Most DNA-based
molecular motors are ‘linear-tracking’ motors and use the repetitive
nature of the repeating nucleotide base-pair to enable them to move along
DNA. The best example, and one of the most closely studied at the single-molecule
level, is RNA polymerase (Harada et al., 2001) . This enzyme is responsible
for synthesis of messenger RNA (the reading intermediate between DNA and
protein) and uses the energy of this synthesis reaction to enable movement
along the DNA, reading the bases as it moves and copying them into a single
chain RNA molecule. Many other motors follow this pattern but usually have
different functions and as a consequence interact differently with DNA (e.g.
DNA helicases are responsible for unwinding the two strands of DNA, DNA
polymerase synthesises a new strand of DNA, DNA repair enzymes are able
to detect and remove damaged bases in the DNA).
Single molecule studies
of RNA polymerase (and other polymerases) have involved immobilisation
of the motor (enzyme) onto a surface; the enzyme will then bind the DNA,
which carries a bead at one end (Schafer et al., 1991) . This stage is
then followed by measurement of the forces exerted on the bead, required
to stall movement along the DNA, by means of an optical trap (effectively
a laser light that ‘holds’ the bead at its point of focus).
However, there is
another type of DNA-based molecular motor that interacts with a specific
site on the DNA and then moves the remaining DNA toward that site. These
motors belong to a large superfamily (SF-II) of
helicase-like
enzymes (Flaus and Owen-Hughes, 2001) and are particularly well illustrated
by Type I restriction-modification (R-M) enzymes, but also include type
III R-M enzymes, chromatin remodelling factors and a few chimeric enzymes.
Type I R-M enzymes are distinguished from other restriction enzymes by
the fact that binding to an unmethylated recognition site on the DNA,
elicits DNA cleavage at a distantly located, non-specific site on the
same DNA molecule. ATP, which is required for DNA restriction, fuels translocation
of the distal DNA toward the recognition site (Figure 1). Cleavage occurs
when translocation is blocked (Figure 2 and Janscak et al., 1999b) , which
can be due to collision with another type I R-M enzyme, or due to lack
of DNA to translocate (e.g. on circular DNA Szczelkun et al., 1996) .
Rotation is also an inevitable outcome of this translocation as the regular
binding surfaces on the DNA are arrayed helically and the translocating
motor follows the helical groove. Figure 1
The solid block represents the recognition
sequence for the enzyme. The enzyme binds
at this site and upon addition of ATP DNA
translocation begins. During translocation,
an expanding loop is produced.
These enzymes
are unusual in that they are simple actuators – they move one part
of the DNA relative to another section of the DNA and do not require immobilisation
on a surface to reproduce measurable motion (although the DNA needs to
be surface attached for an observable displacement of a bead). This suggests
a simple mechanism for detecting DNA movement through the use of a magnetic
bead. In the case of type I R-M enzymes cleavage must be prevented in
order to provide a useful molecular motor.
The simplest device
for measuring such movement is a magnetic tweezer device. Magnetic tweezers
allow real time monitoring of protein DNA interactions without surface
interference and with femtonewton sensitivity. In addition, these systems
can measure DNA displacements as low as 10nm as well as being able to
produce negative, or positive, supercoils into the DNA, one turn at a
time, through manipulation (spinning) of the magnetic bead (Strick et
al., 1999; Strick et al., 2000).
Figure 2
A) The open box is the DNA binding site
for the motor. (B) The wild-type enzyme
has two motor subunits that translocate
the adjacent DNA in a bi-directional fashion.
(C) The hatched block represents a
blockage attached to the DNA.
Collision between the motor and the
blockage results in DNA cleavage.