comparision of pressure vessel codes

24
Comparison of pressure vessel codes Why do the codes differ and How do they differ Presented by: Ray Delaforce 3/24/2011 By Ray Delaforce 03/24/11 By Ray Delaforce

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Co

mp

ari

so

n o

f p

res

su

re v

es

se

l c

od

es

Wh

y d

o th

e c

od

es d

iffe

r a

nd

Ho

w d

o th

ey d

iffe

r

Pre

sente

d b

y:

Ray D

ela

forc

e

3/2

4/2

011

By R

ay D

ela

forc

e

03

/24/1

1

By R

ay D

ela

forc

e

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

es

e a

re t

he

co

de

s w

e a

re g

oin

g t

o c

om

pa

re:

•A

SM

E S

ecti

on

V

III, D

ivis

ion

1

•A

SM

E S

ecti

on

V

III, D

ivis

ion

2

•P

D 5

500

•E

N 1

3445 P

art

3

Bu

t fi

rst

we

lo

ok

at

the

mo

st

fun

da

me

nta

l re

qu

ire

me

nt

Wh

at

is t

he A

LL

OW

AB

LE

ST

RE

SS

?

Th

is is t

he p

rim

ar y

str

ess w

e m

ust

no

t exceed

y

A P

RIM

AR

Y s

tre

ss

re

su

lts

fro

m in

tern

al

pre

ss

ure

Th

ere

are

SE

CO

ND

AR

Y s

tre

ss

es

–w

e d

o n

ot

dis

cu

ss

th

em

3/2

4/2

011

By R

ay D

ela

forc

e

03

/24/1

1

By R

ay D

ela

forc

e2

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

We

fir

st

loo

k a

t a c

ou

ple

of

imp

ort

an

t m

ate

rial p

rop

ert

ies

Let

us lo

ok a

t th

e S

tress-S

train

dia

gra

m –

we g

et

a lo

t o

f in

form

ati

on

El

ti

Co

llap

se c

an

occu

r w

hen

we r

each

th

e y

ield

po

int

Le

t u

s l

oo

k a

t th

e i

mp

ort

an

t fe

atu

res

of

ou

r s

tee

l

Ela

sti

c

Ra

ng

eP

lasti

c R

an

ge

Fra

ctu

re

Du

cti

leR

an

ge

ess !

Yie

ld P

oin

t

Du

cti

le R

an

ge

All

bl

St

bt

h

Stre

Allo

wab

le S

tresses a

bo

ut

here

3S

train

"0.2

% s

train

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us lo

ok a

t th

e S

tress-S

train

dia

gra

m –

we g

et

a lo

t o

f in

form

ati

on

Co

nsid

er

ste

el:

U

TS

= 7

0 0

00 p

si (4

82 M

Pa)

Yie

ld 3

8000 p

si (2

62 M

Pa)

Co

llap

se c

an

occu

r w

hen

we r

each

th

e y

ield

po

int

Le

t u

s l

oo

k a

t th

e i

mp

ort

an

t fe

atu

res

of

ou

r s

tee

l

Th

ere

are

th

ree im

po

rtan

t fe

atu

res w

e m

ust

co

nsid

er

1.

Th

ere

is t

he l

imit

of

pro

po

rtio

nality

Y

ield

Po

int

0.2

% s

train

2.

Th

e U

ltim

ate

Te

nsile S

tren

gth

(U

TS

) W

hen

fra

ctu

re o

ccu

rs

3.

Th

e D

ucti

lity

=

Yie

ld / U

TS

M

ust

be less t

han

1.0

Th

ere

is a

4th

on

e –

Cre

ep

wh

ich

occu

rs a

t h

igh

er

tem

pera

ture

s

4

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Allo

wab

le s

tress

is b

as

e o

n t

he

se

ch

ara

cte

ris

tic

s o

f th

e m

eta

l

AS

ME

Secti

on

VIII

Div

isio

n 1

AS

ME

Secti

on

VIII

Div

isio

n2

S =

sm

aller

of:

U

TS

/ 3

.5 o

r Y

ield

/ 1

.5

= 2

0 0

00 p

si

(138 M

Pa)

AS

ME

Secti

on

VIII

Div

isio

n 2

EN

13

44

5

Sm

= s

maller

of:

U

TS

/ 2

.4

o

r

Yie

ld / 1

.5

Bo

thb

ased

on

PE

DE

uro

pean

req

uir

em

en

ts

= 2

5 3

00 p

si

(174 M

Pa)

EN

13

44

5

f =

sm

all

er

of:

U

TS

/ 2

.4 o

r Y

ield

/ 1

.5

Bo

th b

as

ed

on

PE

D E

uro

pean

re

qu

ire

me

nts

= 2

5 3

00 p

si

(174 M

Pa)

PD

5500

f =

sm

all

er

of:

U

TS

/ 2

.35

or

Y

ield

/ 1

.5

= 2

5 3

00 p

si

(174 M

Pa)

5W

e c

on

sid

er

Carb

on

Ste

el fo

r sim

plicit

y

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

We

lo

ok a

t th

is o

n t

he S

tress S

train

dia

gra

m

AS

ME

VIII, D

ivis

ion

1 h

as a

larg

er

safe

ty m

arg

in –

safe

r

Th

is c

od

e is s

till t

he f

avo

ure

d c

od

e t

hro

ug

ho

ut

the W

orl

d

ess !

Yie

ld P

oin

t

AS

ME

VIIID

ii

i1

AS

ME

VIII D

ivis

ion

2, E

N 1

3445 &

PD

5500

Stre

AS

ME

VIII D

ivis

ion

1

Str

ain

"6

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the c

ylin

dri

cal

sh

ell

Here

are

th

e b

asic

dim

en

sio

ns

We

sh

all i

gn

ore

jo

int

eff

icie

ncy E

(z)

Wd

thl

lti

fth

lid

P=

300 p

si

(207 M

Pa)

D=

60 i

ns (

1 5

24 m

m)

We n

ow

do

th

e c

alc

ula

tio

n f

or

the

cy

lin

de

r:

t =

0.4

54

in

(11

.53

4 m

m)

By A

SM

E V

III

Div

isio

n 1

S(f

)=

20 0

00 p

si

(174 M

Pa)

By A

SM

E V

III

Div

isio

n 2 t=

0.4

53

in(1

1.5

16

mm

)t

0.4

53

in

(11

.51

6 m

m)

By E

N 1

3445

DO

Di

7tA

SM

Ee

EN

13445 &

PD

5500

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the c

ylin

dri

cal

sh

ell

Here

are

th

e b

asic

dim

en

sio

ns

We

sh

all i

gn

ore

jo

int

eff

icie

ncy E

Wd

thl

lti

fth

lid

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the E

llip

tical

Head

P=

300 p

si

(207 M

Pa)

D=

60 i

ns (

1 5

24 m

m)

We n

ow

do

th

e c

alc

ula

tio

n f

or

the

cy

lin

de

r:

t =

0.4

54

in

(11

.53

4 m

m)

By A

SM

E V

III

Div

isio

n 1

S(f

)=

20 0

00 p

si

(174 M

Pa)

By A

SM

E V

III

Div

isio

n 2 t=

0.4

53

in(1

1.5

16

mm

)t

0.4

53

in

(11

.51

6 m

m)

By E

N 1

3445

t0

45

3i

(11

51

6)

Th

at

is w

hy t

he d

iffe

ren

ces

are

so

sm

all –

the f

orm

ula

e

are

nearl

y t

he s

am

e !

t =

0.4

53

in

(11

.51

6 m

m)

By P

D 5

500

t=

04

53

in(1

15

16

mm

)

Th

is f

orm

ula

lo

oks o

dd

,

bu

t is

actu

ally j

ust

ab

ou

t

8

t =

0.4

53

in

(11

.51

6 m

m)

the s

am

e a

s t

he o

thers

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the c

ylin

dri

cal

sh

ell

Here

are

th

e b

asic

dim

en

sio

ns

We

sh

all i

gn

ore

jo

int

eff

icie

ncy E

Wd

thl

lti

fth

lid

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the E

llip

tical

Head

We n

ow

do

th

e c

alc

ula

tio

n f

or

the

cy

lin

de

r:

t =

0.4

54

in

(11

.53

4 m

m)

By A

SM

E V

III

Div

isio

n 1

Cylin

der

based

on

the

By A

SM

E V

III

Div

isio

n 2 t=

0.4

53

in(1

1.5

16

mm

)

Cylin

der

based

on

th

e

eq

uilib

riu

m e

qu

ati

on

t 0

.45

3 in

(11

.51

6 m

m)

By E

N 1

3445

t0

45

3i

(11

51

6)

Th

at

is w

hy t

he d

iffe

ren

ces

are

so

sm

all –

the f

orm

ula

e

are

nearl

y t

he s

am

e !

t =

0.4

53

in

(11

.51

6 m

m)

By P

D 5

500

t=

04

53

in(1

15

16

mm

)

Th

is f

orm

ula

lo

oks o

dd

,

bu

t is

actu

ally j

ust

ab

ou

t

9

t =

0.4

53

in

(11

.51

6 m

m)

the s

am

e a

s t

he o

thers

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the E

llip

tical

Head

Min

or

Sh

ap

e is b

ased

on

tru

e e

llip

se

Majo

r

hD

/2h

= 2

P=

300 p

si

(207 M

Pa)

D60

i(1

524

)

DA

SM

E D

ivis

ion

1 –

sim

ple

calc

ula

tio

nA

SM

E D

ivis

ion

2 –

co

mp

licate

d c

alc

.

D=

60 i

ns (

1 5

24 m

m)

S(f

)=

20 0

00 p

si

(138 M

Pa)

t =

0.4

51

in

t

= 1

1.4

47

mm

Head

form

ula

alm

ost

iden

tical

toth

ecylin

der

form

ula

:H

ea

d f

orm

ula

alm

os

t id

en

tical to

th

e c

ylin

der

form

ula

:

Ellip

tical

head

: C

ylin

der:

10

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Let

us n

ow

lo

ok a

t a t

yp

ical

calc

ula

tio

n –

the E

llip

tical

Head

Min

or

Sh

ap

e is b

ased

on

tru

e e

llip

se

Majo

r

hD

/2h

= 2

P=

300 p

si

(207 M

Pa)

D60

i(1

524

)

DA

SM

E D

ivis

ion

2 –

co

mp

licate

d c

alc

.

1 T

here

are

man

y s

tep

s t

o d

o

D=

60 i

ns (

1 5

24 m

m)

S(f

)=

25 3

00 p

si

(174 M

Pa)

2 C

an

no

t c

alc

ula

te t

dir

ectl

y .

.

.o

nly

P

Div

isio

n2

allo

ws

hig

her

str

ess

On

th

e n

ext

slid

e w

e s

ho

w t

he c

alc

ula

tio

n p

er

PV

Eli

te

Div

isio

n 2

allo

ws

hig

her

str

es

s

11

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

Th

e E

llip

tical

head

is t

ran

sfo

rmed

in

eq

uiv

ale

nt

To

risp

heri

cal

Head

12

Cro

wn

rad

ius

Kn

uckle

rad

ius

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

Next

we m

ust

calc

ula

te s

om

e g

eo

metr

y f

acto

rs

13

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

Even

mo

re g

eo

metr

y a

nd

oth

er

facto

rs…

……

Even

mo

re g

eo

metr

y a

nd

oth

er

facto

rs a

nd

mo

re –

lots

of

facto

rs

14

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

Even

mo

re g

eo

metr

y a

nd

oth

er

facto

rs a

nd

mo

re –

lots

of

facto

rs

Fin

ally

we

en

du

pw

ith

ou

rsta

rtin

gp

ressu

re

15

PV

Elite

do

es a

n i

tera

tive c

alc

ula

tio

n t

o e

nd

up

wit

h t

he p

ressu

re

Fin

ally w

e e

nd

up

wit

h o

ur

sta

rtin

g p

ressu

re

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

We

had

to

sta

rt t

he c

alc

ula

te w

ith

a ‘g

uess’ th

ickn

ess t

An

d w

e e

nd

ed

up

wit

h o

ur

sta

rtin

g p

ressu

re

We

have t

o u

se a

co

mp

ute

r to

do

th

is c

alc

ula

tio

n !

Th

e c

om

pu

ted

th

ickn

ess is t

= 0

.32

19

in

t

= 8

.17

67

mm

16

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

-A

SM

E D

ivis

ion

2

EN

13445 h

as a

sim

ilar

meth

od

–s

lig

htl

y l

ess c

om

plicate

d t

han

AS

ME

Th

e f

inal co

mp

ute

d t

hic

kn

ess is:

t

= 0

.3886 in

t

= 9

.8619 m

m

17

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

e m

eth

od

of

co

mp

uti

ng

th

e h

ead

by P

D 5

500 is v

ery

dif

fere

nt

Min

or

1 C

alc

ula

te

h /

D =

0.2

5

Majo

r

h2 C

alc

ula

te

P /

f =

0.1

19

P=

300 p

si

(207 M

Pa)

D60

i(1

524

)

D

D=

60 i

ns (

1 5

24 m

m)

f=

25 3

00 p

si

(174 M

Pa)

PD

5500 u

ses a

gra

ph

ical so

luti

on

s –

like t

his

18

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Here

is t

he G

rap

h u

sed

to

co

mp

ute

th

is h

ead

th

ickn

ess

1 C

alc

ula

te

h /

D =

0.2

5

2 C

alc

ula

te

P /

f =

0.1

19

e / D

e =

D x

(e

/D)

19

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

re v

essel co

des

Th

is i

s t

he c

alc

ula

tio

n u

sin

g P

V E

lite

t =

0.3

792 in

t

= 9

.6317 m

m

Each

co

de h

as i

ts o

wn

way o

f co

mp

uti

ng

a h

ead

–a

nd

oth

er

part

s

Bu

t, w

here

do

co

des ‘b

orr

ow

’ p

roced

ure

s f

rom

oth

er

co

des ?

20

CO

MP

AR

ISO

N o

f th

e v

ari

ou

s p

ressu

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CO

MP

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N o

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CO

MP

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N o

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We

have lo

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f co

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We

have learn

ed

so

me im

po

rtan

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su

es

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AS

ME

VIII D

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en

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AS

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)

24

It i

s h

op

ed

yo

u g

ot

so

me v

alu

e o

ut

of

this

web

inar