Machine Foundation Dr. Bhatia

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Foundations for Industrial Machines Understandi~g. Dynarni~s of Machine Found~ Design Considerations -

r~-F-L-s-m-i-d-th p-riv-a-te-L-im-i-te-d~DeSign~~l

L

-;:=========_= Bombay 4,5& 18

th

March 2010

JI

Hyderabad 12, 13 & 26 th March 2010

Training Program by

Dr. K. G. Bhatia

D-CAD TECHNOLOGIES 158, Vardhman Grand Plaza, Mangalam Place, Rohini Sect -3, New Delhi 110085, India Tel: +91-11-27948306, +91-9873003427

~

Foundations for Industrial Machines Understanding· Dynamics of Machine Foundation Design Consideration

Training Program by

Dr. K. G. Bhatia B. Sc. Engg, ME, PhD FIE. FfSET,FfASE, MfSWE, FIGI

Formerly General Manager, BHEL Member - Research Council, SERC -G (CSIR) President - Indian Society of Earthquake Technology Chairman -Indian Society of Earthquake Technology, Delhi Chapter Expert Member - Group on Earthquake Preparedness of NCT of Delhi

Specialization: Structural Dynamics, Earthquake, Wind, Shock, Impact, Stress, Vibration, Machine Foundation, Vibration Isolation

O-CAO TECHNOLOGIES Center for Applied Dynamics 158, Vardhman Grand Plaza, Mangalam Place, Rohini Sect -3, New Delhi 110085, India Tel: +91-11-27948306, +91-9873003427 Regd, Off: C-2/155, West Enclave Pitampura, New Delhi -110034, India Tel: +91-11-27027746, +91-9810013428 email: [email protected];[email protected] Visit

www.machinefoundation.com; www.structuraldynamics.co.in

Foundations for Industrial Machines Dr. K G Bhatia

Understanding Dynamics of Machine Foundation Design Considerations

1

2

• Machine • Foundation • Support System

Dynamic Force

Machine

Foundation

3

M/c Foundation Design END OBJECTIVE

~/

>-

Desired Performance

y

Minimum Vibration Transmission

1>-

Structural Integrity

I

4

Columns

5

6

PH FAN -FAN-PED-TOP -Vertical-

1:]

,.'" 0

"-

26

( Speed 1000 rpm

=16.8Hz

)

w

E

0.2

~

13

96

~

E E

168Hz

0

41,5

83

20

-)

101.04.2009 16:07:06

O/Ail 0.457 mmls rms

~ 1:] O~

30

orders

1000 RPM

PH FAN -FAN-PED-TOP -Horizon!a!-

r--------;::;[s=pe:::ed::;,o:::::oo=,p=m====::---c =16.8Hz

U~

~

E ~

0.2

E E

168 Hz

101:04.200916:06:44

O/AII 0.541 mm/s rms

1000 RPM

7

PH FAN -FAN-PED-TOP -Axial· ill

" "0

~

E

-"'. E E

1:] 1.2 1

26

96

[ Speed 1000 rpm = 16.8Hz

08 13 06 04 02 10

30

20

168 Hz

-)

101:04.2009 16:07:20

Transient Resonance @ 8,75 Hz

or.ders

1000 RPM

O/A1I1.696 mm/s rms

PH FAN - FAN DE . Vertical-vel Spec 1$0 Hz Cursor A

11,625 Hz

0,612 orders

0,696 mOlls OIAlll,109 01011.

'm"

Max Speed 800 rpm (13.33 Hz)

IflIi 01-44_2009 18:29:48

O/A1I1.10e 01011. tmS

8

PH FAN FAN DE - Horizontal- Vel Spec 1000 Hz

Sub-harmonic@ 7.6 Hz

12.5

H~

m"

0665 OIA111.116

Operating Speed 945 rpm (15.7 Hz)

"' "" "'

"" "' I " "' "' " 1

9

30m

Top Deck 30mx10mx1.5mthk Ht. above zero Level 10m

[ A Typical TG Foundation)

10

o

l._--t-+- -r-+----+---I--c=l-----I--~--J

Pick~up Locations,

Top Deck Left Edge

:~/~-j



1_·"·__1,,,,,,,,,·+,·

:Pick-up Locations

i"Vertical Amplitudes

1,,,, -··!----------i----·····!·,·,,,,··+·-------r--··------!-----

plck··up Locatiom

Top Deck Right Edge

"'[

"

'----t-----+----+-~---c--+---+_r_----' Pick_up Locatiorl!;

Horizontal Amplitudes

210 MW TG Foundation - Top-Deck Vibration Record

Top

17 , ,

Bottom

COLUMNS

11

----

-

:

Typical Column Vibration Modes

12

Identical Foundations for Identical Machines on different soil c. ~

Foundation on Hard Rock

_.-

o

2

Distance in meters along length from Turbine end

13

Identical (adjacent) Foundations for Identical Machines on Identical Soil Top of Deck

Unit -2

::T

Unit -I

+

~

Base

--+ --I

o

20

:

I

40

I

--+---60

Vibration in microns

Vibration along column height

A uniform reduction of vibration amplitudes from top to bottom of bearing housing exhibits a healthy trend. For one of the bearing housing, the trend was opposite. Records are shown in Figure

Bearing

o

I

20

40

60

I

80

I

I

100

Vibration In microns

Amplitude along Bearing Height 200 MW TG Foundation

14

WARNING

MOTTO

There are many factors that significantly influence the response

15

Cost of Machine foundation

InadequatelY constructed foundations

Shutdown cost

Terminology Commonly Used in the Presentation DOF » SDOF )r 2 DOF » MDOF Damping Equation of equilibrium Equation of Motion Resonance Response )r Transient )r Steady State Amplitude Mass& MMI Stiffness );> Linear » Rotational

System Eccentricity Harmonics )r Sub harmonics '" Super harmonics Modes of Vibration Coupling of Modes Balance Grade Rotor Eccentricity Unbalance Force Short Circuit Torque Bearing failure Loads Thermal Loads Handling Loads Earthquake Loads

16

Basic Design Philosophy

Equation of Motion Free Vibration

Pv = Support

.

_ .v rad/s

~ m

17

\

Equation of Motion Forced Vibration

Support

....

-- ......... _.

Magnification

I I I I I I I I I I

l "---------

NOTOK

Response

I /

OK Strength Design

18

Strength Analysis & Design •

Short Circuit Forces



Earthquake Forces



Electro-magnetic Forces



Equivalent Dynamic Loads



Thermal Loads

Springs attached @ Centroid

19

Uncoupled Six Natural Frequencies

y

"

edt-x

About Axis

Along Axis

z

Pe=

ff e Mmx

--

x

,

Six DOr's 3 Dispalcements x, y, z along X, Y & Z axes respectively and 3 Rotations

e,

ljI,

¢

about X, Y & Z axes respectively

P==~

... -

Motion in X-V Plane y

A Rigid Block Supported by Translational & Rotational Springs

20

Natural Frequencies Limiting Frequencies PIfI::::

2

(2

2)

1 Px+p¢! --21 PI =-2-

Yz

Yz

~

FE --

M moy

J(Px+P¢ 2 2)' -4yzPxp¢ 22 1(--;

2 1 (2 ,) 1 2)' 22 p, ~-2- p, +p¢ +-2-'1 p, +P¢ -4y, P,P¢ y,

r Z

--

• -

-

• -

2 k 2 k¢ Px = -r , P¢ = - -

= Mill: .

m

Millo;'

Millo:

P2

• PI2

Pu or PLl eould either be Px or P¢

-

• -

y,

-

Pl.l

• -

PI

3 Frequencies

--7

Y3

Only One Frequency 2 Frequencies

= (k

p y

~;

y,~ k

2

Y,

f

Y1H=l

Y,

v~

~ 1 - OOF

System

2-DOF

System y

Frequencies are coupled

21

PI2 =

/1;

v-;;

Motion is coupled

k,

2-DOF System

Natural Frequencies

.-

--

Coupled Frequencies

P,&P2 • -

P2

- Pu • Pu

• -

• -

PI

Tube Bundle

DATA for Foundation Design :--

Equipment Data - Weight - Height of Centroid - Associated forces: - Seismic -Wind - Thermal - Nozzle Reactio n Forces - Frictional Forces - Thermal Loads :-- Foundation Data :-- Soil Data

Base Plate

Fixed Tube Heat Exchanger

22

Machine Data:

Coupling

DrIve MachIne

• Mass of Stator • Mass of Rotor • Operating Speed Driven Machme

A Typical Mlc Foundation System

• Gear ratio

• • • •

Unbalance Dynamic Forces Excitation Frequencies Number of Blades No. of Poles ( Electro magnetic forces) • Type of Bearing ( Journal Bearing or Anti-friction Bearing) • Permissible amplitudes

Foundation Data Soil data • Dynamic Soil Parameters

• Static Equipment

Dynamic Machine

EQPT

Frame or Block

Deck

Deck

Columns

Columns

Frame or Block

23

Equipment Foundation Static Analysis

y

l [mg JI

Equation of Equilibrium Weight

Is

T

k {

Soil + Col

~L Math. Model

== F kyO y =: mg

Displacement Oy = mg

ky

m= mass of Equipment +Deck + Columns + Raft

Strain; Estatic; Stress Shear Force & Bending Moment Structural Design

Representing by an Un-Damped SDOF System (S

Columns

Mathematica I M:.;:;o""de"'I'--_-"J

y = { ::} x

Response

{flJ

1

24

Equation of Motion

Response

System Property that Causes Vibration Amplitude to Diminish Steadily For Machine foundation, we consider Viscous Damping, where RESISTING FORCE is proportional to VELOCITY

25

my y Mass

Y

kv (Soil + Col)

Cy (Soil + Col)

In

~j

r

T

kyY

f CyY

Free Body Diagram

[EqUation of Motion]

Solution to equation of motion

The damping value for which the radical becomes zero is termed as Critical Damping of the system.

26

For Under-Damped System, Free Vibration Response becomes:

Constants A & B are evaluated using Initial Conditions

,,'--------------'/

27

1.'5 . .

1.0 0.5

o -0.5 -1.0

-1.5

Free Vibration Response Undamped System Sy" 0, Under-Damped ~J' < I

tiT

~~

..--+

Critically Damped

~y =

I & Over-Damped c"v > 1

28

y

!

Dynamic Force F(t)

m

~v (Soil + Col)

Response

Mass

y= Cy

1

(Soil + Col)

y

f.J f.J y

Forced Vibration Equation ofMotion

= J(1-fJ:)'+(2fJ/;) = Dyn. Mag. Factor

py=)~; f3y=~;; Sy = damping constant

I Equipment Foundation]

Displacement

5=~ y k

[ Machine Foundation]

Response

y

f.J y

y={~}xi~)

= Dyn. Mag. Factor

29

r---

I~~,o I .\

5j 41 ~.

:;

~

=

0

.~

u

'"§,

J

j Resonance

2~

I !~,

!

.j:'

;;: I

I 0

0.5

0

J'n

fi

0.1

= y

1

~(I- 13;) + (213y sy ~ = 1.,

fl.

y

I

=

(2 S y)

I

'7f

rn

fly

For 2% damping fly = 25 For5%dampingfly =10 For 10% damping fI" = 5

~ 2.0

1.5 Frequency Ratio

2,5

3.0

~~

Points to Note That in case of machine foundation design ... •

Machines weigh several tons



Foundation overall dimensions runs in multiple of meters



Columns sizes are relatively large say 1m x 1.5 m or so



Beam sizes are also relatively large say 1m wide and 1.5 m to 2.0 m deep



Dynamic Forces in several tons

30

All those elements which contribute to mass and lor stiffness must not be ignored

All the assumptions and approximations made during modeling must be duly validated

• Natural Frequency • Excitation Forces • Excitation Frequencies

31

,tfI"'-------, \

:8

Machine

+

: Response

~=8

y==t~}xl~)

I I Foundation

I \

Support

,-------'"

32

Machine Mass - Point of Application

Excitation Forces - Point of Application

33

Machine Centroid

~

Actual ,"-o OJ

Py < OJ

Frequency Margin + 20 %

4

01""·""··.,. 0,5 o

."., O,K

10

1.2

15

2,0

2.5

),0

Frequency Ratio fJ

Magnification Factor p vs. Frequency Ratio rl ± 20% Frequency Margin Region

44

Fr~!l1e

Foul1d"tion ,,~

Column sizes (as marked on the layout drawing) are generally provided by the customer/supplier. More often than not, it has become the practice by the designers to stick to these dimensions Such a practice is undesirable and must be discouraged. Given sizes should be taken as indicative only and the designer must assess the validity of keeping in view the Top Deck Eccentricity -------------'

Max Displacement

38~7

Columns Original

mm

Max Displacement

28~8

mm

Columns Modified

45

.. l!!!.!Im .

---

e:t

Why do we need such thick sections for Frame Foundation? •

46

Rotor Catenary Like a rope

Differential Settlement along Length

Every Mode Shape and associated Frequency does convey a message that must be well understood by the designer.

47

&

48

.. • Shear Modulus • Coefficient of Sub-grade Reactions • Soil damping • Soil Mass participation

Pile stiffness Properties • Single Pile - Load Test o Vertical Stiffness o Lateral Stiffness o Damping • Pile Groupo Vertical Stiffness o Lateral Stiffness o Damping

49

IEffect due to static streststevetl I--~~~~~~~~~~~....,r-

Suffix 01 - Test Level Suffix 02 - Foundation Level

Formation Levei

Foundation Level

• WHETHER SOIL BEHAVES LIKE AN ELASTIC BODY? • WHETHER IT OBEYS HOOK'S LAW?

Presumption: Foundation undergoes elastic vibrations as long as the total pressure (including static & dynamic pressure) on the soil is lower than its elastic limit

50

It is the Ratio of Pressure to Deformation

Uniform Compression

FI,

y

Uniform Shear

.....J .....

Non-uniform Compression

Non·uniform Shear

Foundnlion

Fy

Block

c ~!2~ "

z

Soil

und~r

y

A y

~!2. Ay

UnifonTI Compression

Force ~v Applied to the Foundation Block Resting over the Soil

E 1 C ~1.l3~ /, u \l-v· IvA 4 G ro 1 I-v A

---

E

G=

2(1 + v) A

~ If

ro2

Coefficient of Non- Uniform Compression

Coefficient of Uniform Shear

Coefficient of Non- Uniform Shear

C .J.. = 0.5 Cu C 1=1.5

C,

51



Foundation Supported directly over Soil



Foundation Supported over Piles

Linear Springs F

k =----'-=C xA x x T

Rotational Springs ko=MO=CDxl f) v xx

F

k y =---"'-=C u xA y

F

k

=_Z

Z

z

=C xA T



k. =-=Cxl 'I'

¢

'I'

zz

52

Soil Mass participation

oo==:;>

No-Soil Mass participation

Embedment Effect

DO==:;>

Results in increased Damping

Soil damping

DO==:;>

8 to 10 %

1. Understanding the dynamic behaviour of a single pile as well as group of piles - Definite gaps exists 2. Dynamic characteristics of piles - Complex Task and suffers with many Associated Uncertainties 3. Dynamic Behaviour of Group of Piles - is still considered to be in its Infancy 4. Reliability of dynamic characteristics? - Reliability computed dynamic response?

53

Vertical pile stiffness (k v ) and Lateral pile stiffness ( k h )

• Foundation: • Pile:

Length 'L', Width 'B' and Depth 'H' Diameter'd' & Pile spacing's'

Piles are so placed that their spacing along length and width of the foundation remains same. Influence Coefficient 0.65 aejf

=0.212 ( ;

)

Effective vertical stiffness of each pile Effective lateral stiffness of each pile Pil,S",,10' { PIle D,ameter

(!..)} d

"'ff } { Coemcien t as Proposed

{co'm:':, Aft" BM"O} Tablel-14 pp48

033 )

043

4 45

0.52 0.56 0.60 0.68

5 6

041 0.64 0.65

This empirical relationship provides a fairly good estimate of influence coefficient of a single pile

54

Case Studies Field Perform·ance

55

Whenever high vibrations are notice on any machine . • In 9 out of 10 cases, the blame always goes to machine manufacturer • In 50 % of the cases, the source of the problem may not be machine alone and solution may lie somewhere else • Each and every associated segment tries to play safe and becomes defensive • It results in -Delay in finding solution It requires Right Attitude to tackle all failure problems with of course Right Team of Experts armed with Right Instrumentation

• A uniform reduction of vibration amplitudes from top to bottom of bearing housing exhibits a healthy trend. • For one of the bearing housing, the trend was opposite. _ Records are shown in Figure Bearing

4 1325

~l Ji

0

d·,..e:--+_.::l,

.1 .. : "- '\. .J r , ""

/

11

o

--I

20

!

I

40

"Bearln!!

"

I _·+-+-t--t-"1

60

80

100

Vibration In microns

Amplitude along Bearing Height 200 MW TG Foundation

56

• The grout underneath the bearing seating plate was totally carbonized perhaps due to chemical reaction of the grout with spilled oil • It behaved like charcoal powdery cake having no strength and it was fully soaked in oil. • After re-grouting the pedestal the problem disappeared

I3ctlow

o o~_~

, i

Compressor

o

_ Base Plate

o

i

I

o

o o

D ,~-----

I

PLAN

----

o

LC

-===='==:;::==~_ 0

Vibration pick up Location

~\r-::-!~~-~~~~~1!

SECTION

Motor Compre~sor Unit on a Block Foundation

57

Vibration measurement records at various pick-up locations

Longitudinal

Transverse

Vertical

40

Foundation Base frame Channel

40

20

Base Plate Motor Tank

Compressor

NRV Piping

25 60/420

~ I I 500

1500

150

125

150

90

300

~

I I 2600 I 11000

100

I

800

I

• High base plate vibration indicated loosening of foundation bolts. • Close examination· revealed broken welding of support lug to base frame. • Repair of support lug and tightening foundation bolts brought down vibration level from 420 microns to 130 microns. • This also brought down compressor vibration levels to 250 /300 /250 microns in X N /Z direction • High piping vibration levels suggested need to isolate NRV. • Isolation of NRV resulted in drastic reduction of vibration all through. NRV levels were still around 200 microns.

58

• A reciprocating compressor on a frame foundation was to be located inside a plant building. • Dynamic forces developed by compressor were extremely high • Supporting the foundation over the soil results in excessive amplitudes of vibration • The size of the base raft also can not be increased because of restrictions imposed by other structural foundation.

The only options were i) either to strengthen the soil by whatsoever possible means, ii) resort to pile supported foundations or iii) use strong stiffness material underneath the base of the foundation so as to limit the amplitudes within permissible levels. The decision by the company was to resort to isolation technique and design the foundation.

59

,----------- -

Machine

/

I

..

1 [J . ~t· i,(_

"

'1[:':::_: '

,. ..

Detail· A

.

Isolation Pad f Cork Pad Placement of Isolator In case of Frame Foundation

• A common raft was provided spanning across width of the building • Compressor foundation was placed over the raft with Cork as Isolation device so as to minimize transmission of forces from machine to the common foundation • This system was designed by the author in 1974 • With this arrangement Machine was installed and has run satisfactorily keeping the amplitudes within permissible limits

60

Cork thickness of 75 mm below the frame foundation was found to be adequate. Cork properties were tested at one of the national laboratory. Recommended values for computation are as under: Compressive strength Elastic Modulus (Static) Elastic Modulus (Dynamic) Coefficient of Uniform Compression

500 kN/m2 10 MPa 15 MPa

20 x 10 4 kN/m 3

• The concept was used once again by the author, in 1979, for design of a Frame Foundation for a Gas Turbine.

• The need arose because of slip during planning. While making the layout, not adequate space was left to accommodate the GT. • Unlike previous case, the machine is a high rpm machine and it was rather easy to get the required frequency ratio for achieving desired isolation.

• The success has given improved confidence level for such designs.

61

Dissimilar vibration behaviour of Two Identical Units on Identical Foundations placed next to each other • Machine was running with high vibrations since a decade and a half. • High column vibrations as well as high deck vibrations are reported in one unit whereas another identical unit just adjacent to it is reported running satisfactorily. • Cracks at the column top below deck have also been observed. These are perhaps locations of construction joint of column with top deck.

26.0 OJ

o '"

-- -

I {9-- -

2 45 67 -e----®3 - - - - - - - ®® - - -- - -- -- - ® - ® - . Bearing #

--------'

A 210 MW T G Foundation (Typical) - Top Deck Plan Showing Column and Bearing Locations

62

Bearing Vibrations

~

75

ji'

50

§

s

Horilonlal

75

50

.g

? 25

n

25

0E

< 0 j..LILL.lL..UIl...LJLL.lL..UIlJ 2

3

Vertical

Axial

Bcaring Numbers

Bearing Nwnbers

JOO

4

5

0

6

Bearing Numbers

~

2

III Unit 2 Bearing Level Amplitudes Turbo Generator Units! & 2

Top Deck Vibrations

i~ ~,-

I(,

\6

"

16

I I I \

rI I

j

I

"---

.:.100 (I zon Cols A

I)

B

" , ,

169

2<

-I

I)

r:

\

I I

I

200 -200

49

\

I

I

12 \0

I \

I

L

"

L

I

\

I

·200 () 201l -2-00

F

\ \ \ \ \ \ I

,

I)

:100 -200 0200 -200 I) ZOO -200 I) '201l II K L

A~,i.r!J,Amp-lil\I!l~..lm,i~[,\lfl~.l

Amplitude Variation in Columns Along Height Axial Amplitudes

64

• Ratio of bearing amplitudes of two units is of the order of 3 • Ratio of top deck amplitudes is of the order of 2 • It is a wild guess and a question mark whether cracking of the columns at top (close to deck bottom (soffit of beam) is responsible for such a behaviour or such high vibrations have resulted in cracking of the column? • Visual examination of the column vibration and plot of amplitudes indicate that 2nd mode frequency of some of the individual columns in transverse direction has tendency to be in resonance with operating speed. Similar behaviour is also noticed for some columns in axial direction.

FFT analysis of column vibrati.on • FFT analysis of records confirm to the above observation. • It is seen that the resonant frequency of some of the columns lie close to 50 Hz which is the machine running speed. • Though the amplitude levels are low, the trend is not healthy. • It is primarily because the analytical tools available about two decades back were not adequate to carry out such a detailed analysis and moreover the need was neither emphasized by the owner I customer nor by machine manufacturer.

65

Col A 1,!llil

Unll I

-

1

To be

noted that scales are d,lfferent Ihthese

, ,;dlagrams Fr~'1l1en~y

-

in rPM

--'1 1

I i

, '0

1(0

,

I .i

1JLi'" ,

10

10

,

10

Frequency in C1'M

F!'(\I\I",1
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