements

Lecture D31 : Linear Harmonic Oscillator
Two-Dimensional Unsteady Planing Elastic Plate Michael Makasyeyev Institute of Hydromechanics of NAS of Ukraine, Kyiv.
ME 302 DYNAMICS OF MACHINERY
ME 302 DYNAMICS OF MACHINERY
1 ME 302 DYNAMICS OF MACHINERY Cam Dynamics Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.
Periodic motion Frequency Period. Periodic motion – Any motion that repeats itself.
ME 302 DYNAMICS OF MACHINERY
8.0 SECOND MOMENT OR MOMENT OF INERTIA OF AN AREA
Lecture 2 Free Vibration of Single Degree of Freedom Systems
1 ME 302 DYNAMICS OF MACHINERY FRICTION FORCE Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.
1 ME 302 DYNAMICS OF MACHINERY Virtual Work-Energy Methods Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.
1 ME 302 DYNAMICS OF MACHINERY Dynamic Force Analysis Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu.
Chapter 5 Rotation of a Rigid Body. §5-5 Angular Momentum of a rigid Body Conservation of Angular Momentum §5-1 Motion of a Rigid body §5-2 Torque The.
ENGR 215 ~ Dynamics Section 17.1
Constraints. Pendulum Tension  The Newtonian view is from balanced forces. Tension balances radial component of gravity  The tension force is conservative.
Mechanical Vibrations
1 Lecture #5 of 25 Moment of inertia Retarding forces Stokes Law (viscous drag) Newton’s Law (inertial drag) Reynolds number Plausibility of Stokes law.
ME 482: Mechanical Vibrations (062) Dr. M. Sunar.
Rigid Bodies Rigid Body = Extended body that moves as a unit Internal forces maintain body shape Mass Shape (Internal forces keep constant) Volume Center.
Rotational Motion. The Effect of Torque  A tangential force on a mass creates an acceleration. Tangential force: F t = m a tTangential force: F t = m.
The simple pendulum Energy approach q T m mg PH421:Oscillations F09
Dynamic Equilibrium. Orbital Potentials  Kepler orbits involve a moving system. Effective potential reduces to a single variable Second variable is cyclic.
Torque and Simple Harmonic Motion Week 13D2 Today’s Reading Assignment Young and Freedman:
Harmonic Motion AP Physics C.
Taylor Series.
Computer Assisted Laboratory Experiments in Mechanics Roman Kezerashvili New York City Technical College The City University of New York.
NAZARIN B. NORDIN What you will learn: Load transfer, linear retardation/ acceleration Radius of gyration Moment of inertia Simple.
… constant forces  integrate EOM  parabolic trajectories. … linear restoring force  guess EOM solution  SHM … nonlinear restoring forces  ? linear.
Chapter 12: Forces and Motion
Oscillators fall CM lecture, week 4, 24.Oct.2002, Zita, TESC Review simple harmonic oscillators Examples and energy Damped harmonic motion Phase space.
1 Honors Physics 1 Class 18 Fall 2013 Harmonic motion Unit circle and the phasor Solution to the spring differential equation Initial and boundary conditions.
Advanced Higher Mechanics Linear and Parabolic Motion Mathematical Techniques for Mechanics Force, Energy and Periodic Motion AH.
Chapter 5: Double and Triple Integrals I. Review Q1 & Q2 from preclass Ch. 5- Double and Triple Integrals > Review.
Chapter 11: Rotational Dynamics  As we did for linear (or translational) motion, we studied kinematics (motion without regard to the cause) and then dynamics.
Torque Calculations with Pulleys
MAT 1228 Series and Differential Equations Section 3.7 Nonlinear Equations
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.
Simple Harmonic Motion: SHM
1 Honors Physics 1 Summary and Review - Fall 2013 Quantitative and experimental tools Mathematical tools Newton’s Laws and Applications –Linear motion.
8.0 SECOND MOMENT OR MOMENT OF INERTIA OF AN AREA
1/61/6 M.Chrzanowski: Strength of Materials SM1-08: Continuum Mechanics: Stress distribution CONTINUUM MECHANICS (STRESS DISTRIBUTION)
Engineering Applications using MATLAB
Oscillations Different Situations.
What is called vibration Analysis Design
Differential Equations Linear Equations with Variable Coefficients.
Copyright Kaplan AEC Education, 2008 Calculus and Differential Equations Outline Overview DIFFERENTIAL CALCULUS, p. 45 Definition of a Function Definition.
A Differential Equation is said to be linear if the dependent variable and its differential coefficient occur in it in the first degree only and are not.
… constant forces  integrate EOM  parabolic trajectories. … linear restoring force  guess EOM solution  SHM … nonlinear restoring forces  ? linear.
Oscillations By M.P.Chaphekar. Types Of Motion 1.Translational Motion 2. Rotational Motion 3. Oscillatory Motion.
1 10. Harmonic oscillator Simple harmonic motion Harmonic oscillator is an example of periodic motion, where the displacement of a particle from.
Units of N/m m 2 = N m = J  Total potential energy is Example: Problem A block (m = 1.7 kg) and a spring (k = 310 N/m) are on a frictionless incline.
PRIOR READING: Main 1.1, 2.1 Taylor 5.1, 5.2 SIMPLE HARMONIC MOTION: NEWTON’S LAW
Lab 10: Simple Harmonic Motion, Pendulum Only 3 more to go!!  mg T length = l A B C mg T T -mgsin  -mgcos  The x-component of the weight is the force.
Course Outline Course Outline Exam topics MATLAB tutorial
PHYS 1443 – Section 003 Lecture #22
Simple and Compound Pendulum
Mechanical Vibrations
CHAPTER III LAPLACE TRANSFORM
Advanced Higher Mechanics
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  kx
BTE 1013 ENGINEERING SCIENCES
Oscillations AP Physics C.
Physics 111 Practice Problem Solutions 14 Oscillations SJ 8th Ed
Use power series to solve the differential equation. {image}
Today (2/23/16) Learning objectives:
73 – Differential Equations and Natural Logarithms No Calculator
Differential Equations
Systems of Equations Solve by Graphing.
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  -kx
Presentation transcript:

1 ME 302 DYNAMICS OF MACHINERY Dynamic Force Analysis III Dr. Sadettin KAPUCU © 2007 Sadettin Kapucu

Gaziantep University 2 Measuring Mass Moment of Inertia If the boundaries (surfaces) of the volume is well defined mathemetically, we calculate Mass Moment of Inertia by integration. if this is not possible and a specimen exist, we move it and measure the motion. Motion is related to the mass moment of inertia. O G  G

Gaziantep University 3 Measuring Mass Moment of Inertia by Compound Pendulum Differential equation of motion of the compound pendulum. This is a second order nonlinear differential equation. To ease the solution this equation must be linearized which can be linearized by using Taylor series expansion then O G  mg mgsin  mgcos  rGrG

Gaziantep University 4 Measuring Mass Moment of Inertia by Compound Pendulum Where A&B are arbitrary coefficient related with the initial values of the motion t is time  n is natural circular frequency O G  mg mgsin  mgcos  rGrG nn

Gaziantep University 5 Measuring Mass Moment of Inertia by Compound Pendulum When O G  mg mgsin  mgcos  rGrG

Gaziantep University 6 Measuring Mass Moment of Inertia by Compound Pendulum 1 cycle Elapsed time for one cycle is called period 

Gaziantep University 7 Measuring Mass Moment of Inertia by Compound Pendulum Procedure Measure time; say 20 cycles by a stopwach. Calculate one period by dividing this time into 20, which minimize the personal mistakes. With only unknown I 0

Gaziantep University 8 Measuring Mass Moment of Inertia by Torsional Pendulum Differential equation of motion of the Torsional pendulum.  k  With only unknown I 0

Gaziantep University 9 Measuring Mass Moment of Inertia by Filar Pendulum mg   mg/2  0.5mgcos  0.5mgsin  G G b l

Gaziantep University 10 Measuring Mass Moment of Inertia by Filar Pendulum mg   mg/2 G G b l

Gaziantep University 11 Measuring Mass Moment of Inertia by Filar Pendulum mg   mg/2 G G b l