Estimation of Fundamental Natural Frequency, Damping Ratio and Equivalent Mass 421L/521L (Lab 8)

Slides:



Advertisements
Similar presentations
Lecture 2 Free Vibration of Single Degree of Freedom Systems
Advertisements

DISPLACEMENT TRANSMISSIBILITY IN BASE EXCITATION
Lecture 2 Free Vibration of Single Degree of Freedom Systems
Dr. Adnan Dawood Mohammed (Professor of Mechanical Engineering)
MAK4041-Mechanical Vibrations
1 Fifth Lecture Dynamic Characteristics of Measurement System (Reference: Chapter 5, Mechanical Measurements, 5th Edition, Bechwith, Marangoni, and Lienhard,
ME 482: Mechanical Vibrations (062) Dr. M. Sunar.
ME 322: Instrumentation Lecture 30 April 6, 2015 Professor Miles Greiner.
VIBRATION MEASURING DEVICES
Oscillation.
1 HOMEWORK 1 1.Derive equation of motion of SDOF using energy method 2.Find amplitude A and tanΦ for given x 0, v 0 3.Find natural frequency of cantilever,
S1-1 SECTION 1 REVIEW OF FUNDAMENTALS. S1-2 n This section will introduce the basics of Dynamic Analysis by considering a Single Degree of Freedom (SDOF)
HOMEWORK 01C Eigenvalues Problem 1: Problem 2: Problem 3: Problem 4: Lecture 1 Problem 5: Problem 6:
Mechanical Vibrations
Fiber-Optic Accelerometer Using Wavefront-Splitting Interferometry Hsien-Chi Yeh & Shulian Zhang July 14, 2006.
Introduction of Floor Vibration for Steel Structures ENCE710 – Advanced Steel Structures C. C. Fu, Ph.D., P.E. Department of Civil & Environmental Engineering.
Ch.10 Elasticity & Oscillations Problems: 3, 4, 27, 29. Elastic deformation Hooke’s Law Simple Harmonic Motion (SHM) period & frequency of SHM (sections.
MODULE 09 Inman chapter 5.
Chapter 7. Free and Forced Response of Single-Degree-of-Freedom Linear Systems 7.1 Introduction Vibration: System oscillates about a certain equilibrium.
Copyright © 2009 Pearson Education, Inc. Chapter 14 Oscillations.
The Physical Pendulum Damped Oscillations Forced Oscillations
Response of a joint passive crowd- SDOF system subjected to crowd jumping load Jackie Sim, Dr. Anthony Blakeborough, Dr. Martin Williams Department of.
April Second Order Systems m Spring force ky F(t) (proportional to velocity) (proportional to displacement)
A PPLIED M ECHANICS Lecture 03 Slovak University of Technology Faculty of Material Science and Technology in Trnava.
1 Lecture D32 : Damped Free Vibration Spring-Dashpot-Mass System Spring Force k > 0 Dashpot c > 0 Newton’s Second Law (Define) Natural Frequency and Period.
MECH 391 Instrumentation Lab 9 Vibration Analysis of an Aluminum Cantilever Beam Performed: 03/15/04 Sinan Ozcan : I believe I performed 100% of this lab.
PAT328, Section 3, March 2001MAR120, Lecture 4, March 2001S14-1MAR120, Section 14, December 2001 SECTION 14 STRUCTURAL DYNAMICS.
Basic structural dynamics I Wind loading and structural response - Lecture 10 Dr. J.D. Holmes.
Vibrations & Waves. In the example of a mass on a horizontal spring, m has a value of 0.80 kg and the spring constant, k, is 180 N/m. At time t = 0 the.
CHAPTER - 3 FORCED OSCILLATOR Mrs. Rama Arora Assoc. Professor Deptt. Of Physics PGGCG-11 Chandigarh.
8/8/2011 Physics 111 Practice Problem Statements 14 Oscillations SJ 8th Ed.: Chap 15.1 – 15.5 Oscillations – Basics Hooke’s Law: A Mass on a Spring Simple.
1FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2012/2013 2FCI.
Estimation of Fundamental Natural Frequency, Damping Ratio and Equivalent Mass 523L (Session 4)
Chapter 2 Free Vibration of Single Degree of Freedom Systems
What is called vibration Analysis Design
1 MIDTERM EXAM REVIEW. 2 m 081.SLDASM REVIEW Excitation force 50N normal to face k=10000N/m m=6.66kg Modal damping 5%
Modal Analysis-hw-04 The schematic diagram of a large cannon is shown below. When the gun is fired, high-pressure gases accelerate the projectile inside.
Modal Testing 523L (Session 5). Frequency Response Frequency Response Function – System characteristics in frequency domain How to find FRF – Mathematical.
ME 322: Instrumentation Lecture 31 April 8, 2015 Professor Miles Greiner.
MECH 322 Instrumentation Lab 10 Damped Vibration of a Weighted Cantilever Beam Performed: 4/1/15 Group 0 Miles Greiner Lab Instructors: Marissa Tsugawa.
Vibrationdata 1 Unit 18 Force Vibration Response Spectrum.
Physics Section 11.2 Apply properties of pendulums and springs A pendulum exhibits harmonic motion. A complete cycle is called an oscillation. The maximum.
1 10. Harmonic oscillator Simple harmonic motion Harmonic oscillator is an example of periodic motion, where the displacement of a particle from.
Force Vibration Response Spectrum
Modal Testing 421L/521L (Lab 9) 10/21/2016. Frequency Response Frequency Response Function – System characteristics in frequency domain How to find FRF.
Mechanical Vibrations
Linseed oil + Styrene + Divinylbenzene
Structural damping - an energy dissipation mechanism
Equations of Motion: Kinetic energy: Potential energy: Sin≈
Characterization of C Pod
Characterization of NanoG
Characterization of Omega Pod
MAK4041-Mechanical Vibrations
Oscillatory Motion.
Theoretical Mechanics DYNAMICS
Mechanical Engineering at Virginia Tech
Equations of Motion: Kinetic energy: Potential energy: Sin≈
1/10 prototype support tube
Chapter 3 Harmonically Excited Vibration
ME321 Kinematics and Dynamics of Machines
WEEKS 8-9 Dynamics of Machinery
ME321 Kinematics and Dynamics of Machines
ENGINEERING MECHANICS
Equations of Motion: Kinetic energy: Potential energy: Sin≈
ME321 Kinematics and Dynamics of Machines
ME321 Kinematics and Dynamics of Machines
VIBRATION.
VIBRATION.
Ch.10 Elasticity & Oscillations
DYNAMICS OF MACHINERY Presented by E LAKSHMI DEVI M.Tech,
Presentation transcript:

Estimation of Fundamental Natural Frequency, Damping Ratio and Equivalent Mass 421L/521L (Lab 8)

Single DOF Modeling E, I, L, ρ Cantilever k c E, I, L, ρ Fixed-Fixed M accelerometer E, I, L, ρ Cantilever k c E, I, L, ρ Fixed-Fixed M E: Young’s modulus I: Moment of inertia L: length ρ: mass per unit length x k, stiffness, N/m m, mass, kg c, damping coefficient, N/(m/s) mx”+cx’+kx = f(t) x(t) = Aexp(-ξωnt)COS(ωnsqrt(1-ξ2)t- ψ)+Bsin(ωt) Time response = Transient response + Forced response(sinusoidal) Where, ωn=sqrt(k/m), undamped natural frequency, rad/s ξ =c/sqrt(2mk), damping ratio ωd=ωnsqrt(1-ξ2), damped natural frequency, rad/s

Visualization of responses Exponential part Sinusoidal part Transient response Forced response (Sinusoidal input) Transient response + Forced response

Experiment Identify the fundamental mode characteristics using logarithmic decrement Mount Accelerometer onto beam End for cantilever beam Center for fixed-fixed beam Excite beam by applying ‘impulse’ or initial displacement Observe transient response (No forced response) Collect time response Pick two peaks and measure amplitude and period Find natural frequency, damping ratio Find equivalent mass from beam equation Find damping coefficient and stiffness

? Equivalent mass and natural frequency estimation by Rayleigh method (See the handout) Cantilever Beam meq = 0.2235ρ L ωn=3.6639sqrt(EI/(ρL4)) rad/s Fixed-Fixed Beam meq = 0.3836ρ L ωn=22.373sqrt(EI/(ρL4)) rad/s Does your measurement match to your estimation? Show your measurement and measured value What if you count the mass of the accelerometer?

Experimental setup: Cantilever Beam Aluminum Beam Thickness = 4.84mm Width = 19.09mm Length = 640mm Accelerometer is mounted at the end of the beam Mass of accelerometer = 7.83 gram

Cantilever Beam NOTE: X1,2 = time in s, y1,2 = acceleration in g, (m = ‘mili’)

Work Sheet: Cantilever Beam # Item Unit Value A Time @ peak #1 s B Time @ peak #2 C Amplitude @ peak #1 g D Amplitude @ peak #2 E Time between A and B F Number of periods between A and B G Period of oscillation, E/F # Item Unit Value H Damped natural frequency, wd rad/s I Natural frequency, wn J zeta K Equivalent mass, meq kg L Stiffness, k N/m M Damping, c N/(m/s) N Natural frequency estimation by Rayleigh method

Experimental setup: Fixed-Fixed Beam Aluminum Thickness = 4.84 mm Width = 19.09 mm Length = 640 mm Accelerometer is mounted at the center Mass of accelerometer = 7 .83 gram

Fixed-Fixed Beam NOTE: X1,2 = time in s, y1,2 = acceleration in g, (m = ‘mili’)

Work Sheet: Fixed-Fixed Beam # Item Unit Value A Time @ peak #1 s B Time @ peak #2 C Amplitude @ peak #1 g D Amplitude @ peak #2 E Time between A and B F Number of periods between A and B G Period of oscillation, E/F # Item Unit Value H Damped natural frequency, wd rad/s I Natural frequency, wn J zeta K Equivalent mass, meq kg L Stiffness, k N/m M Damping, c N/(m/s) N Natural frequency estimation by Rayleigh method

Different material? Repeat the experiment with Steel and any nonmetal material Compare the result