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Vibration Measurement Presented by Mr.Kiratikorn Kaewpankan 553040033-2 Mechanical Engineering KhonKaen University
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Vibration Measurement Present

Dec 19, 2015

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Page 1: Vibration Measurement Present

Vibration Measurement

Presented byMr.Kiratikorn Kaewpankan553040033-2

Mechanical Engineering KhonKaen University

Page 2: Vibration Measurement Present

ObjectiveTo determine the damped natural

frequency and damping ratio of vibration system by testing.

To determine the damped and undamped natural frequency of vibration system by theory.

Compare frequency from testing and theory.

Page 3: Vibration Measurement Present

Experimental equipment.

1. Vibration system

2. Vibration measurement

Page 4: Vibration Measurement Present

3. Computer and software (Vibview)

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How to Experiment1. Turn on vibration measurement and setting.

2. Install the sensor at the end of the beam.

3. Use rubber hammer to tap on the beam and wait until the scope shown result in graph.

4. Record the graph and use Vipview to change the graph to the number that use to plot.

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Beam

Free Body Diagram

Page 7: Vibration Measurement Present

Theory

Mass moment of inertia

𝐽𝑏=13π‘šπ‘π‘

2𝐽 s=π‘šπ‘ (𝑠¿¿2+h2)ΒΏ

βˆ‘ π‘€π‘œ= 𝐽 �̈�𝐽 �̈�=βˆ’π‘˜1 𝑦1𝑙1πœƒβˆ’π‘˜2 𝑦2 𝑙2πœƒ+𝑐1 �̈�+𝑐2 �̈�

𝐹=π‘˜ 𝑦𝐽 �̈�+π‘˜1 𝑙1

2πœƒ+π‘˜2 𝑙22πœƒ=0

ωω

From

Change

We can find

=full volume of beam

=inner volume of beam

Page 8: Vibration Measurement Present

βˆ’ 𝐽 πœ”2+(π‘˜ΒΏΒΏ1 𝑙12+π‘˜2 𝑙2

2)=0ΒΏ

πœ”π‘›=√ (π‘˜ΒΏΒΏ1 𝑙12+π‘˜2 𝑙2

2)𝐽

ΒΏ

(Ο‰

Now we want to find but this vibration system can’t be find pure βˆ‘ π‘€π‘œ=0

𝐹 1𝑙1 cosπœƒ+𝐹2 𝑙2π‘π‘œπ‘ πœƒ=π‘šπ‘€π‘€ cosπœƒ

𝐹=π‘˜π‘¦π‘˜1 𝑦1𝑙1π‘π‘œπ‘  πœƒ+π‘˜2 𝑦2 𝑙2π‘π‘œπ‘ πœƒ=π‘šπ‘€π‘€ cosπœƒ

π‘˜1 𝑦1𝑙1+π‘˜2 𝑦2𝑙2=π‘šπ‘€π‘€

Page 9: Vibration Measurement Present

𝑦 π‘₯

𝑙π‘₯= 𝑦𝑀

Similar triangles

π‘˜1𝑙1𝑦𝑀𝑙1+π‘˜2𝑙2

𝑦𝑀𝑙2=π‘šπ‘€π‘€

π‘˜1𝑙12+π‘˜2𝑙2

2=π‘šπ‘€π‘€π‘€π‘¦

Using = 10 kg = 98.1 N

π‘˜1𝑙12+π‘˜2𝑙2

2=2275 . 470𝑁 .π‘š

Page 10: Vibration Measurement Present

ResultsSection 1. I’m use the average of 5graph to fine natural frequency and damping ratio

When n= cycle of vibration V0 = maximum velocity=

t0, tn=time for vibration

Page 11: Vibration Measurement Present

we use for five graph

𝑓 𝑑 𝑒=27 .5229+27 .5229+27 .1003+27 .1257+27 .2537

5

𝑓 𝑑𝑒=27 .3111𝐻𝑧

πœ”π‘‘=2πœ‹ 𝑓 π‘‘πœ”π‘‘π‘’=2πœ‹ (27 .3111𝐻𝑧 )=171 .6007π‘Ÿπ‘Žπ‘‘ /𝑠

= 0.1145Logarithmic decrement

=𝛿

√(2πœ‹)2+𝛿2Damping Ratio

0 .1145

√(2πœ‹)2+0 .11452=0 .0182=

Find Damping Ratio ()

Page 12: Vibration Measurement Present

Section 2. From Theory

πœ”π‘›=√ (π‘˜ΒΏΒΏ1 𝑙12+π‘˜2 𝑙2

2)𝐽

ΒΏ

π‘˜1𝑙12+π‘˜2𝑙2

2=2275.470𝑁 .π‘š

= = = )() = =

Page 13: Vibration Measurement Present

We can change Undamped into Damped

πœ”π‘‘π‘‘=πœ”π‘›βˆš1βˆ’2From testing

= 27.9246 Hz

πΈπ‘Ÿπ‘Ÿπ‘œπ‘Ÿ=| 𝑓 π‘‘π‘‘βˆ’ 𝑓 𝑑

𝑓 𝑑𝑑|Γ—100%ΒΏ|27.9246Hzβˆ’27.3111Hz27.9246Hz |Γ—100%=2.1969%

Error between and and

Page 14: Vibration Measurement Present

Bonus >> No weight. How about frequency ?

𝐽=[ 13 0 .23377614 (0 .598)2]New J ΒΏ0 .027866 π‘˜π‘” .π‘š2

Change Undamped into Damped

πœ”π‘‘π‘‘=πœ”π‘›βˆš1βˆ’2

πœ”π‘‘π‘‘= (287 .203 rad /s )Γ—βˆš1βˆ’0 .01822

πœ”π‘‘π‘‘=287 .155 rad /s

= 45.702 Hz

Page 15: Vibration Measurement Present

SummaryFrom testingDamped natural frequency () = 27.3111 Hz Damping ratio =0.0182

From TheoryUndamped Natural frequency () =27.9292 Hzdamped Natural frequency () =27.9249 Hz

Bonus no weightUndamped Natural frequency () = 45.470 Hzdamped Natural frequency () = 45.702 Hz

Error of Damped natural frequency between testing and theory =2.19 %

Page 16: Vibration Measurement Present

Discussion