Comparison of Transmissibility of Non-Metallic Materials For Vibration Isolation

Similar documents
Calibration of Hollow Operating Shaft Natural Frequency by Non-Contact Impulse Method

Assistant Professor, Department of Mechanical Engineering, Institute of Engineering & Technology, DAVV University, Indore, Madhya Pradesh, India

Vibration Analysis of deep groove ball bearing using Finite Element Analysis

CHAPTER 7 FAULT DIAGNOSIS OF CENTRIFUGAL PUMP AND IMPLEMENTATION OF ACTIVELY TUNED DYNAMIC VIBRATION ABSORBER IN PIPING APPLICATION

Analytical and Experimental Investigation of a Tuned Undamped Dynamic Vibration Absorber in Torsion

Vibration Fundamentals Training System

Review on Fault Identification and Diagnosis of Gear Pair by Experimental Vibration Analysis

9LEUDWLRQ 0HDVXUHPHQW DQG $QDO\VLV

An Analytical Method of Prediction of Stability and Experimental Validation using FFT Analyzer in End Milling process

Vibration Analysis on Rotating Shaft using MATLAB

EIGEN MODES IDENTIFICATION FOR HYBRID WIRE ROPE ISOLATORS

Lab VIEW Programming for Vibration Analysis

Rotating Machinery Fault Diagnosis Techniques Envelope and Cepstrum Analyses

Experimental Study of a Exhaust Pipe Using FFT Analyzer

Preliminary study of the vibration displacement measurement by using strain gauge

Signal Analysis Techniques to Identify Axle Bearing Defects

Response spectrum Time history Power Spectral Density, PSD

Active Vibration Isolation of an Unbalanced Machine Tool Spindle

Economical Method of Reducing vibration on Machine Foundation

Vibration based condition monitoring of rotating machinery

Study of Improper Chamfering and Pitting Defects of Spur Gear Faults Using Frequency Domain Technique

Appearance of wear particles. Time. Figure 1 Lead times to failure offered by various conventional CM techniques.

Introduction*to*Machinery*Vibration*Sheet*Answer* Chapter*1:*Vibrations*Sources*and*Uses*

Also, side banding at felt speed with high resolution data acquisition was verified.

DESIGN AND FABRICATION OF GRINDING ATTACHMENT FOR LATHE MACHINE TOOL

COMPARATIVE STUDY OF VIBRATION ISOLATORS USING PARAMETER TRANSMISSIBILITY

Analysis on Acoustic Attenuation by Periodic Array Structure EH KWEE DOE 1, WIN PA PA MYO 2

Elastic Support of Machinery and Equipment

VIBRATION ANALYSIS OF DRILLING OPERATION

Industrial vibration sensor selection: Piezovelocity transducers

Copyright 2017 by Turbomachinery Laboratory, Texas A&M Engineering Experiment Station

Wavelet Transform for Bearing Faults Diagnosis

AGN 008 Vibration DESCRIPTION. Cummins Generator Technologies manufacture ac generators (alternators) to ensure compliance with BS 5000, Part 3.

Fundamentals of Vibration Measurement and Analysis Explained

Performance Enhancement of Automotive Silencer Using Finite Element Analysis

Experimental investigation of crack in aluminum cantilever beam using vibration monitoring technique

CHAPTER 5 FAULT DIAGNOSIS OF ROTATING SHAFT WITH SHAFT MISALIGNMENT

Shaft Vibration Monitoring System for Rotating Machinery

ACOUSTIC NOISE AND VIBRATIONS OF ELECTRIC POWERTRAINS

FREE VIBRATION ANALYSIS AND OPTIMIZATION OF STREEING KNUCKLE

Monitoring The Machine Elements In Lathe Using Vibration Signals

RESEARCH PAPER CONDITION MONITORING OF SIGLE POINT CUTTING TOOL FOR LATHE MACHINE USING FFT ANALYZER

Effect of crack depth of Rotating stepped Shaft on Dynamic. Behaviour

CHAPTER 3 DEFECT IDENTIFICATION OF BEARINGS USING VIBRATION SIGNATURES

FAULT DETECTION IN DEEP GROOVE BALL BEARING USING FFT ANALYZER

Bearing fault detection of wind turbine using vibration and SPM

An Alternative to Pyrotechnic Testing For Shock Identification

MODELLING AND CHATTER CONTROL IN MILLING

An Improved Method for Bearing Faults diagnosis

INDUCTION MOTOR FAULT DIAGNOSTICS USING FUZZY SYSTEM

Current-Based Diagnosis for Gear Tooth Breaks in Wind Turbine Gearboxes

Detection of Wind Turbine Gear Tooth Defects Using Sideband Energy Ratio

Industrial vibration sensor selection: piezovelocity transducers

Testing Sensors & Actors Using Digital Oscilloscopes

CHAPTER 3 THE DESIGN OF TRANSMISSION LOSS SUITE AND EXPERIMENTAL DETAILS

FAULT DIAGNOSIS OF SINGLE STAGE SPUR GEARBOX USING NARROW BAND DEMODULATION TECHNIQUE: EFFECT OF SPALLING

Guan, L, Gu, F, Shao, Y, Fazenda, BM and Ball, A

Application Note. Monitoring strategy Diagnosing gearbox damage

Design of a System to Control the Noise of Dry Fluid Coolers

Theory and praxis of synchronised averaging in the time domain

1433. A wavelet-based algorithm for numerical integration on vibration acceleration measurement data

Classification of Misalignment and Unbalance Faults Based on Vibration analysis and KNN Classifier

On the analyzer under UTILITY - CHANGE SETUP - MEASUREMENT MODE - OVERALL LEVEL MODE, the user can select either DIGITAL or ANALOG.

A study of Savitzky-Golay filters for derivatives in primary shock calibration

STUDY ON IDENTIFICATION OF FAULT ON OUTER RACE OF ROLLER BEARING USING ACOUSTIC EMISSION

A simulation of vibration analysis of crankshaft

SEPARATING GEAR AND BEARING SIGNALS FOR BEARING FAULT DETECTION. Wenyi Wang

Fault diagnosis of massey ferguson gearbox using power spectral density

CYLINDRICAL STUD MOUNT SERIES

Natural Frequencies and Resonance

Fault Detection of Double Stage Helical Gearbox using Vibration Analysis Techniques

Comparative Analysis of Triaxial Shock Accelerometer Output

Investigation of Effect of Chatter Amplitude on Surface Roughness during End Milling of Medium Carbon Steel

Optical Encoder Applications for Vibration Analysis

Capacitive MEMS accelerometer for condition monitoring

Lab 2b: Dynamic Response of a Rotor with Shaft Imbalance

Application Note #2442

Fabrication & Testing of composite tractor trolley chassis Mr. Ashish Azade 1 Mr.Tushar B.Shinde 2

System Inputs, Physical Modeling, and Time & Frequency Domains

Investigation and Analysis of Chatter Vibration in Centerless Bar Turning Machine

Design, construction and testing of a vibrometer

Frequency Response Function Measurements of Disc and Drum Brake With its Verification by CAE

About Doppler-Fizeau effect on radiated noise from a rotating source in cavitation tunnel

Acoustic Performance of Helmholtz Resonator with Neck as Metallic Bellows

SVENSK STANDARD SS :2014

CHAPTER 6. CALCULATION OF TUNING PARAMETERS FOR VIBRATION CONTROL USING LabVIEW

Condition Monitoring and Vibrational Analysis of Shaft Through Experimental and FEA Approach

FAN NOISE & VIBRATION

1 INTRODUCTION 2 MODELLING AND EXPERIMENTAL TOOLS

Solution of Pipeline Vibration Problems By New Field-Measurement Technique

Gear Noise Prediction in Automotive Transmissions

Automobile Independent Fault Detection based on Acoustic Emission Using FFT

On-Line Monitoring of Grinding Machines Gianluca Pezzullo Sponsored by: Alfa Romeo Avio

GENERAL PURPOSE PIEZOELECTRIC LOAD CELL

An observation on non-linear behaviour in condition monitoring

Statistical analysis of low frequency vibrations in variable speed wind turbines

Developer Techniques Sessions

ANALYSIS OF MACHINERY HEALTH CONSIDERING THE PARAMETERS OF VIBRATION IN A MULTI-FUNCTIONING ARRANGEMENT

A Comparative Study of Wavelet Transform Technique & FFT in the Estimation of Power System Harmonics and Interharmonics

Effect of temperature on modal characteristics of steel-concrete composite bridges: Field testing

Transcription:

IOSR Journal of Mechanical and Civil Engineering (IOSR-JMCE) e-issn: 2278-1684,p-ISSN: 2320-334X PP. 57-61 www.iosrjournals.org Comparison of Transmissibility of Non-Metallic Materials For Vibration A. R. Lavhande, S. B. Tuljapure (Department of Mechanical Engineering, Walchand Institute of Technology, Solapur, India) Abstract : Vibrations in the machines are introduced during operation due unbalanced forces. Therefore it should be eliminated or at least reduced. Vibration can be reduced by introducing the isolation between the vibration source and receiver. In this paper, the vibrations generated due to gyroscope coupled with variable speed motor are analyzed and reduced using nonmetallic isolators. The materials used are cork, rubber, and neoprene. The transmissibility is compared for three different speeds. For measuring the vibrations, FFT analyzer is used. Keywords : FFT Analyzer, Isolator, Transmissibility, Vibration isolation. I. Introduction Vibrations occur in most of machines. A vibration problem is nicely described by the source path receiver model. Source is a mechanical or fluid disturbance, generated internally by the machine, such as unbalance, torque pulsations, gear tooth meshing, fan blade passing, etc. Path is the structural or airborne path by which the disturbance is transmitted to the receiver. Receiver is the responding system, generally foundation or base structure. The objective of this paper is to analyze the vibrations induced in gyroscope coupled with varying speed motor and to analyze and compare the vibrations after using isolator. Compare the transmissibility to check which material for better isolation. 1. Vibration Vibration isolation is defined as the prevention of vibrations from entering a system or we can also define transmissibility as the percent of vibrational energy that is being transmitted through a structure. Mathematically these two terms are simply related.transmissibility is a measure of the reduction of transmitted force or motion afforded by an isolator. Transmissibility is the ratio of the force amplitude transmitted to the foundation to the amplitude of the exciting force. Thus transmissibility can be formulated as: Where T is the Transmissibility ratio FT is force transmitted, Fo is exciting force, X is motion transmitted, Y is motion excited by the source. The effectiveness of the isolator, expressed in per cent is: % = (1-T)*100 (2) If the vibration frequency is not constant or if the vibration involves a large number of frequencies, the desired reduction of vibration may not be attainable by altering the natural frequency of the responding system. It may be possible to achieve equivalent results by the dissipation of energy to eliminate the severe effects of resonance. Generally the isolators are springs, pads and mounts. Generally, Materials used for isolator are steel for spring; neoprene, rubber etc. are preferred for pad and mounts. In this paper the transmissibility for cork, rubber and neoprene are compared. 1.1 FFT Analyzer FFT analyzers are used for the measurement of vibration. It consists of accelerometer used as sensor. Accelerometer is connected to the vibrating base with the help of adhesive and it senses the vibratory motion. FFT analyzers make use of the FFT (fast Fourier transform) algorithm to calculate the spectra of blocks of data. FFT analyzers produce a (complex) spectrum with a number of spectral lines equal to half the number of (real) time samples transformed. (1) 57 Page

II. Experimentation 2.1 Problem Identification The experimental setup of gyroscope coupled with variable speed motor has vibrations. The amplitude of vibration increases with increase in speed. The vibrations in gyroscope are transferred to wooden table. This vibration causes table to vibrate. The gyroscope is coupled with the variable speed motor whose speed can be adjusted with the help of regulator. As the speed of the motor is varied from 1 rpm to above, the vibrations are also increased which can be sensed at the foundation table. 2.2 Experimental Procedure In the work, experimental setup of gyroscope coupled with variable speed motor is used. The whole setup is rested on wooden table. The unbalanced forces are produced in rotating motor causes base to vibrate. Different nonmetallic material pads are used as isolator to attenuate vibrations and regulator is used to vary the speed of motor. Here the gyroscope is vibration source and wooden table is vibration receiver. The isolator pads of rubber are kept in between them as path.the motor speed can be varied from 0 to 3000 rpm by adjusting the voltage regulator. The base of gyroscope has 30 cm diameter and is rested on wooden table. Four isolator pads are used for isolation purpose. The materials used for the isolator are cork, rubber and neoprene. These pads are kept between base and wooden table. The dimensions of material for isolator are taken as same. Each isolator has 5mm thickness and 50 mm length and width. The vibrations are analyzed for three different speeds viz. 1000 rpm, 1600 rpm, and 2200 rpm and spectrum is taken using FFT analyzer.oros NV gate 8.0 FFT analyzer is used to measure the acceleration at different speeds. The accelerometer sensor is attached to table with the help of adhesive. The experiment is carried out in two stages. In the first stage, the speed is adjusted and graph is recorded. This gives values of vibration induced in the setup. In second stage, the four isolator pads are kept between setup and the base (red dots shown in figure) and graph is recorded. This gives the values of vibration transmitted through rubber pad isolator to base. The gyroscope coupled to the motor is shown in Fig. 1 Fig. 1 Gyroscope coupled with varying speed motor experimental setup Fig. 2 Isolators used for the experimental work 58 Page

III. Results and Discussions The data obtained is tabulated as follows. The transmissibility is calculated using equation 3 given above. (rpm) Table 1: Transmissibility analysis of CORK pad for different speeds RMS value of Acceleration Transmissibility Without isolator With isolator Ratio (Xo), m/s² (Xt), m/s² T.R.= Xt/Xo 1000 850 E-06 398 E-06 0.4682 53.17 1600 1.075 E-03 655 E-06 0.6093 39.07 2200 1.804 E-03 997 E-06 0.5526 44.73 Table 2: Transmissibility analysis of RUBBER pad for different speeds RMS value of Acceleration Transmissibility Without isolator With isolator Ratio (Xo), m/s² (Xt), m/s² T.R.= Xt/Xo (rpm) 1000 850 E-06 704 E-06 0.8282 17.18 1600 1.075 E-03 981 E-06 0.9125 8.70 2200 1.804 E-03 1.513 E-03 0.8387 16.13 Table 3: Transmissibility analysis of NEOPRENE pad for different speeds RMS value of Acceleration Transmissibility Ratio (rpm) Without isolator With isolator (Xo), m/s² (Xt), m/s² T.R.= Xt/Xo 1000 850 E-06 680 E-06 0.8 20 1600 1.075 E-03 695 E-06 0.6465 35.35 2200 1.804 E-03 785 E-06 0.435 56.5 For data obtained it is seen clearly that with increase in the speed, the vibration also increases. For low speeds the vibrations are less. For high speed the neoprene shows great reduction in vibration. The effectiveness of isolation of neoprene at high speeds is 56.5 %, while of cork is 44.73%. The effectiveness of isolation for cork material as isolator remains constant for low to high speeds.the transmissibility is calculated for each material at different speeds. The cork provides minimum average value of transmissibility= 0.543, neoprene provides average value of transmissibility= 0.627, while rubber provides average value of transmissibility= 0.86. The vibration spectrum recorded using FFT analyzer for high speed i.e. 2200 rpm is shown in figure below. The graph gives clear idea of reduction of vibration. The spectrum is frequency in hz. vs. acceleration in m/s². The spectrum shows peak values of vibration before and after isolation. IV. Conclusions And Future Scope The vibration increases with increase in speed of motor. The main purpose of this work is to compare the transmissibility of nonmetallic materials. Cork shows reliable and good isolation behavior. From the discussions it is come to know that the cork shows good isolation property. Depending upon the results obtained and mean effectiveness of isolation, the materials for isolator pads can be arranged as Rubber < Neoprene < Cork.In fig 6, it can be seen that when compared to rubber and cork, neoprene greatly reduces the vibrations. The effectiveness of isolation of neoprene pad for 2200 rpm is 44.73%. Cork pad is suitable for low as well as high speeds.rubber is used as isolator in machine workshop, but neoprene also shows good isolation property. As compared to cork and neoprene the rubber is less costly and thus more thick rubber pads can be used for isolation purpose. For precise vibration isolation cork should be used as isolator. The combination of rubber and cork can reduce the vibrations. 59 Page

Fig. 3 vs. Transmissibility ratio for isolators Fig. 4 vibration spectrum for Cork material as isolator Acknowledgements I would like to express my sincere gratitude to our Principal Dr. S. A. Halkude and Dr. P. R. Kulkarni (Head of Mechanical Engineering Department) for giving me the opportunity to widen the knowledge and also for their constant encouragement and inspiration during project work. Also I am very thankful to my guide Prof. S. B. Tuljapure for giving much of their valuable time, precious guidance. Fig. 5 vibration spectrum for Rubber material as isolator 60 Page

Fig. 6 Vibration spectrum for Neoprene material as isolator References [1]. A. Tiwari, A. Chandsarkar,Analyze the transmissibility of various materials using vibration analysis, International journal of engineering sciences & research Technology,3(8),2014,247-251. [2]. D. D. L. Chung,Review materials for vibration damping, Journal of material science 36,2001,5733-5737. [3]. Chen Xueqian, Shen Zhanpeng, He Qinshu, Du Qiang & Liu Xinen,Influence of uncertainty and excitation amplitude on the vibration characteristics of rubber isolator, Journal of Sound and Vibration 377,2016, 216 225. [4]. C. M. Harris, Allan G. Piersol, Harris,shock and vibration handbook (McGRAW-HILL,2002). [5]. G. K. Grover, Mechanical vibrations (Nem chand & bros, 2009) 61 Page