The signal expected from a MAD experiment can be calculated using an approximation similar to that derived by Crick and Magdoff [1956] for an MIR experiment. The equations used are:
perturbation due to =
(NA/2NT)1/2(2 A/Zeff)
perturbation due to =
(NA/2NT)1/2(| A i - A j|)/Zeff
|
where
= 0)
Since the perturbations due to
and
are orthogonal, we may take
the net expected signal to be the root-mean-square of these two quantities.
A remarkable property of anomalous scattering is that it does not fall off
with sin(
)/
. This means that the
contribution of anomalous scattering to the total measured intensity
actually increases at higher resolution. On the other hand, your
data quality normally falls off at higher resolution, so you may or may
not be able to take advantage of this behaviour.
To show how this works, here is an interactive form to calculate the approximate signal expected from a MAD experiment. For a more detailed discussion of the signal available from a MAD experiment, see Hendrickson & Ogata (1997) or Bella & Rossmann (1997)
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