1296 VOLUME 18 NUMBER 11 NOVEMBER 2011 nature structur al & molecular biology
Previous studies indicated that the C-terminal tail of Tfam is essential
for transcriptional activation
8
and physical interaction with Tfb2m
9
.
In the crystal structure, when Tfam is bound to the LSP promoter, the
HMG-box B domain binds at the half-site further upstream from the
transcription start site (Figs. 1c and 6c). Without DNA bending,
the C-terminal tail would face away from the transcriptional start
site (Fig. 6d). However, the DNA U-turn redirects the C-terminal
tail toward the transcriptional machinery (Fig. 6c). We speculate
that one of the functions of DNA bending by Tfam is to enable the
C-terminal tail to interact with the rest of transcriptional machinery.
Based on previous results
9
, Tfb2m is a favored candidate for such an
interaction. Remarkably, transcription from HSP1 is much less sensi-
tive to DNA bending by Tfam. Based on sequence analysis, the Tfam
binding sites in HSP1 versus LSP are in reverse orientations relative to
the direction of transcription
4,8
(Fig. 1b). When Tfam is bound to the
HSP1 promoter, HMG-box B would be expected to bind the half site
adjacent to the transcriptional start. The C-terminal tail is therefore
in proximity to the transcriptional machinery, regardless of whether
the DNA is bent or not. In future studies, it will be important to test
this proposal by determining the structure of Tfam in complex with
HSP1 promoter DNA.
METHODS
Methods and any associated references are available in the online
version of the paper at http://www.nature.com/nsmb/.
Accession codes. Protein Data Bank: atomic coordinates and
structure factors for the Tfam–mtDNA complex have been deposited
under the accession code 3TMM.
Note: Supplementary information is available on the Nature Structural
&
Molecular
Biology website.
ACKNOWLEDGMENTS
We thank N. Chan (California Institute of Technology) for making some
mutant constructs, Y. Zhang and Z. Liu (California Institute of Technology)
for suggestions on phase determination and structure refinement, T. Walton
(California Institute of Technology) for advice on SEC-MALS, S. Shan (California
Institute of Technology) for use of equipment and insightful discussions, the
staff at the Stanford Synchrotron Radiation Lightsource (SSRL) for technical
support with crystal screening and data collection, and members of the Chan
laboratory for critical reading of the manuscript. We acknowledge the Gordon
and Betty Moore Foundation for support of the Molecular Observatory at Caltech.
SSRL is supported by the US Department of Energy and National Institutes of
Health (NIH). This work was supported by NIH grants GM083121 (D.C.C.) and
GM062967 (D.C.C.).
AUTHOR CONTRIBUTIONS
H.B.N. and D.C.C. designed the experiments, analyzed the data and wrote the
paper. H.B.N. carried out the crystallography and performed the experimental
work. J.T.K. helped with the crystallographic analysis.
COMPETING FINANCIAL INTERESTS
The authors declare no competing financial interests.
Published online at http://www.nature.com/nsmb/.
Reprints and permissions information is available online at http://www.nature.com/
reprints/index.html.
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a r t i c l e s
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