Summary: Longer spectrum runs were performed on each
of the available low energy sources. The
channel vs. energy graph was re-plotted based on the new data. The behavior is still linear. The only issue at the moment, is that the
signal levels are close to the noise count levels, causing the peaks from each
of the sources to be fairly broad. This
should be OK. since we're just looking
for evidence of a signal at all, resolution won't be critical in this
application. The iron magnet cooling supply
was completely installed and can supply two gallons per minute to the magnet,
meeting the specification. A Cs 137
Dewar attenuation spectrum was started. The
data will be collected on the morning of the 21st.
Bias
|
1500 V
|
Gate Window
|
0.5 uS
|
Threshold
|
1.5mV
|
Attenuation
|
0 dB
|
Data set
|
HBC_00015
|
Source
|
Cs 137 Taped to window
|
Start Time
|
8:53 AM
|
Stop Time
|
11:58 AM
|
Date
|
2014_08_20
|
x-y scope V/div
|
1, 0.5
|
Shielded?
|
Yes
|
Tube
|
Harshaw B-
|
Bias
|
1500 V
|
Gate Window
|
0.5 uS
|
Threshold
|
1.5mV
|
Attenuation
|
0 dB
|
Data set
|
HBC_00016
|
Source
|
Cd 109 Taped to window
|
Start Time
|
12:15 PM
|
Stop Time
|
1:38 PM
|
Date
|
2014_08_20
|
x-y scope V/div
|
1, 0.5
|
Shielded?
|
Yes
|
Tube
|
Harshaw B-
|
Bias
|
1500 V
|
Gate Window
|
0.5 uS
|
Threshold
|
1.5mV
|
Attenuation
|
0 dB
|
Data set
|
HBC_00017
|
Source
|
Am 241 Taped to window
|
Start Time
|
2:01 PM
|
Stop Time
|
6:41 PM
|
Date
|
2014_08_20
|
x-y scope V/div
|
1, 0.5
|
Shielded?
|
Yes
|
Tube
|
Harshaw B-
|
Channel Linearity
Source
|
Peak Channel
|
Energy eV
|
Cd109
|
59
|
22100
|
am241
|
95
|
26344
|
Cs 137
|
108
|
32000
|
Am241
|
271
|
59541
|
Cd109
|
421
|
88000
|
1023
|
197523.88
|
Magnet Cooling
To cool the magnet properly, a water flow of two gallons per minute is required. That corresponds to 3.785 liters every 30
seconds. 3.75+ liters was measured into
a bucket, and a piece of tape was placed with its lower edge at the water
level. Flow speed trials were run by
watching the water level compared to the tape in 30 second intervals. The required flow rate was achieved after
several incremental water flow increases at the sink. The flow can be measured at the sink, but as
a ball park indictor, the “CW” indicator should be readable from left to right
and perched at about 30 degrees to the horizontal.
There were initially leaks at the right most input manifold
and at the garden hose output manifold. There
is still a leak at the sink fitting. A
weight has been placed on top of the hose to hold it in the sink so the leak
flows down the drain rather than down the cabinet.
Signal Attenuation
Due to Dewar
The material that makes up the liquid helium Dewar will attenuate
the signal form the experiment. The level
of attenuation is being measured by collecting count data on each of the
sources inside and outside the Dewar.
The setup for the Dewar attenuation runs is shown below. The source was lowered into the sample
chamber of the Dewar on the end of a wooden yard stick It was taped in place with a thin layer of
paper, (to protect the source from the tape), and two layers of electrical
tape. The yard stick was roughly centered
in the chamber with two rolls of masking tape as shown below.
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