The concept of single-molecule analysis with Type I R-M enzymes was to make use of a Magnetic Tweezer Setup to study DNA-translocators, these enzymes are DNA-based molecular motors that, unlike other DNA-based enzymes such as polymerases, do not simply track along the DNA, but instead remain bound at their recognition site and move the DNA ends relative to this site (this makes them a simple nanoactuator – Figure 2). There potential use in nanodevices is made easier because they do not depend upon surface attachment of the motor to enable relative motion of the end of the DNA (as is required for a polymerase - Harada et al., 1999; Wang et al., 1998), but only surface attachment of DNA, which is a relatively simple process.

Magnetic tweezers allow real time
monitoring of protein DNA interactions without surface
interference and with femtonewton sensitivity. This system can
measure DNA displacements as low as 10nm. The magnetic bead
required for these measurements will be attached to the end of the
DNA through the biotin molecules incorporated into the DNA (see
above). The other end of the DNA is surface attached,
through incorporation of digoxygenin (DIG) into the DNA and
surface coating of anti-DIG within the flowcell. The system
is also able to produce negative, or positive, supercoils into the
DNA, one turn at a time, through manipulation (spinning) of the
magnetic bead. By using DNA molecules with single binding sites
the stalling forces and translocation forces can be determined. We
will also determine rate, processivity, pausing and step-size as a
function of ATP concentration.Figure 2
The beauty of this system is two-fold:
(i) Real-time measurements of translocation can be made with both R1-
and R2-complexes.
(ii) The magnetic bead, bound to the DNA, can be physically rotated by the
external magnets of the system. Provided the DNA substrate is NOT nicked,
this results in the introduction of positive or negative supercoils in the DNA
(dependent upon the direction of rotation). This allows us to study the
effect of supercoiling on translocation as well as measure supercoiling that is
induced by the translocation.
Using AFM
we have recently been able to show images of DNA translocation and shown that
two loops are formed from a R2-complex (see Figure below and
van
Noort et al 2005) as expected. However, one unexpected result
for the AFM studies was that the rate of translocation is far lower than that
observed in solution (some 10-fold). Despite this problem, AFM represents
the quickest method for visualising translocation with single-molecules.
Last modified on
24 July 2010
© University of Portsmouth
Author Dr Keith Firman.