2a7e

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(New page: 200px<br /><applet load="2a7e" size="350" color="white" frame="true" align="right" spinBox="true" caption="2a7e, resolution 1.66&Aring;" /> '''On the Routine Use o...)
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==Overview==
==Overview==
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Complete and highly redundant data sets were collected at different, wavelengths between 0.80 and 2.65 A for a total of ten different protein, and DNA model systems. The magnitude of the anomalous signal-to-noise, ratio as assessed by the quotient R(anom)/R(r.i.m.) was found to be, influenced by the data-collection wavelength and the nature of the, anomalously scattering substructure. By utilizing simple empirical, correlations, for instance between the estimated deltaF/F and the expected, R(anom) or the data-collection wavelength and the expected R(r.i.m.), the, wavelength at which the highest anomalous signal-to-noise ratio can be, expected could be estimated even before the experiment. Almost independent, of the nature of the anomalously scattering substructure and provided that, no elemental X-ray absorption edge is nearby, this optimal wavelength is, 2.1 A.
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Complete and highly redundant data sets were collected at different wavelengths between 0.80 and 2.65 A for a total of ten different protein and DNA model systems. The magnitude of the anomalous signal-to-noise ratio as assessed by the quotient R(anom)/R(r.i.m.) was found to be influenced by the data-collection wavelength and the nature of the anomalously scattering substructure. By utilizing simple empirical correlations, for instance between the estimated deltaF/F and the expected R(anom) or the data-collection wavelength and the expected R(r.i.m.), the wavelength at which the highest anomalous signal-to-noise ratio can be expected could be estimated even before the experiment. Almost independent of the nature of the anomalously scattering substructure and provided that no elemental X-ray absorption edge is nearby, this optimal wavelength is 2.1 A.
==About this Structure==
==About this Structure==
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[[Category: Mueller-Dieckmann, C.]]
[[Category: Mueller-Dieckmann, C.]]
[[Category: Panjikar, S.]]
[[Category: Panjikar, S.]]
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[[Category: Tucker, P.A.]]
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[[Category: Tucker, P A.]]
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[[Category: Weiss, M.S.]]
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[[Category: Weiss, M S.]]
[[Category: a-dna]]
[[Category: a-dna]]
[[Category: double helix]]
[[Category: double helix]]
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''Page seeded by [http://oca.weizmann.ac.il/oca OCA ] on Tue Jan 29 17:56:04 2008''
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''Page seeded by [http://oca.weizmann.ac.il/oca OCA ] on Thu Feb 21 16:24:20 2008''

Revision as of 14:24, 21 February 2008


2a7e, resolution 1.66Å

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On the Routine Use of Soft X-Rays in Macromolecular Crystallography, Part III- The Optimal Data Collection Wavelength

Overview

Complete and highly redundant data sets were collected at different wavelengths between 0.80 and 2.65 A for a total of ten different protein and DNA model systems. The magnitude of the anomalous signal-to-noise ratio as assessed by the quotient R(anom)/R(r.i.m.) was found to be influenced by the data-collection wavelength and the nature of the anomalously scattering substructure. By utilizing simple empirical correlations, for instance between the estimated deltaF/F and the expected R(anom) or the data-collection wavelength and the expected R(r.i.m.), the wavelength at which the highest anomalous signal-to-noise ratio can be expected could be estimated even before the experiment. Almost independent of the nature of the anomalously scattering substructure and provided that no elemental X-ray absorption edge is nearby, this optimal wavelength is 2.1 A.

About this Structure

2A7E is a Protein complex structure of sequences from [1]. Full crystallographic information is available from OCA.

Reference

On the routine use of soft X-rays in macromolecular crystallography. Part III. The optimal data-collection wavelength., Mueller-Dieckmann C, Panjikar S, Tucker PA, Weiss MS, Acta Crystallogr D Biol Crystallogr. 2005 Sep;61(Pt 9):1263-72. Epub 2005, Aug 16. PMID:16131760

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