HRRL radiation tests

Building a new positron beamline in the HRRL cell might require moving the linac itself. To help assess whether this is feasible with current shielding, radiation levels were measured on Feb 4, 2009 by M. Balzer and G. Stancari.

The HRRL was set at 15 MeV beam energy, 20 mA peak current, 1 kHz repetition rate, and 30 ns pulse width. Five OSL dosimeters were placed at each of 15 locations in the cell. Locations are marked on the following map:

Media:dosimeter-locations-20090204.pdf

Readings in mrad are reported in the following table. They were taken before exposure (first column) and after a couple of minutes of machine tuning (second column). Readings in the third column were taken 94 minutes after the second reading. During these 94 minutes, the machine was running with the settings mentioned above.

Media:exposure-measurements-20090204.pdf

Dose rates in mrad/hr at each of the 15 locations can be estimated by subtracting column 2 from column 3, averaging over the 5 dosimeters, and multiplying the result by (60 min/hr) / (94 min). RMS spreads refer to variations within each group of 5.

Location	Dose rate	RMS spread
	(mrad/hr)	(mrad/hr)
1	9	4
2	396	57
3	7940	204
4	2831	117
5	4408	373
6	29339	3332
7	72517	687
8	36507	4746
9	5	5
10	37	4
11	164	40
12	2734	313
13	5828	120
14	7793	2579
15	62431	27155

Experimental Cell Dose Measurement with HRRL

This experiment is done on 5/17/2010, at 10:00 am.

Dr. Khalid Chouffani wrote the note. Here is photocopy of his note:

page #1

page #2

16 MeV Beam Energy

Experimental cell measurement with HRRL.

Conditions are:

Rap rate: 40 Hz

Pulse width: 1 [math]\mu sec[/math]

[math]\Delta[/math]E=(10-17) MeV

Peak current of beam (mA)	Energy of beam (MeV)	Measurement on Channel 17, Experimental Cell (mrad)	Measurement on Channel 16, Accelerator cell (mrad)
100	16	4.5 [math]\pm [/math] 0.2	45.5 [math]\pm [/math] 2
69.2	16	4 [math]\pm [/math] 0.2	35, 42.5
60.8	16	3.5 [math]\pm [/math] 0.1	29.2, 28.9
58.0	16	2.8, 2.9	26, 26.7
47.6	16	2.3	19.6, 21.3
33.2	16	1.8, 1.7	19.5, 19.0, 13.7

Beam bear through 1/4 inches diameter collimator with 4 inches lead.

16 MeV Beam Energy

Conditions are:

Rap rate: 40 Hz

Peak current of beam (mA)	Energy of beam (MeV)	Measurement on Channel 17, Experimental Cell (mrad)	Measurement on Channel 16, Accelerator cell (mrad)
136	16	0.3	99.2, 98.7

10 MeV Beam Energy

Conditions are:

Rap rate: 110 Hz

[math]\Delta[/math]E=(8-16) MeV

Peak current of beam (mA)	Energy of beam (MeV)	Measurement on Channel 17, Experimental Cell (mrad)	Measurement on Channel 16, Accelerator cell (mrad)
48.4	10	4.6, 4.7	117.6, 117.5
36.8	10	3.8, 3.9	104.4, 103.5, 102.9
30.8	10	3.1 [math]\pm [/math] 0.1	72.8, 72.9, 72.5
26	10	2.5	56.7, 56.4, 54.6

Channel 17 Dose Estimation in New Position

Channel 17 is a dose measuring detector on in the HRRL experimental cell.

Calculating number of particles per second

We have electron beam of:

Frequency: f (HZ)

Peak current: I (mAmp = 0.001 Amp)

Pulse width: [math] \Delta[/math] t ( [math] 1 ns=1*10^{-9} [/math] seconds )

So, how many electrons we have in each second?

By Q=It, we have

                                         [math]    N*e=f*I*\Delta t [/math] 

Where N is the total electron numbers hits target per second, e is electron charge and f, I and [math] \Delta t [/math] are given above. So

                          <math>  N = f*I*\Delta t/e= f*I*\Delta t/(1.6*10^{-19}) <math> 

So, we have around 3.12075*1012 electrons hit radiator per second.

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