Introduction
- Sucato C.A.
- Upton T.G.
- Kashemirov B.A.
- Batra V.K.
- Martínek V.
- Xiang Y.
- Beard W.A.
- Pedersen L.C.
- Wilson S.H.
- McKenna C.E.
- Florián J.
- Warshel A.
- Goodman M.F.
Results
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Pol β binds better to DNA with a 5′-phosphate group

The effects of DNA gap size and 5′-phosphate on nucleotide incorporation
Substrate | Gap size | 5′-P | kpol | Kd (dNTP) | kpol/Kd (dNTP) |
---|---|---|---|---|---|
nt | s−1 | μm | s−1 μm−1 | ||
JS1+pT | 1 | Yes | 3.0 ± 0.1 | 1.5 ± 0.2 | 2.0 ± 0.3 |
JS1−pT | 1 | No | 2.5 ± 0.1 | 4.6 ± 0.4 | 0.5 ± 0.1 |
JS3+pT | 3 | Yes | 1.7 ± 0.0 | 3.9 ± 0.2 | 0.4 ± 0.0 |
JS3−pT | 3 | No | 1.6 ± 0.0 | 43.8 ± 4.8 | 0.04 ± 0.00 |
JS5+pT | 5 | Yes | 1.2 ± 0.0 | 12.1 ± 1.7 | 0.1 ± 0.0 |
JS5−pT | 5 | No | 1.4 ± 0.1 | 73.0 ± 9.9 | 0.02 ± 0.00 |
JT | Recessed | No | 1.8 ± 0.1 | 32.5 ± 4.0 | 0.06 ± 0.01 |

Formation of binary complexes depends on the DNA substrates

JS1+pT | JS1−pT | JS3+pT | JS3−pT | JS5+pT | JS5−pT | JT | |
---|---|---|---|---|---|---|---|
Binary (Å) | 44.8 ± 0.6 | 51.4 ± 1.2 | 47.7 ± 0.6 | 53.5 ± 0.6 | 47.3 ± 0.7 | 51.7 ± 1.3 | 52.7 ± 0.8 |
Ternary (Å) | 40.6 ± 0.7 | 41.9 ± 1.0 | 40.7 ± 0.8 | 41.8 ± 1.0 | 41.8 ± 0.2 | 40.7 ± 0.1 | 40.3 ± 0.4 |
Pre-catalytic conformational changes depend on the gap size and 5′-phosphate



Reverse fingers closing for JS1+pT and JS1-pT DNA


Discussion
DNA substrate influences binary complex conformation
The fingers and lyase domains interact upon formation of the ternary complex with single-nucleotide gapped DNA


Gap size and the presence of 5′-phosphate influence rates of pre-catalytic conformational changes
The NCS requires single-nucleotide gapped DNA
Conclusion
Experimental procedures
Generation of IAEDANS-labeled human WT Pol β
Generation of DNA substrates
Gel mobility shift assay
where m is a scaling factor and b is the apparent minimum Y value.
Single-turnover kinetics
for each nucleotide concentration, where A is the amplitude of product formation, kobs is the observed rate, and t is the time. The kobs from these fits were plotted versus [dCTP] and fitted to the hyperbolic equation 3,
where kpol is the polymerization rate of the enzyme and Kd (dNTP) is the equilibrium dissociation constant of the incoming dNTP from the Pol β–DNA binary complex.
Steady-state fluorescence emission scan
where FDA is the emission of IAEDANS at 490 nm in the presence of Dabcyl and FD is the fluorescence of IAEDANS in the absence of Dabcyl-labeled DNA. The efficiency was then used in equation 5 to estimate the distance separating the two probes (r),
where R is the Förster radius, defined as the distance at which energy transfer is 50%. This distance was estimated to be 37.76 Å using equation 6,
where κ2 is the relative orientation of the transition dipoles of the probes and is assumed to be equal to ⅔ for a dynamic random average, and η is the refractive index, assumed to be 1.344 in a solution of Tris-HCl (
where we measured ED, the maximum normalized emission of IAEDANS and ϵA, the extinction coefficient of Dabcyl at each wavelength (λ).
Stopped-flow FRET
KinTek Explorer modeling
Author contributions
Supplementary Material
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Footnotes
This work was supported by NCI, National Institutes of Health Grant R01 CA080830 (to J. B. S.). The authors declare that they have no conflicts of interest with the contents of this article. The content is solely the responsibility of the authors and does not necessarily represent the official views of the National Institutes of Health.
This article contains Figs. S1–S10.
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