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Gravitational Waves: a new window to observe the Universe

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The Classical Detection Method:<br />

Weber Bars<br />

1<br />

With l = x − xh+<br />

2<br />

cos2Ω(<br />

t − z)<br />

each particle in <strong>the</strong> bar is<br />

accelerated<br />

2<br />

d l 1 2<br />

= xΩ<br />

h cos 2Ω(<br />

t − z)<br />

2<br />

+<br />

dt 2<br />

y<br />

z<br />

x<br />

L<br />

dm = ρdx<br />

transducer<br />

Detection of <strong>the</strong> motion:<br />

How big a signal will <strong>the</strong><br />

transducer see?<br />

=<br />

h<br />

+<br />

h LQ<br />

16<br />

⇒ h = 10 −20<br />

L = 1m<br />

Q = 1.6×10 4<br />

h + = 10 −23<br />

Current bars can detect<br />

10 −16 m

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