D isplacement of BRT

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Displacement of BRT Junko Katayama

description

D isplacement of BRT. Junko Katayama. Transmission Monitor System. TMS. ETM. BRT. GPT. QPD. What I did. Lateral and angular motion of BRT cause the noise on QPDs. I computed those BRT motion noise and shot noise for both SOFT and HARD mode in two cases ; TMS table fixed on the ground - PowerPoint PPT Presentation

Transcript of D isplacement of BRT

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Displacement of BRT

Junko Katayama

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BRTGPT

ETM

QPD

TMS

Transmission Monitor System

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What I did

Lateral and angular motion of BRT cause the noise on QPDs.I computed those BRT motion noise and shot noise for both SOFT and HARD mode in two cases ;• TMS table fixed on the ground• TMS suspended by pendulum

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Angular motionThere are two types of angular motion.1. Surface wave on the ground (v=5000m/s)

Θ = 2πf * xseis / v

2. Table motion (simulation data from ATC)

x3

x1

x2

y1

y3y2

Z-rotation X,Y-rotations1 = x1s2 = -1/2*x2 + √3/2*y2s3 = -1/2*x3 - √3/2*y3

Rθz =(s1+s2+s3)/3Rθxy = (((z2+z3)/2)*2-z1)

z1

z3z2

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Angular motioncomparing surface wave & table move

↑ dominant

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Table motion is quite smaller than surface wave→ consider only surface wave as the angular motion of BRT

From the next slide,I computed the noise contribution to h for each SOFT and HARD mode.There are two lines with each noise ;Ex) shot1 : shot noise on QPD1 shot2 : shot noise on QPD2

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SOFT modefixed on the ground

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HARD modefixed on the ground

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Transfer Function

X = 1/(1-(ω/ω0)2+iω/Qω0)*xseis

Θ = dk(1% *xseis)/(-Iw2+2d2k)

z2-z1=1% *xseis

I=M(2d)2/12

d=1m , M=200kg

Mg

d

z2z1

↑Suspended by

2 wires

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SOFT modesuspended

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HARD modesuspended

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Conclusion

• rotation of TMS table is not dominant→ surface wave is dominant

• we can get HARD signal with TMS suspended…cannot get SOFT because of the shot noise