Chapter 9 – Emerging Biophysics Techniques 409
For example (see Goodman et al., 2005), a tetrahedron can be made from four 55 nucleo
tide base DNA strands. Each of the six edges of the tetrahedron is composed of one of six
17-base “edge subsequences” (edge length ~7 nm), which is hybridized to its complementary
segment. Each DNA strand contains three of these subsequences, or their complements,
which are separated by short sequences specifically designed not to hybridize with a com
plementary strand, and thus act as a “hinge,” to ensure that the tetrahedron vertices have
flexibility to accommodate a 60° kink. Each strand runs around one of the four faces and is
hybridized to the three strands running around the neighboring faces at the shared edges,
and each vertex is a nicked three-arm junction, and can exist as two stereoisomers (see
Chapter 2). Such a structure has the potential for acting as nanoscale brick for more exten
sive synthetic 3D structures.
A valuable lesson to learn for the student is the importance of basic, rudimentary thought,
when it comes to the intellectual process of designing such nanostructures. When published
in research articles in their final form, fancy graphics are inevitably employed. However, the
initial intellectual process is often far more basic, down-to-earth, and human than this, as can
be seen wonderfully exemplified from the right panel of Figure 9.3b.
It is also possible to engineer larger DNA nanostructures than the simple 3D geometrical
shapes. These can include structures that are more complex than simple geometrical objects.
In principle, a single strand of DNA can be used to generate such structures, referred to as
the scaffold, though to hold it stably in place often requires several short sequences known as
staples, which pin down certain duplex regions relative to each other, which might be liable
to move relative to each other significantly otherwise. Such exotic structures have included
2D tiles, star shapes and 2D snowflake images, smiley faces, and embossed nanolettering,
even a rough nanoscale map of North and South America. Many of these exotic designs, and
the engineering principles used in their formulations, can be seen in the work of Caltech’s
Paul Rothemund in a pioneering research paper that was cited roughly 3000 times in the first
10 years since its publication, which says a great deal about the huge impact it has had to this
emerging field (Rothemund, 2006).
One limit to the size of an artificial DNA structure is mismatched defects. For example,
base pair interactions that do not rely on simple Watson–Crick base pairing. Although rela
tively uncommon, the effects over larger sections of DNA structures may be cumulative.
Also, the purification methods are currently relatively low throughput, which arguably has
limited extensive commercial exploitation for “useful” structures beyond the satisfaction of
designing nanoscale smiley faces, though it seems tempting to imagine that these techno
logical barriers will be reduced by future progress.
“Useful” DNA nanostructures include nanostructures that can be used as calibration tools
or standards for advanced fluorescence microscopy techniques. For example, since optimized
DNA nanostructures have well-defined atomic coordinates, then different color dyes can be
attached as very specific locations and used as a calibration sample in FRET measurements
(see Chapter 4).
Also, DNA origami can generate valuable 2D arrays that can be used as templates for the
attachment of proteins. This has enormous potential for generating atomic level structural
detail of membrane proteins and complexes. As discussed previously (see Chapter 7), there
are technical challenges of generating stable lipid–protein interactions in a large putative
crystal structure from membrane proteins, making it difficult to probe structures using x-ray
crystallography. The primary alternative technique of nuclear magnetic resonance (NMR)
(see Chapter 5) has associated disadvantages also. For example, it requires purified samples
>95% purity in the concentration of several mg mL−1 typically prepared from recombinant
protein to be prepared by time-consuming genetic modification of bacteria such as E. coli
(see Chapter 7). NMR is also relatively insensitive for small proteins whose molecular weight
is smaller than ~50 kDa.
The main alternative structural determination technique for membrane proteins is elec
tron cryo-EM that allows direct imaging of biomolecules from a rapidly frozen solution
supported on an electron-transparent carbon film and circumvents many of the problems
associated with NMR and x-ray crystallography (see Chapter 5). However, high electron
current flux in EM imaging can damage samples. Also, there are increased risks of protein