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Soft Condensed Matter - Small Angle Scattering
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I22 Contact

Beamline phone numbers:
+44 (0) 1235 77 8617
+44 (0) 1235 77 8713 

Principal Beamline Scientist: 
Nick Terrill

Tel: +44 (0) 1235 778047
E-mail: [email protected]

More

Science Group Leader

Robert Rambo

Email: [email protected]
Tel: +44 (0)1235 56 7675

  1. Instruments
  2. Soft Condensed Matter
  3. Small Angle Scattering
  4. I22
  5. Planning Your Experiment
  6. Energy and Camera Length

Energy and Camera Length

In order to determine the optimum set up for each experiment, a couple of important pieces of information are needed. If you do not understand or know the answers to any of these questions, please contact a member of the beamline team who will be happy to advise you.

  • What is the q range of interest for your experiment?
  • Which energy will you need to use for your experiment?
  • Does your sample has a preferred orientation or alignment? Do you want to maximise the q-range by setting the beamstop at the top, or investigate orientation effects using a central beamstop?
  • Do you need to measure WAXS?

Using this information, the table below can help you to work out the set up requirements for each experiment. Please note that there is a time cost associated with all set up changes during an experiment and so we do not recommend more than one camera length, energy or sample environment change during an experiment. Please discuss all set up requirements in advance with your local contact.

Energy and wavelength

The beamline team will often refer to the energy of the beamline, which relates to the wavelength of the light used. I22 is monochromatic, so a single wavelength is used. Energy and wavelength are related by this simple equation:

Most laboratory sources and other scattering tools will refer to the wavelength rather than the energy, so it's good to know how to switch between the two. Some popular choices of energy are:

12.4 keV 1 Å
8 keV 1.54 Å (Cu K alpha)
17.5 keV 0.71 Å (Mo K alpha)

Camera length and energy table

SAXS using Pilatus P3-2M (2D detector). There is a beta perspective in DAWN, currently called DEDI (soon to be renamed BeaCon) that will allow you to configure camera length according to energy and q-scale

 

Isotropic SAXS (Beamstop at top)

 

1.9

5 4.90E-03 0.350 17.9 1300
  7 6.80E-03 0.490 12.8 930
  10 9.67E-03 0.700 8.96 650
  12.4 1.20E-02 0.870 7.23 525
  14 1.40E-02 0.980 6.40 465
  17 1.60E-02 1.19 5.27 380
  20 1.90E-02 1.40 4.48 325
3.9 5 2.39E-03 0.174 36.1 2630
  7 3.34E-03 0.244 25.8 1880
  10 4.78E-03 0.348 18.1 1320
  12.4 5.92E-03 0.432 14.6 1060
  14 6.69E-03 0.487 12.9 940
  17 8.12E-03 0.592 10.6 775
  20 9.55E-03 0.696 9.03 660
5.9 5 1.59E-03 0.116 54.3 3960
  7 2.22E-03 0.162 38.8 2830
  10 3.17E-03 0.231 27.2 1980
  12.4 3.93E-03 0.287 21.9 1600
  14 4.44E-03 0.324 19.4 1420
  17 5.39E-03 0.393 15.9 1170
  20 6.34E-03 0.463 13.6 990
7.9 5 1.19E-03 0.087 72.6 5300
  7 1.66E-03 0.121 51.8 3780
  10 2.37E-03 0.173 36.3 2650
  12.4 2.94E-03 0.215 29.2 2140
  14 3.32E-03 0.242 25.9 1890
  17 4.03E-03 0.294 21.3 1560
  20 4.75E-03 0.346 18.1 1320
9.7 5 9.72E-04 0.071 88.5 6460
  7 1.36E-03 0.099 63.2 4620
  10 1.95E-03 0.142 44.3 3230
  12.4 2.41E-03 0.176 35.7 2600
  14 2.72E-03 0.199 31.6 2300
  17 3.31E-03 0.241 26.0 1900
  20 3.89E-03 0.284 22.1 1620

 

Anisotropic SAXS (Beamstop at centre)

 

1.9 5 4.90E-03 0.187 33.6 1300
  7 6.80E-03 0.262 24 930
  10 9.67E-03 0.375 16.8 650
  12.4 1.20E-02 0.464 13.5 525
  14 1.40E-02 0.524 12.00 465
  17 1.60E-02 0.637 9.87 380
  20 1.90E-02 0.75 8.39 325
3.9 5 2.39E-03 0.093 67.9 2630
  7 3.34E-03 0.13 48.5 1880
  10 4.78E-03 0.185 33.9 1320
  12.4 5.92E-03 0.23 27.4 1060
  14 6.69E-03 0.259 24.2 940
  17 8.12E-03 0.315 20.0 775
  20 9.55E-03 0.37 17 660
5.9 5 1.59E-03 0.061 102.0 3960
  7 2.22E-03 0.086 73 2830
  10 3.17E-03 0.123 51.1 1980
  12.4 3.93E-03 0.152 41.2 1600
  14 4.44E-03 0.172 36.5 1420
  17 5.39E-03 0.209 30.1 1170
  20 6.34E-03 0.246 25.5 990
7.9 5 1.19E-03 0.046 136.5 5300
  7 1.66E-03 0.064 97.5 3780
  10 2.37E-03 0.092 68.2 2650
  12.4 2.94E-03 0.114 55.1 2140
  14 3.32E-03 0.129 48.8 1890
  17 4.03E-03 0.156 40.2 1560
  20 4.75E-03 0.184 34.1 1320
9.7 5 9.72E-04 0.038 167.0 6460
  7 1.36E-03 0.053 119 4620
  10 1.95E-03 0.075 83.3 3230
  12.4 2.41E-03 0.094 67.2 2600
  14 2.72E-03 0.106 59.5 2300
  17 3.31E-03 0.128 49.0 1900
  20 3.89E-03 0.151 41.6 1620

 

WAXS using Pilatus3-2M-DLS-L

 

The exact q-ranges available from the WAXS detector are variable due to the large number of possible sample/WAXS Detector/SAXS detector configurations but, as a guide, numbers below are given for sample - WAXS detector distance = 175.4mm and with the pirmary beam passing 2mm from the edge of the WAXS detector chips.

5

0.029 1.91 1.98
7 0.040 2.67 2.77
10 0.058 3.82 3.95
12.4 0.072 4.73 4.90
14 0.081 5.34 5.54
17 0.098 6.49 6.72
20 0.116 7.63 7.91

 

NOTE: For a given detector geometry and energy, if qmin(WAXS) < qmax(SAXS) you will have overlap between data sets.

 

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