Search

Complexes formed between phi29 DNA polymerase (DNAP) and DNA fluctuate discretely between the pre-translocation and post-translocation states on the millisecond time scale. The translocation fluctuations can be observed in ionic current traces when individual complexes are captured atop the α-hemolysin nanopore in an electric field. The presence of complementary 2'-deoxynucleoside triphosphate (dNTP) shifts the equilibrium across the translocation step toward the post-translocation state. Here we have determined quantitatively the kinetic relationship between the phi29 DNAP translocation step and dNTP binding. We demonstrate that dNTP binds to phi29 DNAP-DNA complexes only after the transition from the pre-translocation state to the post-translocation state; dNTP binding rectifies the translocation but it does not directly drive the translocation. Based on the measured time traces of current amplitude, we developed a method for determining the forward and reverse translocation rates and the dNTP association and dissociation rates, individually at each dNTP concentration and each voltage. The translocation rates, and their response to force, match those determined for phi29 DNAP-DNA binary complexes and are unaffected by dNTP. The dNTP association and dissociation rates do not vary as a function of voltage, indicating that force does not distort the polymerase active site and that dNTP binding does not directly involve a displacement in the translocation direction. This combined experimental and theoretical approach and the results obtained provide a framework for separately evaluating the effects of biological variables on the translocation transitions and their effects on dNTP binding.

Complexes formed between the bacteriophage phi29 DNA polymerase (DNAP) and DNA fluctuate between the pre-translocation and post-translocation states on the millisecond time scale. These fluctuations can be directly observed with single-nucleotide precision in real-time ionic current traces when individual complexes are captured atop the α-hemolysin nanopore in an applied electric field. We recently quantified the equilibrium across the translocation step as a function of applied force (voltage), active-site proximal DNA sequences, and the binding of complementary dNTP. To gain insight into the mechanism of this step in the DNAP catalytic cycle, in this study, we have examined the stochastic dynamics of the translocation step. The survival probability of complexes in each of the two states decayed at a single exponential rate, indicating that the observed fluctuations are between two discrete states. We used a robust mathematical formulation based on the autocorrelation function to extract the forward and reverse rates of the transitions between the pre-translocation state and the post-translocation state from ionic current traces of captured phi29 DNAP-DNA binary complexes. We evaluated each transition rate as a function of applied voltage to examine the energy landscape of the phi29 DNAP translocation step. The analysis reveals that active-site proximal DNA sequences influence the depth of the pre-translocation and post-translocation state energy wells and affect the location of the transition state along the direction of the translocation.

Complexes of phi29 DNA polymerase and DNA fluctuate on the millisecond time scale between two ionic current amplitude states when captured atop the α-hemolysin nanopore in an applied field. The lower amplitude state is stabilized by complementary dNTP and thus corresponds to complexes in the post-translocation state. We have demonstrated that in the upper amplitude state, the DNA is displaced by a distance of one nucleotide from the post-translocation state. We propose that the upper amplitude state corresponds to complexes in the pre-translocation state. Force exerted on the template strand biases the complexes toward the pre-translocation state. Based on the results of voltage and dNTP titrations, we concluded through mathematical modeling that complementary dNTP binds only to the post-translocation state, and we estimated the binding affinity. The equilibrium between the two states is influenced by active site-proximal DNA sequences. Consistent with the assignment of the upper amplitude state as the pre-translocation state, a DNA substrate that favors the pre-translocation state in complexes on the nanopore is a superior substrate in bulk phase for pyrophosphorolysis. There is also a correlation between DNA sequences that bias complexes toward the pre-translocation state and the rate of exonucleolysis in bulk phase, suggesting that during DNA synthesis the pathway for transfer of the primer strand from the polymerase to exonuclease active site initiates in the pre-translocation state.

Coupling nucleic acid processing enzymes to nanoscale pores allows controlled movement of individual DNA or RNA strands that is reported as an ionic current/time series. Hundreds of individual enzyme complexes can be examined in single-file order at high bandwidth and spatial resolution. The bacteriophage phi29 DNA polymerase (phi29 DNAP) is an attractive candidate for this technology, due to its remarkable processivity and high affinity for DNA substrates. Here we show that phi29 DNAP-DNA complexes are stable when captured in an electric field across the α-hemolysin nanopore. DNA substrates were activated for replication at the nanopore orifice by exploiting the 3'-5' exonuclease activity of wild-type phi29 DNAP to excise a 3'-H terminal residue, yielding a primer strand 3'-OH. In the presence of deoxynucleoside triphosphates, DNA synthesis was initiated, allowing real-time detection of numerous sequential nucleotide additions that was limited only by DNA template length. Translocation of phi29 DNAP along DNA substrates was observed in real time at Ångstrom-scale precision as the template strand was drawn through the nanopore lumen during replication.

DNA polymerases are molecular motors that catalyze template-dependent DNA replication, advancing along template DNA by one nucleotide with each catalytic cycle. Nanopore-based measurements have emerged as a single molecule technique for the study of these enzymes. Using the alpha-hemolysin nanopore, we determined the position of DNA templates bearing inserts of abasic (1',2'-dideoxy) residues, bound to the Klenow fragment of Escherichia coli DNA polymerase I (KF) or to bacteriophage T7 DNA polymerase. Hundreds of individual polymerase complexes were analyzed at 5 A precision within minutes. We generated a map of current amplitudes for DNA-KF-deoxynucleoside triphosphate (dNTP) ternary complexes, using a series of templates bearing blocks of three abasic residues that were displaced by approximately 5 A in the nanopore lumen. Plotted as a function of the distance of the abasic insert from n = 0 in the active site of the enzyme held atop the pore, this map has a single peak. The map is similar when the primer length, the DNA sequences flanking the abasic insert, and the DNA sequences in the vicinity of the KF active site are varied. Primer extension catalyzed by KF using a three abasic template in the presence of a mixture of dNTPs and 2',3'-dideoxynucleoside triphosphates resulted in a ladder of ternary complexes with discrete amplitudes that closely corresponded to this map. An ionic current map measured in the presence of 0.15 M KCl mirrored the map obtained with 0.3 M KCl, permitting experiments with a broader range of mesophilic DNA and RNA processing enzymes. We used the abasic templates to show that capture of complexes with the KF homologue, T7 DNA polymerase, yields an amplitude map nearly indistinguishable from the KF map.

DNA polymerases catalyze template-dependent genome replication. The assembly of a high affinity ternary complex between these enzymes, the double strand-single strand junction of their DNA substrate, and the deoxynucleoside triphosphate (dNTP) complementary to the first template base in the polymerase active site is essential to this process. We present a single molecule method for iterative measurements of DNA-polymerase complex assembly with high temporal resolution, using active voltage control of individual DNA substrate molecules tethered noncovalently in an alpha-hemolysin nanopore. DNA binding states of the Klenow fragment of Escherichia coli DNA polymerase I (KF) were diagnosed based upon their ionic current signature, and reacted to with submillisecond precision to execute voltage changes that controlled exposure of the DNA substrate to KF and dNTP. Precise control of exposure times allowed measurements of DNA-KF complex assembly on a time scale that superimposed with the rate of KF binding. Hundreds of measurements were made with a single tethered DNA molecule within seconds, and dozens of molecules can be tethered within a single experiment. This approach allows statistically robust analysis of the assembly of complexes between DNA and RNA processing enzymes and their substrates at the single molecule level.

This paper demonstrates feedback voltage control of a single DNA molecule tethered in a biological nanopore. The nanopore device monitors ionic current through a single protein pore inserted in a lipid bilayer. The limiting aperture of the pore is just sufficient (1.5 nm diameter) to accommodate single-stranded DNA. The tethered DNA is double stranded on each end, with a single stranded segment that traverses the pore. Voltage control is used to regulate the motion of the tethered DNA, for repeated capture and subsequent voltage-promoted dissociation of DNA-binding enzymes above the nanopore. In initial experiments using the Klenow fragment of Escherichia coli DNA polymerase I, control of 8 independent tethered DNA molecules yielded 337 dissociation events in a period of 380 seconds. The resulting distribution of DNA-protein dissociation times can be used to model the free energy profile of dissociation. Moreover, the approach is applicable to numerous enzymes that bind or modify DNA or RNA including exonucleases, kinases, and other polymerases.