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.
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.
Perhaps the only drawback is the question of the influence of the applied force on the function of the enzyme, but this does not seem to be a problem and single molecule data has been found to closely match bulk solution analysis using strand displacement (Seidel et al 2008).
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.
More recently, the AFM has been used to also study the subunit assembly of Type I R-M enzymes by measuring molecular volumes of different complexes formed with different cofactors and antagonists, or by using applied forces to pull apart the complexes and measure the forces involved in protein-protein interactions (unpublished observations).
Last modified on
21 September 2011
© Dr Keith Firman
Author Dr Keith Firman.