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Temperature rise of SVD2 IR beampipe during single beam study Samo Stanič, SVD Meeting 2003/10/30

Temperature rise of SVD2 IR beampipe during single beam study

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Temperature rise of SVD2 IR beampipe during single beam study. Samo Stani č, SVD Meeting 2003/10/30. Single beam study LER I max =1A, i max =0.84 mA n b = 1187 bunches (1 train, fill pattern 10x4+1x5) HER I max =0.6A, i max =0.805 mA n b = 745 bunches - PowerPoint PPT Presentation

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Page 1: Temperature rise of SVD2 IR beampipe during single beam study

Temperature rise of SVD2 IR beampipeduring single beam study

Samo Stanič, SVD Meeting   2003/10/30

Page 2: Temperature rise of SVD2 IR beampipe during single beam study

Single beam study

LER Imax=1A, imax=0.84 mA   nb = 1187 bunches(1 train, fill pattern 10x4+1x5)

HER Imax=0.6A, imax=0.805 mA   nb = 745 bunches (16 trains, fill pattern 10x4+1x5, gap 120 buckets)

HOM power estimate in Be

PHOM = kl I2 / (fb nb) = kl i2 nb / fb

fb = 100 kHz kl (Be) = 0.01-0.02 V/pC (ABCI est. for BL=6mm)

Pgen(LER)= 85-170W Pgen(HER) = 50-100WPmax(LER)= 4-9W Pmax(HER) = 2-5W (assuming max 5% goes into heat)

Page 3: Temperature rise of SVD2 IR beampipe during single beam study

SVD2 IR beampipe temp. sensors

6 sensors on Be

4 sensors on manifolds

7 sensors in BWD(incl. 1 on and 1 behindCu Cooling block)

8 sensors in FWD(incl. 1 on and 1 behindCu Cooling block)

24 7

Page 4: Temperature rise of SVD2 IR beampipe during single beam study

On cooling block

On manifold

On Be

Behind cooling block

RTD Around the manifold

Page 5: Temperature rise of SVD2 IR beampipe during single beam study

RTD under BWD mask

RTD behind BWDCu block

RTD on Be staggered in phi(2 are hidden)

Page 6: Temperature rise of SVD2 IR beampipe during single beam study

Locations of temp. sensors on the beampipe:full phi and z coverage

Page 7: Temperature rise of SVD2 IR beampipe during single beam study

We know exact temperatures of paraffin before and after Be(in the both manifolds)

Page 8: Temperature rise of SVD2 IR beampipe during single beam study

T(I) =Tconst +dT(I)

T(ILER)= 0.2+0.3 I2T(IHER)= 0.2+0.6 I2

dT(ILER= 1A)=0.3 deg dT(ILER=1.8A)=1.0 deg dT(ILER=2.5A)=1.9 deg

dT(IHER=0.6A)=0.2 deg dT(IHER=1.2A)=0.9 deg dT(IHER=1.5A)=1.4 deg

Quadratic fit of the temperature difference betweenin- and out-flowing paraffin

Page 9: Temperature rise of SVD2 IR beampipe during single beam study

Heat deposit in Be:

dTLER=0.3 deg dTHER=0.2 deg

dm/dt=0.88kg/min (1.1l/min) Cp=2300kJ/kg/K

P=dm/dt * Cp * dT Pmeas(LER) = 10W P[W]=34 * dT [K] Pmeas(HER) = 7W

If we extrapolate dT(I):

Pext(ILER=2.5A) = 65W Pext(IHER=1.5A) = 50W

The fit of present data is close to design value for Be (100W)

Single beam study with larger currents would help…

Page 10: Temperature rise of SVD2 IR beampipe during single beam study

Be pipe LER side(paraffin inlet)

Tmp(11): beampipez=101mm from IP

LER 1A/HER 0.6AdT=0.28 degLER 1.8A/HER 1.2AdT=0.72 deg LER 2.5A HER 1.5AdT=1.19 deg

Page 11: Temperature rise of SVD2 IR beampipe during single beam study

Be pipe HER side(paraffin outlet)

Tmp(28): beampipez=-54mm from IP

LER 1A/HER 0.6AdT=0.5 degLER 1.8A/HER 1.2AdT=1.8 deg LER 2.5 HER 1.5AdT=3.17deg

Page 12: Temperature rise of SVD2 IR beampipe during single beam study

Hot spot LER side

Tmp(7): beampipez=160mm from IP(after Cu cooling block)

LER 1A/HER 0.6AdT=3.6 degLER 1.8A/HER 1.2AdT=12.5 deg LER 2.5 HER 1.5AdT=22.1 deg

Page 13: Temperature rise of SVD2 IR beampipe during single beam study

Hot spot HER side

Tmp(24): beampipez=-105mm from IP(after Cu cooling block)

LER 1A/HER 0.6AdT=1.8 degLER 1.8A/HER 1.2AdT=10 deg LER 2.5 HER 1.5AdT=18.5deg