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False asymmetries/Ground Loops David Bowman 4/27/12.

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Presentation on theme: "False asymmetries/Ground Loops David Bowman 4/27/12."— Presentation transcript:

1 False asymmetries/Ground Loops David Bowman 4/27/12

2 Why do we need a filter? The signal consists of a large number of pulses with widths of ~ 2 micro second We sample at ~ 20 micro sec intervals (50 KHz rate) It is necessary to form a time average of the signal to avoid loss of information because if the pulse width is less than the sampling interval, some pulsed don’t contribute

3 Time response of different filters Time The desirable feature of the Bessel filter is that the time response does not have oscillations.

4 Signal flow Detector, preamp TRIUMF adjustable gain module Sum and difference and filter Amplifier – Ring sums and detector differences VME 3 – ADC of Ring Sums, spin state and monitors VME2 – ADC of detector differences Different components are located in different crates and racks. – Communication by ground loops – Communication within Sum, Difference, and Filter box via ground loops and stray capicatance

5 Ground loops If the loop is defined by conductors, E appears across the largest resistance

6 Reconfigure analog signal processing chain Eliminate TRIUMF gain box, Sum and difference box, Ring sums Build new Bessel filter box with (gain of 3 -> gain of 6) connected to detector signals by twinex (shielded twisted pair) and connected to ADC’s in VME2 by twinex.

7 Least bit ADC noise –staircase problem  is bin width,  is RMS noise on analog signal. If  is ~.5 , average ADC signal ~ input signal It is possible to achieve 6 V detector signal, and  ~.5 


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