Understanding dynamic response

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GE Oil & Gas Understanding Dynamic Response Extract from Bently Nevada Machinery Diagnostics Training

description

Understanding Dynamic Response of a simple structure. This applies to conventional turbo-machinery diagnostics and understanding the sychronous vibration response through the full speed range.

Transcript of Understanding dynamic response

Page 1: Understanding dynamic response

GE Oil & Gas

Understanding Dynamic Response

Extract from Bently Nevada Machinery Diagnostics Training

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Transient Vibration Data Formats

• Amplitude and Phase displayed together

• Slow roll runout vector• Heavy/high spot location• Rotor and structural resonances• Rotor mode shape “1st critical”

Bode’ and Polar Plots

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Bode' Plot

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Polar Plot• Typical “synchronous rotor response”.Phase lag angle increases with machine speed.Amplitude increases to a max. at “critical” speed, then reduces

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Dynamic Stiffness – Simple Model

K D

M

Dynamic Unbalance Force

F(t) = m.r. W2 = U. W2

DampingSpring

MassDisplacementFrom rest

d (t)

Equation of Motion: dMdDdKF t )(ti

t ed )(let:

dieid ti

deid ti 222then:

and:

dMdDidKF 2

DiMKd

F 2

Simple Dynamic Stiffness:

Direct

displacement accelerationvelocity

Quadrature

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Dynamic Stiffness at Low Speed

K

Synchronous Dynamic Stiffness

f = 20 D.W

M.W2

At low speeds, dominant factor is “Spring Stiffness”

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Dynamic Stiffness at Resonance

K

Synchronous

Dynamic Stiffness f = 90

D.W

M.W2

At resonance, dominant factor is “Damping Stiffness”

This is also known as “Quadrature Stiffness”

2MK

At Resonance:

M

Kres

Resonant Frequency:

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Dynamic Stiffness at High Speed

K

Synchronous Dynamic Stiffness f = 150

D.W

M.W2

At high speeds, dominant factor is “Mass Stiffness” – i.e: Inertial

effect

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Synchronous Vibration Response – Low Speed

M.W2

K

D.W

At low speeds, displacement is in same direction as

unbalance force

Unbalance

Unbalance Force = U.W2

Dynamic response (displacement) = Force / Dynamic Stiffness

Displacement

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M.W2

K

D.W

At resonance, displacement has a 90 degree phase lag from

unbalance force

Unbalance Force = U.W2

Dynamic response (displacement) = Force / Dynamic Stiffness

Displacement

f = 90

Synchronous Vibration Response – Resonance

Unbalance

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M.W2

K

D.W

At high speeds, displacement vector is almost opposite the unbalance

force

Unbalance Force =

U.W2

Locus of displacement vectors through the whole speed range

Dynamic response (displacement) = Force / Dynamic Stiffness

Displacement

Synchronous Vibn Response – High Speed

Unbalance

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1X (Synchronous) Response

90°

180°

270°

ROTN

Probe

Heavy Spot

WR = System Resonance Frequency

W

WWR

High Spot

Angle of Heavy Spot

fu

f

0

90°

180°

Ph

ase L

ag

1X

Am

plitu

de |

A|

A

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Transient Vibration Analysis

• Reveals information on whether Dynamic stiffness has changed from run to run. Confirms integrity of the rotor.

• Shows symptoms caused by increased system stiffness – like seal rubs

• Indicates where we should add our trial balance weights

• Gives clues about why the machine behaves this way – ie: might be running near a natural resonance…

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Questions?