Angewandte
Communications
Chemie
[
28]
a modified Alexa fluorophore (50%) as well as with the
reaction of an inversely functionalized nitroxide radical
(
Information), as the double integral of the iron signal for
equally concentrated samples is 171 a.u. and 263 a.u. for
C58T1 and C58R1, respectively, yielding a ratio of 0.65, which
matches the ratio of the modulation depths. These differences
in iron contents in CYP101 preparations are a known
[
31]
64%). The reason for the lower labeling yield as compared
to MTSSL is that the in vivo protein expression leads to
partial reduction of the non-canonical azide group of the
[
32]
[31,35,36]
amino acid. The labeling efficiency for 3 is with 36% lower
phenomenon.
than what was reported for a similar reaction in the literature
The distance distribution for C58T1 (Figure 3b) reveals
two maxima at 2.0 nm and 3.5 nm with a standard deviation of
0.2 nm and 0.15 nm, respectively. To translate this spin–spin
distances into biologically relevant CAlpha distances, it is
necessary to match them with in silico predictions, for
[
33]
(
70%),
which is attributed to the comparatively mild
labeling conditions that were applied here.
Since CYP101 contains iron(III) as an intrinsic para-
magnetic cofactor, labeling the protein with one trityl only is
sufficient for enabling distance measurements between the
trityl label and the iron center. Such measurements are
desirable since metal cofactors play a critical role in many
biological processes and their localization within a biological
[37]
example, using mtsslWizard. At this point, however, the
mtsslWizard prediction differs from the experimental result in
terms of mean distance and width of distribution, although it
encompasses the experimental distribution and also predicts
the experimentally obtained bimodality, which is probably
due to label–protein interactions. In order to exclude that the
bimodality is an artifact of the background correction, the two
peaks were demonstrated to prevail for various backgrounds
(see the Supporting Information). Compared to C58R1,
which revealed a nitroxide–Fe distance of 3.06 nm with
a standard deviation of 0.11 nm (Figure 3d), the T1 side-
chain shifts the distribution to 0.4 nm longer distances
because of the three bonds longer linker and causes a broad-
ening of the distribution.
[34]
structure
is often crucial for the understanding of for
example, a function of protein. Previous studies indicated,
that for distance measurements involving the CYP101 low-
[
35]
spin iron(III), RIDME is better suited than PELDOR.
Therefore, trityl labels 1 and 3 were tested for such RIDME
measurements. Labels 1 and 3 were chosen because 1 is the
analog of the nitroxide standard MTSSL and 3 enables in-cell
measurements.
In Figure 3a, the in vitro Q-band RIDME time trace of
CYP101 labeled with 1 (C58T1) and the corresponding
distance distribution are shown. The time trace is well-
Also, in the case of CYP101 mutant C58 labeled with 3
(C58T3), a modulated time trace could be obtained with
À1/2
modulated and has a high SNR of 20.84 S/Nmin . For the
À1/2
sake of comparison, also the RIDME data for the MTSSL-
labeled analog is shown (C58R1). Here, the SNR was
a SNR calculated as 10.85 S/Nmin . The decrease in SNR
relative to CYP101 mutant C58T1 is due to the lower labeling
efficiency of 3. The modulation depth of this sample is only
7% and thus a factor of 3 lower than found for C58T1, but
matches again with an iron content reduced by the same
factor (see the Supporting Information). However, even with
this rather low labeling efficiency and low iron content a good
quality RIDME time trace could be obtained. The distance
À1/2
calculated as 13.08 S/Nmin . Thus, the trityl sample pro-
vides a 60% better SNR than the MTSSL sample, which
matches expectations, as only about 40% of the nitroxide
spectrum but all of the trityl spectrum is excited. The
observed modulation depth for C58T1 is 15% lower than
the 35% obtained for C58R1. However, this can be attributed
to a lower iron content in CYP101 C58T1 (see the Supporting
III
distribution for C58T3 reveals a trityl–Fe distance with
maxima at 2.4 nm and 3.5 nm and standard deviations of
0
.25 nm and 0.12 nm, respectively. Within error, the mtsslWi-
zard prediction matches the experimental inasmuch as it
predicts a bimodal distribution, but again differs in terms of
mean distance and width of distribution. The distance
distributions obtained for labels 1 and 3 are of a smaller
width than those found in the literature for other trityl labels
where standard deviations of 0.19 nm and 0.37 nm were
[
15,17]
reported.
This is partially due to a smaller label volume
and a smaller number of rotatable bonds (see the Supporting
Information), but it should be considered that the width of the
distribution is also dependent on the labeling site and
therefore not immediately comparable between different
proteins.
In order to demonstrate that in-cell measurements are
feasible, xenopus laevis oocytes were injected with CYP101
C58T3 (final in-cell concentration 250 mm). The injected cells
were placed in a quartz tube, shock frozen and subjected to
Figure 3. a) Q-band RIDME time traces of CYP101 mutant C58 labeled
with 1 (blue solid line), 3 (green solid line) and MTSSL (red solid line)
overlayed with the corresponding DeerAnalysis fits (black dashed
lines). The corresponding distance distributions are shown in b) for
C58T1, c) C58T3 and d) C58R1. The purple lines are the mtsslWizard
predictions.
III
trityl-Fe Q-band RIDME measurements (Figure 4).
The obtained RIDME time trace (see the Supporting
Information) was background corrected using a polynomial of
the same order as for the in vitro time trace revealing
À1/2
a modulation depth of 4% and a SNR of 1.97 S/Nmin . The
Angew. Chem. Int. Ed. 2016, 55, 1 – 6
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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