BISMV & H 0 -H - psb injection VACUUM REQUIREMENTS

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BISMV & H 0 -H - PSB INJECTION VACUUM REQUIREMENTS LIU - PSB meeting 29th October 2012 C. Pasquino, P. Chiggiato, J. Hansen

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BISMV & H 0 -H - psb injection VACUUM REQUIREMENTS. C. Pasquino, P. Chiggiato, J. Hansen. Outline. BISMV vacuum layout; Graphite outgassing tests; Simulation results; PSB injection vacuum layout; Simulation results; SiC outgassing rate measurements; Conclusions and actions. - PowerPoint PPT Presentation

Transcript of BISMV & H 0 -H - psb injection VACUUM REQUIREMENTS

Page 1: BISMV  & H 0 -H - psb  injection  VACUUM  REQUIREMENTS

BISMV & H0-H- PSB INJECTION VACUUM REQUIREMENTS

LIU - PSB meeting 29th October 2012

C. Pasquino, P. Chiggiato, J. Hansen

Page 2: BISMV  & H 0 -H - psb  injection  VACUUM  REQUIREMENTS

Outline• BISMV vacuum layout;• Graphite outgassing tests;• Simulation results;• PSB injection vacuum layout;• Simulation results;• SiC outgassing rate measurements;• Conclusions and actions.

LIU - PSB meeting 29th October 2012

Page 3: BISMV  & H 0 -H - psb  injection  VACUUM  REQUIREMENTS

BISMV – vacuum layout

LIU - PSB meeting 29th October 2012

3 Sputter Ion pumps Starcell 500

2 Sputter Ion pumps Starcell 300

Page 4: BISMV  & H 0 -H - psb  injection  VACUUM  REQUIREMENTS

Bismv – gas loads

LIU - PSB meeting 29th October 2012

Unbaked tank = water vapor outgassing

Magnets outgassing, measured by I. Wevers (EDMS 1097059)

Graphite dumps: thermal outgassing

2

9

**

][10*3

2 cmslmbar

htQ OH

2

12

**10*1

2 cmslmbarQH

212

**10*2

)50(2 cmslmbarQ

CH

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LIU - PSB meeting 29th October 2012

Graphite outgassing test: pumpdown and thermal outgassing

 

R4450 LHC collimator graphite Furnace treatment, 2 hours at 950 ◦C Bakeout ≈ 24 hours at 200 ◦C

Measurement procedure: Pumpdown of 24 hours Bakeout Step of ∆T = 25 ◦C from room

temperature to 200 ◦C Same procedure is followed for the

background signal measurement.In a second measurement campaign a thermocouple was inserted directly to the graphite block to check the effective temperature reached by the latter.

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LIU - PSB meeting 29th October 2012

Graphite outgassing test: pumpdown

The more the graphite is exposed to air the more it outgas.

1st time: A few hours only after the vacuum firing treatment;

2nd time: Following the first measurement and 24 h exposure to the lab

air;

3rd time: Following the second measurement and

weeks of exposure to lab air.

1st and 2nd measurement ≤4*10-10 mbar l/s cm2

3rd measurement 2*10-09 mbar l/s cm2

Outgassing at 10 hours of pumpdown

EDMS DOCUMENT : 1254422

0.1 1 1010-7

10-6

10-5

10-4

10-3

Q (m

bar l

/s)

t (h)

third measurement second measurement first measurement background

Pumpdown

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LIU - PSB meeting 29th October 2012

Graphite outgassing test at different temperatures

0 15 30 45 600

255075

100125150175200225250

T (C

)

t (h)

Graphite Vacuum Chamber

Temperature steps

25 50 75 100 125 150 175 200 22510-13

10-12

10-11

10-10

10-9

10-8

Q (m

bar l

/s cm

2)

T (C)

Q

R4450 Graphite Outgassing

with BG subtracted

Thermal outgassing at 200 ◦C is 4 orders of magnitude higher than at 50 ◦C

Equivalent to 2500 cm2 of SS at RT

0 15 30 45 6010-10

10-9

10-8

10-7

10-6

P to

t (m

bar)

t (h)

P tot

TEMPERATURE

PRESSURE

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BISMV1 BISMV2 BISMV3 BISMV410-10

10-9

10-8

P (m

bar)

Position

N2 Equivalent

BISMV tank pressure profile: graphite at 50C

Electrical network – vacuum analogy simulations

LIU - PSB meeting 29th October 2012

Water vapor outgassing at 100 hours of pumpdown; Outgassing at 50 ◦C and at 200 ◦C from the graphite; H2 outgassed from the bulk metal & magnets; Scrapers or pickups are calculated as equivalent to a dump outgassing NO HEATING OF THE SURROUNDING CONSIDERED.

P tot = 3*10-9 mbar

BISMV1 BISMV2 BISMV3 BISMV410-10

10-9

10-8

Parti

al Pr

essu

re (m

bar)

Position

H2 H2O

dump graphite - 50 C

BISMV1 BISMV2 BISMV3 BISMV410-10

10-9

10-8

Parti

al Pr

essu

re (m

bar)

Position

H2 H2O

graphite dump updated surface_200C

BISMV1 BISMV2 BISMV3 BISMV410-10

10-9

10-8

10-7

P (m

bar)

Position

N2 Equivalent

BISMV tank pressure profile: graphite at 200C

P tot = 1*10-8 mbar

+

+

Page 9: BISMV  & H 0 -H - psb  injection  VACUUM  REQUIREMENTS

PSB H- Injection: vacuum layout

LIU - PSB meeting 29th October 2012

Linac 4 H-

PSB ring

SIP 1

SIP 2

RF shield

Stripping foil

Internal dump

Gate Valve

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LIU - PSB meeting 29th October 2012

Electrical network – vacuum analogy simulations

intertank BSW4 BSW4

10-10

10-9

10-8

Parti

al Pr

essu

re (m

bar)

position

H2 50C H2O

Graphite dump at 50 C

intertank BSW4 BSW4

10-10

10-9

10-8

Pres

sure

(mba

r)

position

Ptot (N2 eq)_50

Ptot = 6*10-9 mbar

Ptot = 3*10-9 mbar

Water vapor outgassing at 100 hours of pumpdown; Outgassing at 50 ◦C and at 175 ◦C from the graphite; NO HEATING OF THE SURROUNDING CONSIDERED.

H2O driven

H2 driven

intertank BSW4 BSW4

10-10

10-9

10-8

Parti

al Pr

essu

re (m

bar)

position

H2 175C H2O

Graphite dump at 175C

intertank BSW4 BSW410-10

10-9

10-8

Pres

sure

(mba

r)

position

If the graphite is treated at the furnace, baked and actively cooled (50 ◦C) the 75 l/s SIP can cope with

this extra gas load.

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LIU - PSB meeting 29th October 2012

SiC outgassing rate measurements: pumpdown

EkaSiC T plus and EkaSiC G tested in pumpdown: No cleaning No heat treatment Tested as received

(vacuum fired by the company?)

It outgasses as a metallic surface!

No difference between the two different grades.

0.1 1 1010-8

10-7

10-6

10-5

10-4

Q (m

bar l

/s)

t [h]

BGD SiC Tplus SiC G

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LIU - PSB meeting 29th October 2012

SiC outgassing rate measurements: accumulation measurements 1/2

After a bake-out at 150 ◦C, the system is cooled down at room temperature: the variable leak valve is closed in order to isolate the sample from the system.

It is possible to measure the outgassing as a function of the heating temperature.

The evaluation of the background is mandatory.

0 30000 600000.0

3.0x10-7

6.0x10-7

Gas Q

uant

ity (T

orr l

)

accumulation time (s)

Hydrogen Linear Fit of Quantity

Equation y = a + b*xAdj. R-Square 0.99922

Value Standard ErrorQuantity Intercept 1.41302E-8 5.29923E-9Quantity Slope 1.02257E-11 1.64682E-13

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LIU - PSB meeting 29th October 2012

SiC outgassing rate measurements: accumulation measurements 2/2

0 30000 6000010-10

10-9

10-8

10-7

10-6

2 15 28 44

Gas Q

uant

ity (T

orr l

)

accumulation time (s)

EkaSiC G outgassing at 50C

By heating the sample, we can evaluate the outgassing as function of different heating temperatures: the last heating steps on the EkaSiC G are on-going.The evaluation of the background as function of the heating temperature is needed to calculate the samples outgassing..

Q H2 Q CH4 Q CO Q CO2

Torr l/s cm2 Torr l/s cm2 Torr l/s cm2 Torr l/s cm2

EkaSiC G 1.2*10-13 1.7*10-15 3.5*10-15 9.9*10-15

Degassing values at room temperature (20 ◦C) with BG subtracted!

We are background

limited…

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LIU - PSB meeting 29th October 2012

Conclusions and actions• The BISMV and the PSB H – injection area have been considered from the

vacuum point of view;• The R4450 graphite outgassing has been tested at different temperatures

from room temperature up to 200 ◦C;• The results of the simulations show that the graphite is compatible with

UHV systems only IF:1. Vacuum firing at 950 ◦C for 2 hours;2. In – Situ bake out at 200 ◦C for 24 hours;3. Working temperature of the graphite block T = 50 ◦C.• Outgassing rate measurements of the SiC are on going but from the very

first results, it looks very promising for UHV applications.