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Local unwinding during replication results in overwinding or supercoiling of surrounding regions
DNA topology
Lk = Tw + Wr
From the field of topology:twist (Tw) = # of dsDNA turnswrithe (Wr) = # of times the helix turns on itselflinking number (Lk) = sum of twist and writhe
Molecules that differ only by Lk are topoisomers of eachother.Lk can only be changed by breaking covalent bonds
Adding 1 negative supercoil reduces Lk by 1
Biochemistry, 5th ed. Berg, Tymoczko, Stryer
DNA topology
Two types of supercoiling
Wasserman & Cozzarelli, Science 1986
Topoisomerases
Type I topoisomerases:- produce transient single-strand breaks (nicks)- remove one supercoil per cycle
- changes linking number by 1 or n- ATP-independent- examples= topo I, topo III, reverse gyrase
Type II topoisomerases:- produce transient double-strand breaks- remove both positive and negative supercoiling
- changes linking number by +/- 2- ATP-dependent- examples= topo II, topo IV, DNA gyrase
Reduce supercoiling strain by changing the linking number of supercoiled DNA
Corbett KD & Berger JM (2004) Structure, molecular mechanisms, and evolutionary relationships in DNA topoisomerases. Annu Rev Biophys Biomol Struct 33, 95–118.
Strand passage by topoisomerases
e.g. DNA Gyrase
DNA Gyrase
• one of two E. coli type II topoisomerases• relaxes (+) supercoils• introduces (–) supercoils• exhibits ATP-independent (–) supercoil
relaxation• Structure:
– α2β2 heterotetramer (GyrA2GyrB2)– binds 140 bp DNA– GyrA-CTD wraps DNA– GyrB-NTD ATPase, N-gate (entry)– GyrA-NTD C-gate (exit)
Figure 1 DNA Gyrase mechanism of action
model for introduction of (-) supercoils: “α mode”
This model does not account for other activities of gyrase- (+) and (-) supercoil relaxation- decatenation - passive relaxation
and the dependence on force and torque in the experiments
G and T proximal
Figure 2 Magnetic tweezers experimental setup
• 15.7 kb DNA molecule with biotinylated or digoxigenated ends• 4 mM MgCl2, 1 mM ATP
• supercoiling quantitatively introduced by rotation of magnets• change in bead position monitored by comparing calibrated diffraction ring patterns
Figure 3 Gyrase activity at low forces
Starting with (+) supercoiled DNA
obs: DNA extended (supercoiling relaxed)
Starting with (+) supercoiled DNA at slightly lower force,obs: DNA extended (supercoiling relaxed), then (-) supercoiling introduced (DNA shortened)
Figure 4 Gyrase activity at high forces
Starting with (+) supercoiled DNA at high tensions:
obs: processive relaxation can occur at high force (tension).
velocity independent of force between 1.5 – 4.5 pNwrapping independent mechanism
“χ- mode” activity“distal T-capture” where G-segment and T-segment are not proximal i.e.:discontinuous DNA segments juxtaposed by plectonemic crossings
G-segment
T-segment
2.5 pN
4.5 pN
Figure 4 Gyrase activity at high forcesDoes high force (+) relaxation require (+) crossings?
(test of “χ-mode” model)
Experiment:110 (+) supercoils introduced, then allowed to be relaxed by gyrase.Then, 110 new supercoils introduced while monitoring length.
Observation:Linear decrease in extension, indicates DNA not relaxed past buckling transition
Consistent with χ-mode relaxation
buckling transition
High force relaxation requires plectonemic crossings (distal T-segments)
Figure 5 Passive relaxation moderelaxation in the absence of ATP
Requires high concentrations of gyrase(20 nM vs 1 nM)
Relaxation observed only for (-) supercoils, and requires plectonemic DNA.(+) supercoil relaxation experiment not shown
Modulation between modes by force
blue= high force passive relaxation of (-) supercoils
yellow = low force α-mode ATP-dependent introduction of (-) supercoils
supp fig 3
ATP does not stimulate (-) supercoil relaxation at forces that inhibit α-mode (0.6 pN)
Start with (-) supercoiled DNA, gyrase, no ATP
obs: processive relaxation at moderate forces.
p-mode requires plectonemes
Three distinct modes observed
1. α-mode: (+) supercoil relaxation, (-) supercoil introduction- ATP-dependent- wrapping mediated- inhibited by high force- proximal T-segment capture
2. χ-mode: (+) supercoil relaxation- ATP-dependent- wrapping independent- processive at high force- distal T-segment capture- requires (+) plectonemes
3. Passive mode: (-) supercoil relaxation- ATP-independent- requires (-) plectonemes- processive at forces that inhibit α-mode
Important observation:not stimulated by ATP
Figure 6 Experiments with DNA braids
DNA braids allow more direct measurements of plectonemic associated modes
Functional predictions:1. Under high force to inhibit wrapping, χ-mode activity should
unbraid L-braided DNA (identical to (+) supercoils)
2. (-) supercoil relaxation strictly ATP-independent suggests chiral preference for distal T-segment capture, thus R-braids should not be relaxed
Figure 6 Gyrase unbraiding DNA
Gyrase rapidly and completely unbraids L-braids ATP-dependently
R-braids are not a substrate for gyrase regardles of ATP, enzyme or force.
L-braids(+) supercoils
1 mM
Braids have zero torque.Indicating that passive-mode relaxation requires negative torque
Putting it all together:Mechanochemical modeling
Figure 7 Branched model for gyrase activity
dominates at low force
dominates at high force
dominates at high negative torque
Figure 7 Force-Velocity curves and proposed mechano-chemical model
where:n= α, χ, or p
kn= rate at zero F and τΔxn= extension distance to transition state Δθn= twist angle to transition state
RL= rate limiting step
rising phase due to dependence of kα, RL on torque
zero-order kχ phase
decrease first by kα sensitivity to forcethen by competition with kp (-) sc introduction
DNA Gyrase operates in three distinct modes
Explains prior puzzling observations• gyrase “slippage” uncoupling of ATP hydrolysis from (-) sc relaxation
• Distal T-capture explains how gyrase can relax circles smaller than the minimum wrapping size
• explains the low-level decatenation in vivo• decatenase activity stimulated by tension forces
• conditional lethality of segregation defects rescued by SetB overexpression SetB induces DNA tension