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تحميل كتاب Frederix P L T M Hoogenboom B W Fotiadis D Atomic Force Microscopy of Biological Samples pdf
المؤلف : D Fotiadis D J Müller and A Engel
عن الكتاب : 2004م - 1443هـ
نبذه عن الكتاب:
lied to the stylus was approximately 50 pN,
preventing a force-induced conformational change of the E–F loop. This loop is
known to deform when the force is increased to 100 pN, thereby changing the
conformation of the bR surface.15 Interestingly, observations of different atomic
models from x-ray crystallography show
that the variation of this region is pronounced: the E–F loop is involved in the
contacts leading to the 3D crystals, and its
conformation is dictated by the 3D packing arrangement of the bR molecules. Although all the bR trimers are identical in
the 2D crystal displayed in Figure 3a, their
surface structure varies significantly.
These changes are related to the flexibility
of the bR surface rather than any noise introduced by the AFM. The flexibility of the
surface lowers the resolution of the ensemble, but structural details of each trimer
are still discernable. The variations in the
trimer structure can be used to calculate
the probability of finding a certain loop at
a certain position (x,y) by mapping the
corresponding peak positions of all individual bR trimers.16 The E–F loop, which
exhibits significant flexibility, is more delocalized than the A–B loop, which occupies a more defined position. The signal about
the threefold axis results from a lipid
molecule protruding 0.1 nm, which is only
occasionally visible in the raw data, but
if present, is precisely localized in the center
of the trimer. Therefore, a strong signal
emerges in the probability map (Figure 3c),
whereas no signal is present in the average
(Figure 3b). Precise localization of a surface
feature suggests that the correspondin .
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وصف كتاب Frederix P L T M Hoogenboom B W Fotiadis D Atomic Force Microscopy of Biological Samples
2004م - 1443هـ
نبذه عن الكتاب:
lied to the stylus was approximately 50 pN,
preventing a force-induced conformational change of the E–F loop. This loop is
known to deform when the force is increased to 100 pN, thereby changing the
conformation of the bR surface.15 Interestingly, observations of different atomic
models from x-ray crystallography show
that the variation of this region is pronounced: the E–F loop is involved in the
contacts leading to the 3D crystals, and its
conformation is dictated by the 3D packing arrangement of the bR molecules. Although all the bR trimers are identical in
the 2D crystal displayed in Figure 3a, their
surface structure varies significantly.
These changes are related to the flexibility
of the bR surface rather than any noise introduced by the AFM. The flexibility of the
surface lowers the resolution of the ensemble, but structural details of each trimer
are still discernable. The variations in the
trimer structure can be used to calculate
the probability of finding a certain loop at
a certain position (x,y) by mapping the
corresponding peak positions of all individual bR trimers.16 The E–F loop, which
exhibits significant flexibility, is more delocalized than the A–B loop, which occupies a more defined position. The signal about
the threefold axis results from a lipid
molecule protruding 0.1 nm, which is only
occasionally visible in the raw data, but
if present, is precisely localized in the center
of the trimer. Therefore, a strong signal
emerges in the probability map (Figure 3c),
whereas no signal is present in the average
(Figure 3b). Precise localization of a surface
feature suggests that the correspondin .
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