Vibration Measurements Vibration Instrumentation. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 11 Fall 2011

Similar documents
10 Measurement of Acceleration, Vibration and Shock Transducers

1-DOF Forced Harmonic Vibration. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 8 Fall 2011

1-DOF Vibration Characteristics. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 7 Fall 2017

Use of reciprocity calibrated accelerometer standards for performing routine laboratory comparison calibrations. Technical paper 226

MAE106 Laboratory Exercises Lab # 6 - Vibrating systems

Chapter 7 Vibration Measurement and Applications

Modeling and Experimentation: Mass-Spring-Damper System Dynamics

Laboratory handouts, ME 340

The secondary winding have equal no. of turns. The secondary windings are placed identically on either side of the primary winding.

Vibration modelling of machine tool structures

Outline of parts 1 and 2

Deriving 1 DOF Equations of Motion Worked-Out Examples. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 3 Fall 2017

Modeling of Resonators

Chapter 5 Design. D. J. Inman 1/51 Mechanical Engineering at Virginia Tech

Institute for Electron Microscopy and Nanoanalysis Graz Centre for Electron Microscopy

Reduced Order Modeling Enables System Level Simulation of a MEMS Piezoelectric Energy Harvester with a Self-Supplied SSHI-Scheme

Silicon Capacitive Accelerometers. Ulf Meriheinä M.Sc. (Eng.) Business Development Manager VTI TECHNOLOGIES

Measurement Techniques for Engineers. Motion and Vibration Measurement

Transactions on the Built Environment vol 22, 1996 WIT Press, ISSN

EE C245 ME C218 Introduction to MEMS Design Fall 2007

Transduction Based on Changes in the Energy Stored in an Electrical Field

Electrostatic Microgenerators

Lecture 19. Measurement of Solid-Mechanical Quantities (Chapter 8) Measuring Strain Measuring Displacement Measuring Linear Velocity

Dynamic Analysis on Vibration Isolation of Hypersonic Vehicle Internal Systems

Springs and Dampers. MCE371: Vibrations. Prof. Richter. Department of Mechanical Engineering. Handout 2 Fall 2017

DEVELOPMENT OF A NOVEL ACTIVE ISOLATION CONCEPT 1

Prof. Dr. Erol KURT Nonlinear Problems in Piezoelectric Harvesters

The student will experimentally determine the parameters to represent the behavior of a damped oscillatory system of one degree of freedom.

ScienceDirect. Response Spectrum Analysis of Printed Circuit Boards subjected to Shock Loads

Dynamic Behaviour of the Rubber Isolator Under Heavy Static Loads in Aerospace Systems

HOMOGENEOUS ELECTRORHEOLOGICAL FLUIDS APPLIED TO VIBRATION CONTROL

Francisco Paulo Lépore Neto. Marcelo Braga dos Santos. Introduction 1. Nomenclature. Experimental Apparatus and Formulation

MEMS INERTIAL POWER GENERATORS FOR BIOMEDICAL APPLICATIONS

Rotational Motion. Figure 1: Torsional harmonic oscillator. The locations of the rotor and fiber are indicated.

Francisco Paulo Lépore Neto. Marcelo Braga dos Santos. Introduction 1. Nomenclature. Experimental Apparatus and Formulation

Laboratory notes. Torsional Vibration Absorber

Driven Harmonic Oscillator

IJSRD - International Journal for Scientific Research & Development Vol. 4, Issue 07, 2016 ISSN (online):

Basic Principle of Strain Gauge Accelerometer. Description of Strain Gauge Accelerometer

Experimental characterization of dry friction isolators for shock vibration isolation

On Non-Ideal Simple Portal Frame Structural Model: Experimental Results Under A Non-Ideal Excitation

COMPLEX MODULUS AND DAMPING MEASUREMENTS USING RESONANT AND NON-RESONANT METHODS

MODELLING AND TESTING OF THE PIEZOELECTRIC BEAM AS ENERGY HARVESTING SYSTEM

Lecture 20. Measuring Pressure and Temperature (Chapter 9) Measuring Pressure Measuring Temperature MECH 373. Instrumentation and Measurements

Energy Harvesting and Dissipation with Piezoelectric Materials

ISO INTERNATIONAL STANDARD

MV Module 5 Solution. Module 5

LECTURE 12. STEADY-STATE RESPONSE DUE TO ROTATING IMBALANCE

2.003 Engineering Dynamics Problem Set 10 with answer to the concept questions

E05 Resonator Design

A Sloping Surface Roller Bearing and its lateral Stiffness Measurement

Dynamics of structures

Applicability of Self-Powered Synchronized Electric Charge Extraction (SECE) Circuit for Piezoelectric Energy Harvesting

Vibration Testing. an excitation source a device to measure the response a digital signal processor to analyze the system response

Sensor Measurements For Diagnostic Equipment

Experimental analysis of influence of initially stressed springs and parameters of excitation on vibration absorber effectiveness

EE C245 / ME C218 INTRODUCTION TO MEMS DESIGN FALL 2011 C. Nguyen PROBLEM SET #7. Table 1: Gyroscope Modeling Parameters

Design and Analysis of dual Axis MEMS Capacitive Accelerometer

7. CONCLUSIONS & SCOPE

THE subject of the analysis is system composed by

On the force drop off phenomenon in shaker testing in experimental modal analysis

Chapter 23: Principles of Passive Vibration Control: Design of absorber

ANALYSIS AND EXPERIMENT OF DYNAMIC CHARACTERISTICS OF ELECTRONIC DEVICE CHASSIS

Vibration Combined High Temperature Cycle Tests for Capacitive MEMS Accelerometers

Comparison between the visco-elastic dampers And Magnetorheological dampers and study the Effect of temperature on the damping properties

Structural changes detection with use of operational spatial filter

Development of a Rubber for a Tuned Mass Damper for Rail Vibration

EXPERIMENTAL DETERMINATION OF DYNAMIC CHARACTERISTICS OF STRUCTURES

Module 4: Dynamic Vibration Absorbers and Vibration Isolator Lecture 19: Active DVA. The Lecture Contains: Development of an Active DVA

Mechanical Sensors 1.

Laboratory handout 5 Mode shapes and resonance

Technical Protocol of the CIPM Key Comparison CCAUV.V-K5

Physics 326 Lab 6 10/18/04 DAMPED SIMPLE HARMONIC MOTION

Chapter 3. Experimentation and Data Acquisition

Module I Module I: traditional test instrumentation and acquisition systems. Prof. Ramat, Stefano

EE C245 / ME C218 INTRODUCTION TO MEMS DESIGN FALL 2009 PROBLEM SET #7. Due (at 7 p.m.): Thursday, Dec. 10, 2009, in the EE C245 HW box in 240 Cory.

Simple Harmonic Motion ===============================================

Critical loss factor in 2-DOF in-series system with hysteretic friction and its use for vibration control

Experiment 5. Simple Harmonic Motion

Alireza Mousavi Brunel University

Finite Element Modules for Demonstrating Critical Concepts in Engineering Vibration Course

666. Controllable vibro-protective system for the driver seat of a multi-axis vehicle

Science Lab #1. Standing Waves

EE C245 ME C218 Introduction to MEMS Design Fall 2007

ME 328 Machine Design Vibration handout (vibrations is not covered in text)

DEVELOPMENT OF DROP WEIGHT IMPACT TEST MACHINE

ME 563 HOMEWORK # 7 SOLUTIONS Fall 2010

REAL-TIME HYBRID EXPERIMENTAL SIMULATION SYSTEM USING COUPLED CONTROL OF SHAKE TABLE AND HYDRAULIC ACTUATOR

Energy balance in self-powered MR damper-based vibration reduction system

Mobility and Impedance Methods. Professor Mike Brennan

Heterogeneous 3D integration considered by the perspective of reliability studied in the European projects e-brains and ESiP

Technical Protocol of the Bilateral Comparison in Primary Angular Vibration Calibration CCAUV.V-S1

PROJECT 1 DYNAMICS OF MACHINES 41514

Numerical Solution of Equation of Motion

Evaluation of a Six-DOF Electrodynamic Shaker System

Precision Machine Design

Using Operating Deflection Shapes to Detect Misalignment in Rotating Equipment

Possible Design Modification for Capacitive Type MEMS Accelerometer

Design and characterization of in-plane MEMS yaw rate sensor

Why You Can t Ignore Those Vibration Fixture Resonances Peter Avitabile, University of Massachusetts Lowell, Lowell, Massachusetts

Transcription:

MCE371: Vibrations Prof. Richter Department of Mechanical Engineering Handout 11 Fall 2011

Overview of Vibration Measurements Follow Palm, Sect. pp 425-430 and 559-562. Additional references: Holman, J.P., Experimental Methods for Engineers, Mc.Graw-Hill, 8th Edition Harris, C.M. and Crede, Ch. (editors), Shock and Vibration Handbook, Mc. Graw-Hill, 2nd Edition. This chapter of the course is just an overview of techniques and equipment for vibration measurements. More detailed studies of vibration measurement are carried out in MCE380: Measurements and Instrumentation Lab and some graduate courses in advanced vibration (MCE512) and mechatronics (MCE603)

Vibration Nomographs For sinusoidal vibration of the form x(t) = Asin(wt +φ) we know that the displacement, velocity and acceleration amplitudes are: x = A ẋ = Aw ẍ = Aw 2 = w ẋ Taking logarithms: log ẋ = log x +logw log ẍ = log ẋ +logw From the last equation log ẋ = log ẍ logw

Vibration Nomographs... In terms of amplitudes (peaks) The log velocity is a linear function of the log frequency, with slope +1 and intercept log x The log velocity is also a linear function of the log frequency, with slope -1 and intercept log ẍ. Given A = log x, we can plot log velocity against log frequency. Varying A gives a family of parallel lines with slope +1. Also, given an acceleration amplitude, we can plot log velocity against log frequency. Varying the acceleration amplitude gives a family of parallel lines with slope -1.

Example Vibration Measurements We write Matlab code to reproduce Fig. 7.1-1 in Palm. We use A =1, 2, 5, 10, 50 and 100 mm. For the acceleration we use 1000, 2000, 5000 and 10000 mm/s 2. The frequency axis ranges between 1 and 10 Hz, while the velocity axis ranges between 100 and 1000 mm/s.

Admissible Vibration Levels in a Nomograph The maximum vibration that can be tolerated by humans or machines are given by a combination of displacement, velocity and acceleration limits. These limits may vary with frequency. 1 It is not the same to sustain a 1mm displacement amplitude at 1 Hz than at 1000 Hz. Should the tolerable displacement increase or decrease with frequency? 2 Displacement amplitude limits as a function of frequency can be plotted in a typical Bode plot. 3 Maximum absolute accelerations also apply across all frequencies (remember that acceleration is proportional to force) 4 Maximum absolute velocities may also apply. 5 A nomograph can be used conveniently for the 2 last kinds of limits (see Palm, Fig. 7.1-2)

Example: Structural Vibration Limits As part of this course, we find the boundaries for acceptable vertical vibration for a small CD player (for skip-free operation).

The Seismic Accelerometer

Seismic Accelerometer Analysis It s just a mass-spring-damper system with base excitation. Recall the force transmissibility formula (Eq. 4.3-13 in Palm) F t = kyr 2 4ζ 2 r 2 +1 (1 r 2 ) 2 +4ζ 2 r 2

Seismic Accelerometer Analysis... Note that Yr 2 = (Yw 2 )/wn, 2 where (Yw 2 ) is the harmonic acceleration amplitude, call it a. Then F t = a(k/wn) 2 4ζ 2 r 2 +1 (1 r 2 ) 2 +4ζ 2 r 2 The term in the square root is practically constant when r << 1 and ζ is not too small. That is, the force sensed by the piezoelectric disk is practically proportional to acceleration for well-damped systems away from r = 1.

Seismic Accelerometer Analysis Unfortunately, the conversion from sensed force to output voltage is not that simple. The piezoelectric ceramic produces electric charge in proportion to force, but a direct charge readout is not reliable due to uncertainty in the capacitance of the cables. (remember V = q/c). A charge amplifier is an electronic device providing an output voltage proportional to charge when operated above certain treshold frequency. Constant accelerations cannot be measured. The overall instrumented accelerometer response looks like this:

MEMS Accelerometer MEMS stands for micro-electro-mechanical systems technology. A MEMS device contains small-scale components (1 to 100 micrometers) acting as inertial masses and stiffnesses. Their motion is sensed by electromagnetic or electrostatic means. The whole package, called lab on a chip can be embedded in electronic packaging as a self-contained unit.

Electrodynamic Shaker A shaker is a 1D vibration exciter driven by voltage. They are available from small table-top units to 20-ton devices that need water cooling.

In-class demo: Accelerometer Calibration We use a MEMS accelerometer with a sensitivity of 1 V/g to calibrate a seismic accelerometer. Equipment: 1 ±1.7 g MEMS accelerometer on evaluation board with analog output. ADXL203. 2 Electrodynamic shaker (vibration exciter) 3 Amplified function generator to drive shaker 4 4-channel oscilloscope 5 PCB 303A SN 2405 piezoelectric accelerometer 6 PCB ICP charge amplifier Vary the excitation frequency between 25 and 95 Hz, at 10 Hz increments. Record the MEMS and piezo accelerometer output voltage amplitudes for each frequency.