[ec392464] | 1 | .. invariant_help.rst |
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| 2 | |
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| 3 | .. This is a port of the original SasView html help file to ReSTructured text |
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| 4 | .. by S King, ISIS, during SasView CodeCamp-III in Feb 2015. |
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| 5 | |
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| 6 | Invariant Calculation Perspective |
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| 7 | ================================= |
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| 8 | |
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[a9dc4eb] | 9 | Description |
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| 10 | ----------- |
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[ec392464] | 11 | |
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[0721c3d] | 12 | The scattering, or Porod, invariant (Q*\) is a model-independent quantity that |
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| 13 | can be easily calculated from scattering data. |
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[ec392464] | 14 | |
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[0721c3d] | 15 | For two phase systems, the scattering invariant is defined as the integral of |
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| 16 | the square of the wave transfer (Q) multiplied by the scattering cross section |
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| 17 | over the full range of Q from zero to infinity, that is |
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[ec392464] | 18 | |
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| 19 | .. image:: image001.gif |
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| 20 | |
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[0721c3d] | 21 | where *g = Q* for pinhole geometry (SAS) and *g = Qv* (the slit height) for |
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| 22 | slit geometry (USAS). |
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[ec392464] | 23 | |
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[0721c3d] | 24 | The worth of Q*\ is that it can be used to determine the volume fraction and |
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| 25 | the specific area of a sample. Whilst these quantities are useful in their own |
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| 26 | right they can also be used in further analysis. |
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[ec392464] | 27 | |
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[0721c3d] | 28 | The difficulty with using Q*\ arises from the fact that experimental data is |
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| 29 | never measured over the range 0 =< *Q* =< infinity. At best, combining USAS and |
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| 30 | WAS data might cover the range 1e-5 =< *Q* =< 10 1/\ |Ang| . Thus it is usually |
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| 31 | necessary to extrapolate the experimental data to low and high *Q*. For this |
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[ec392464] | 32 | |
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[0721c3d] | 33 | High-*Q* region (>= *Qmax* in data) |
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[ec392464] | 34 | |
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[0721c3d] | 35 | * The power law function *C*/*Q*\ :sup:`4` is used where the constant |
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| 36 | *C* (= 2.\ |pi|\ .(\ |bigdelta|\ |rho|\ ).\ *Sv*\ ) is to be found by fitting part of data |
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| 37 | within the range *Q*\ :sub:`N-m` to *Q*\ :sub:`N` (where m < N). |
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[ec392464] | 38 | |
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[0721c3d] | 39 | Low-*Q* region (<= *Qmin* in data) |
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[ec392464] | 40 | |
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[0721c3d] | 41 | * The Guinier function *I0.exp(-Rg*\ :sup:`2`\ *Q*\ :sup:`2`\ */3)* where *I0* |
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| 42 | and *Rg* are obtained by fitting as for the high-*Q* region above. |
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| 43 | Alternatively a power law can be used. |
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[ec392464] | 44 | |
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[0721c3d] | 45 | .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ |
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[ec392464] | 46 | |
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[a9dc4eb] | 47 | Using the perspective |
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| 48 | --------------------- |
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[0721c3d] | 49 | |
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| 50 | 1) Select *Invariant* from the *Analysis* menu on the SasView toolbar. |
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| 51 | |
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| 52 | 2) Load some data with the *Data Explorer*. |
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| 53 | |
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| 54 | 3) Select a dataset and use the *Send To* button on the *Data Explorer* to load |
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| 55 | the dataset into the *Invariant* perspective. |
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| 56 | |
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| 57 | 4) Use the *Customised Input* boxes on the *Invariant* perspective to subtract |
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| 58 | any background, specify the contrast (i.e. difference in SLDs - this must be |
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| 59 | specified for the eventual value of Q*\ to be on an absolute scale), or to |
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| 60 | rescale the data. |
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[ec392464] | 61 | |
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[0721c3d] | 62 | 5) Adjust the extrapolation range as necessary. In most cases the default |
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| 63 | values will suffice. |
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[ec392464] | 64 | |
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[0721c3d] | 65 | 6) Click the *Compute* button. |
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[ec392464] | 66 | |
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[0721c3d] | 67 | 7) To include a lower and/or higher Q range, check the relevant *Enable |
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| 68 | Extrapolate* check boxes. |
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| 69 | |
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| 70 | If power law extrapolations are chosen, the exponent can be either held |
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| 71 | fixed or fitted. The number of points, Npts, to be used for the basis of the |
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| 72 | extrapolation can also be specified. |
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[ec392464] | 73 | |
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[0721c3d] | 74 | 8) If the value of Q*\ calculated with the extrapolated regions is invalid, a |
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| 75 | red warning will appear at the top of the *Invariant* perspective panel. |
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[ec392464] | 76 | |
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[0721c3d] | 77 | The details of the calculation are available by clicking the *Details* |
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| 78 | button in the middle of the panel. |
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[ec392464] | 79 | |
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[0721c3d] | 80 | .. image:: image005.gif |
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[ec392464] | 81 | |
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| 82 | .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ |
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| 83 | |
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[a9dc4eb] | 84 | Parameters |
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| 85 | ---------- |
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[ec392464] | 86 | |
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| 87 | Volume Fraction |
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[a9dc4eb] | 88 | ^^^^^^^^^^^^^^^ |
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[ec392464] | 89 | |
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[0721c3d] | 90 | The volume fraction |phi| is related to Q*\ by |
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| 91 | |
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[ec392464] | 92 | .. image:: image002.gif |
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| 93 | |
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[0721c3d] | 94 | where |bigdelta|\ |rho| is the SLD contrast. |
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[ec392464] | 95 | |
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| 96 | .. image:: image003.gif |
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| 97 | |
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| 98 | .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ |
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| 99 | |
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| 100 | Specific Surface Area |
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[a9dc4eb] | 101 | ^^^^^^^^^^^^^^^^^^^^^ |
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[ec392464] | 102 | |
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[0721c3d] | 103 | The specific surface area *Sv* is related to Q*\ by |
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[ec392464] | 104 | |
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[0721c3d] | 105 | .. image:: image004.gif |
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[ec392464] | 106 | |
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[0721c3d] | 107 | where *Cp* is the Porod constant. |
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[ec392464] | 108 | |
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| 109 | .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ |
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| 110 | |
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[a9dc4eb] | 111 | Reference |
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| 112 | --------- |
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[ec392464] | 113 | |
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[0721c3d] | 114 | O. Glatter and O. Kratky |
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| 115 | Chapter 2 in *Small Angle X-Ray Scattering* |
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| 116 | Academic Press, New York, 1982 |
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[ec392464] | 117 | |
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| 118 | http://physchem.kfunigraz.ac.at/sm/ |
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| 119 | |
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[0721c3d] | 120 | .. ZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZZ |
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[ec392464] | 121 | |
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[a9dc4eb] | 122 | .. note:: This help document was last changed by Steve King, 01May2015 |
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