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A versatile platform for single-molecule enzymology of restriction endonuclease

    https://doi.org/10.1142/S179354581841002XCited by:1 (Source: Crossref)
    This article is part of the issue:

    Abstract

    Enzymes are the major players for many biological processes. Fundamental studies of the enzymatic activity at the single-molecule level provides important information that is otherwise inaccessible at the ensemble level. Yet, these single-molecule experiments are technically difficult and generally require complicated experimental design. Here, we develop a Holliday junction (HJ)-based platform to study the activity of restriction endonucleases at the single-molecule level using single-molecule FRET (sm-FRET). We show that the intrinsic dynamics of HJ can be used as the reporter for both the enzyme-binding and the substrate-release events. Thanks to the multiple-arms structure of HJ, the fluorophore-labeled arms can be different from the surface anchoring arm and the substrate arm. Therefore, it is possible to independently change the substrate arm to study different enzymes with similar functions. Such a design is extremely useful for the systematic study of enzymes from the same family or enzymes bearing different pathologic mutations. Moreover, this method can be easily extended to study other types of DNA-binding enzymes without too much modification of the design. We anticipate it can find broad applications in single-molecule enzymology.

    1. Introduction

    Enzymes, generally proteins or few ribonucleic acids, are macromolecular biological catalysts which play irreplaceable roles in almost every physiological activity in vivo. Many natural and artificial enzymes are developed for the acceleration of chemical reactions in the synthesis industry.13 For example, some complicated drugs can be produced by one-pot enzymatic synthesis in vitro.4 Enzymes are also important tools for molecular biology, bioengineering and materials science. Restriction enzymes and DNA ligases are indispensable tools for recombinant DNA techniques. Cas9 involved in CRISPR system is now the star for genome engineering,5,6 gene knockout or knockdown,7 transcriptional activation8 and cancer research.911 Many enzymes are used to construct hydrogels,1214 catalysts15,16 and drug delivery systems.1719 In all these applications, understanding the action mechanism of enzymes is critical, which lays the foundation for the improvement of their performances. On the other hand, the change of activities of enzymes in vivo due to mutations is tightly related with many diseases.20 Fundamental enzymology studies have a strong impact on medicine and healthcare. Many techniques, such as stopped-flow system21,22 and continuous-flow system,23,24 have been used to study enzymology at the bulk level.

    Single-molecule studies can provide many insights of enzymes that are otherwise inaccessible from bulk studies. Currently, single-molecule techniques have been proven to be powerful tools for studying folding dynamics of proteins2527 and DNA,2830 biomolecular interaction3133 and enzymatic reaction dynamics.3437 Specifically, single-molecule Förster resonance energy transfer (sm-FRET) is widely applied for studying the structure, dynamics and function of proteins at the single-molecule level in real-time.3841 In typical sm-FRET studies, a pair of donor–acceptor fluorescent dyes is introduced to suitable positions of the protein or nucleic acid structure. The distance change of the two labeled positions can be monitored by the FRET effect of the two fluorophores with nanometer resolution in situ, making it a perfect tool for enzymology.4144 However, these studies relied either on the specific labeling of enzyme and the substrate using fluorescent dyes3844 or on the intrinsic fluorescence of the products.45 The former method needs tedious fluorophore labeling and is technically difficult to implement to different systems. The latter one is limited to only a few enzyme systems. In addition, the labeling of fluorescent dyes might affect the intrinsic dynamic of an enzyme. Moreover, in many enzymological processes, the structural changes are too small to be detected even with the state-of-the-art sm-FRET techniques. Herein, we present a versatile platform to measure the activity of DNA endonuclease, based on Holliday junction (HJ) [Fig. 1(a)]. HJ comprises four arms namely X, B, R and H, with two stable native conformations: The “isoI” state with the B-arm far from the H-arm and the “isoII” state with the B-arm close to the H-arm [Fig. 1(b)].46 The intrinsic dynamics of HJ has been extensively studied by sm-FRET and theory.4649 We use the dynamics of HJ as the reporter for the enzymatic reactions taking place on the X-arm. We hypothesize that binding of an enzyme to the X-arm and subsequent enzymatic reactions can affect the intrinsic dynamics of HJ, thus can be detected by analyzing the dynamics of HJ. A similar method was used to study protein-DNA interaction previously by Sarkar et al.50 In this method, the fluorescent dyes are labeled on the reporter arms (H- and R-arms) of HJ instead of the enzyme or the substrate directly, which minimizes the side-effect of dye labeling on the dynamics and activity of the enzyme. Moreover, the enzyme-binding arm (X-arm) and the surface-immobilizing arm (R-arm) are decoupled with the reporter arms, providing plenty of opportunities for the studies of various DNA-binding enzymes. In principle, this method can be used to quickly measure the activity of different enzymes without the need to change the fluorescent substrates. Using restriction enzymes as the example, enzyme binding may slow down the intrinsic dynamics of HJ due to the stabilizing of the two native states. However, after the enzymatic reaction, the X-arm is cut and becomes shorter, leading to faster conversions between “isoI” and “isoII” states. Therefore, the substrate binding and catalytic activity can both be measured from the change of the dynamics of HJ. We have experimentally proved this idea using BamHI as the representative restriction endonuclease [Fig. 1(c)].

    Fig. 1.

    Fig. 1. (Color online) (a) The scheme of designed HJ. The b-strand (red), x-strand (orange), r-strand (blue), h-strand and biotin strand (both green) form the HJ with four arms (B, H, R and X). (b) The scheme of “isoI” and “isoII” states. The “isoI” state has longer distance between Cy3 and Cy5 than “isoII” state. (c) Surface immobilization strategy for sm-FRET experiments. The components are not drawn to relative scale.

    2. Method

    2.1. The preparation of HJ

    HJ-b-strand (5-Cy5-CCCTAGCAAGCCGCTGCTACGG) and HJ-h-strand (5-Cy3-CCGTAGCAGCGCGAGCGGTGGG) were purchased from Invitrogen (ThermoFisher Scientific, Inc., USA). HJ-x-strand (5-GAGGGATCCCCAGTTGAGCGCTTGCTAGGG), HJ-r-strand (5-CGGATGGCTACGATCCCACCGCTCGGCTCAACTGGGGATCCCTC) and biotin strand (5-CGTAGCCATCCGAT-Biotin) were purchased from GenScript (Nanjing, China). All the b-, h-, x-, h- and biotin-strands were dissolved in TN buffer (50mM Tris, 50mM NaCl, pH=8.0), respectively. Then, five kinds of strands were mixed in TN buffer to reach the final concentration of 1μM and the mixture was slowly annealed by PCR machine (slowly cooled from 95C to 15C, then raised to 65C and dropped to 25C for three cycles and finally cooled to 4C). The purity of HJ was confirmed by native-PAGE.

    2.2. The digestion of HJ

    The mixture of HJ and BamHI (R0136S, New England BioLabs, USA) was incubated at 37C for 1h and then analyzed by the denatured PAGE followed by silver staining.

    2.3. Modification of the glass coverslip

    The scheme of coverslip modification is shown in Fig. 1(c). Coverslip was biotinylated following previous reports.5153 The 0.15-mm glass coverslip (24×40mm2, Micro Cover Glasses No. 1, VWR International, LLC) was cleaned in piranha solution (98% H2SO4:30% H2O2=7:3, v/v) for 30min to be hydroxylated. After thoroughly rinsing with MilliQ-water, the coverslip was dried under argon airflow. Then we gently heat the coverslip using blast alcohol burner to decompose any possible fluorescent impurities. After cooling to room temperature, the hydroxyl-functional coverslip was immersed in acetone solution containing 10% (3-aminopropyl)triethoxysilane (APTES, Sigma-Aldrich, USA) for 30min and rinsed thoroughly with acetone and MilliQ-water, respectively. After being dried under argon airflow, the amino-functional coverslip was PEGylated by immersing in aqueous solution (pH=8.0) containing 100-mM NaHCO3, 15mg/mL Biotin-PEG-SVA (MW: 5 kDa, Laysan Bio, Inc., USA) and 150mg/mL Methyl-PEG-SVA (MW: 5kDa, Laysan Bio, Inc., USA) for at least 3h. Finally, the coverslip was rinsed thoroughly with MilliQ-water, followed by drying under argon airflow. The biotin-functional coverslip should be kept in dark and be used freshly.

    2.4. Sample cell for sm-FRET experiments

    The biotin-functional coverslip was made into a sandwich structure cell with several sample channels. TN buffer containing 1% Tween 20 (v/v) was added and incubated for 20min, and then was rinsed with TN buffer three times. TN buffer containing 200μg/mL streptavidin was added to each sample channel and incubated for 1min. After rinsing with TN buffer three times, TN buffer containing 10–50pM HJ was injected into the sample channel and incubated for 20min then rinsed with TN buffer three times.

    2.5. Sm-FRET experiments

    The single-molecule FRET experiments were executed on an Olympus IX-71 with an oil immersion UAPON 100×OTIRF objective lens (numerical aperture=1.49, Olympus). Cy3 was excited by a 532-nm laser and the emission fluorescence of Cy3 and that of Cy5 were split into two channels by a dichroic filter (FF640-FDi01, Semrock). The emission fluorescence of two channels passed through two band-pass filters (FF01-585/40 and FF01-675-67, Semrock), respectively, and the final fluorescence signals were collected by an electron-multiplying charge-coupled device camera (IXon897, Andor Technology). The sm-FRET experiments were carried out in Tris buffer (50mM Tris, pH=8.0) containing 50mM MgCl2. About 1-μL BamHI (20 units) was diluted in 100-μL Tris buffer (50mM Tris, 50mM MaCl2, pH=8.0) for digestion in sm-FRET experiments. Dynamics of the digested BamHI–HJ was obtained 20min later after an addition of BamHI. Here 0.8% (w/v) glucose, 1-mg/mL glucose oxidase, 0.04-mg/mL catalase and 2-mM Trolox were involved as oxygen scavenger system.54,55

    3. Results and Discussion

    3.1. Intrinsic dynamics of HJ with the BamHI restriction site (BamHI–HJ)

    We first used sm-FRET to study the intrinsic dynamics of the newly designed BamHI–HJ containing five strands and longer X- and R-arms. A typical trace of sm-FRET is shown in Fig. 2(a). Cy3 signal (green) and Cy5 signal (red) hopped stochastically between the states of low or high intensity. The efficiency of energy transfer Ewas calculated by Eq. (1) :

    E=ICy5(ICy3+ICy5),(1)
    where ICy3 and ICy5 were the signal intensities of Cy3 and Cy5, respectively. The transfer efficiency depends on the distance between Cy3 and Cy5, according to Eq. (2) :
    E=1(1+(rR0)6),(2)
    where r is the distance between Cy3 and Cy5 and R0 is the characteristic distance at which the sm-FRET efficiency is 0.5. As shown in Fig. 2(b), the transfer efficiency also switched at two conformational states. As the HJ changed to “isoI” state, Cy3 was separated from Cy5. As a result, the transfer efficiency dropped to lower state. Later, the HJ jumped back to “isoII” state, corresponding to higher transfer efficiency [Fig. 2(b)]. The collected traces were summed up to make a histogram. The histogram of sm-FRET efficiency shows a clear bimodal distribution [Fig. 2(c)]. The distribution was fitted by a double-Gaussian function and gave one state located at 0.23 and another state located at 0.71. These results confirmed that introducing the BamHI restriction site on HJ did not significantly change its conformational dynamics.46 The dwell time on each state was also measured [Figs. 2(d) and 2(e)]. The exponential fittings (dark red) gave the transition rates of 0.107s1 and 0.085s1, for “isoI” to “isoII” and “isoII” to “isoI”, respectively. The dynamics is summarized in Table 1. Both transition rates were much slower than the original HJ, with shorter X- and R-arms as reported by previous work.46 This also indicated that the dynamics of HJ is sensitive to the length of each arm. As a result, digesting the restriction site by BamHI should increase the dynamics of HJ.

    Fig. 2.

    Fig. 2. (Color online) (a) Typical traces of sm-FRET experiments. Green and red traces refer to Cy3 and Cy5 signals, respectively. (b) The dependence of efficiency of energy transfer on time. (c) The efficiency of energy transfer distribution of BamHI–HJ. Green curves are Gaussian fittings and dark blue curve is the sum of green curves. (d) The histogram for the dwell time at the “isoII” state. Dark blue curve is exponential fitting. (e) The histogram for the dwell time at the “isoI” state. Dark blue curve is exponential fitting. The data in (a)–(e) were collected in the absence of BamHI.

    Table 1. Results of dynamics.

    Transfer efficiencyTransition rate (s1)
    BamHI–HJisoI0.230.107
    isoII0.710.085
    Digested BamHI–HJisoI0.240.160
    isoII0.680.125
    Original HJaisoI0.25.7
    isoII0.66.1

    a Data from a previous work of McKinney et al.46

    3.2. Dynamics of the digested BamHI–HJ

    Before the sm-FRET experiments, we examined the efficiency of BamHI digestion in bulk using the PAGE gel. We constructed a complex of r-strand and x-strand following the similar protocol for HJ. This complex and BamHI–HJ were incubated with BamHI, respectively, for 1h before being analyzed using denatured PAGE. As shown in Fig. 3(c), both the digested BamHI–HJ (lane 4) and the digested complex (lane 6) had one additional band (red box), compared to the original BamHI–HJ (lane 5) and the complex (lane 7). This confirmed that the extended X-arm in BamHI–HJ can be effectively digested by BamHI. Next, we studied the dynamics of digested BamHI–HJ using sm-FRET. A typical FRET trace is shown in Fig. 3(a). The transfer efficiency hopped more quickly with shorter dwell time after BamHI digestion of the X-arm [Fig. 3(b)]. The distribution of transfer efficiency is also a clear bimodal distribution [Fig. 3(d)] and the double-Gaussian fitting yielded the efficiencies of 0.24 for “isoI” state and 0.68 for “isoII” state. The transfer efficiency of each state did not change much, compared to that of each state before digestion. The duration time of each state was used to create the histograms. The exponential fitting yielded the transfer rates of 0.160s1 and 0.125s1, for “isoI” to “isoII” and “isoII” to “isoI”, respectively [Figs. 3(e) and 3(f)]. The dynamics is summarized in Table 1. Note that the transfer rates for “isoI” to “isoII” and “isoII” to “isoI” increased by 50% and 47%, respectively, after BamHI digestion, suggesting that the dynamics of HJ can indeed serve as a reporter for the action of BamHI.

    Fig. 3.

    Fig. 3. (Color online) (a) Typical traces of digested BamHI–HJ. Green and red traces refer to Cy3 and Cy5 signals, respectively. (b) The time trajectory of the FRET efficiency. (c) The denatured PAGE results of BamHI digestion of HJ. Lane 1: h-strand, lane 2: r-strand, lane 3: biotin strand, lane 4: BamHI–HJ digested by BamHI, lane 5: BamHI–HJ only, lane 6: the complex of r-strand and x-strand digested by BamHI, lane 7: complex of r-strand and x-strand only and lane 8: low molecular weight DNA ladder (N3233L, New England BioLabs). (d) The efficiency of energy transfer distribution of BamHI–HJ after BamHI digestion. Green curves are Gaussian fittings to the two peaks and dark blue curve is the sum of the two Gaussian fitting curves. (e) The histogram for the dwell time at the “isoII” state. Dark blue curve is the exponential fitting. (f) The histogram for the dwell time at the “isoI” state. Dark blue curve is exponential fitting. The data in panels (a), (b) and (d)–(f) were collected after the digestion of BamHI.

    3.3. Direct observation of BamHI digestion based on the HJ dynamics

    As mentioned above, the transition rates of the two states both rose after the BamHI digestion. Statistically, the turnover between the two states will become faster. Thus, we define the average turnover frequency, f, which is equal to the average number of turnovers per second in few seconds, as a measurable quantity to distinguish the undigested and digested BamHI–HJ. As shown in Figs. 4(a) and 4(b), the signal jumped from one to another more frequently after BamHI was added to the system at about 16s (marked by orange arrow). We calculated the average turnover frequency in a time span of 10s. The frequency–time curves were fitted with the Boltzmann function shown in Eq. (3) :

    f=A2+(A1A2)(1+exp((tt0)dt)),(3)
    where f is the average turnover frequency as defined above, t is the time, A1, A2, t0 and dt are fitting parameters. The time interval Δt for the enzyme to finish the digestion reaction equals four times of dt based on Eq. (3) [Fig. 4(g)]. Note that, although f showed relatively large intrinsic fluctuations due to the non-Gaussian distribution (exponential) of the dwell time, such intrinsic fluctuations did not affect the two-state fitting too much. This is because the enzyme kinetics of BamHI is much slower than the dynamics of HJ. Moreover, the transition of f from the low state to the high state of each trace did not occur at the same time after the addition of BamHI [Figs. 4(c)–4(f)]. This lag time (τlag, time interval from adding enzyme to the midpoint of Δt, which is just the parameter t0) suggested the heterogeneous nature of the enzymatic reaction at the single-molecule level and corresponded to the combined time for an enzyme to bind to the restriction site on the X-arm and then successfully digest the substrate. The distributions of Δt and τlag are summarized in Figs. 4(h) and 4(i), respectively. Considering the enzyme substrate exists in three different states: unbound (U), bound (B) and cut (C), the kinetic relations among these states can be described as follows :
    [U]k1[B]k2[C],(4)
    where k1 and k2 refer to the binding rate and the digestion rate, respectively. The unbinding of enzyme from the substrate was ignored as we did not observe unbinding events (causing the increase of turnover frequency from the low state to the original state). For single-molecular turnover events, the probability, p(Δt), is defined as follows56 :
    p(Δt)=k2exp(k2Δt).(5)
    Fitting Eq. (5) to the experimental data yields k2 of 0.23s1, indicating that once binding on the restriction site, BamHI has a 90% probability to finish cutting in 10s.

    Fig. 4.

    Fig. 4. (Color online) (a) Typical trace and (b) transfer efficiency during the BamHI digestion process. The orange arrow shows the moment when BamHI is added. (c)–(f) Four representative traces of the turnover frequency. BamHI was added at time 0. (g) Fitting scheme of panels (c)–(f). Here Δt is the time interval for the enzyme to finish the digestion reaction and τlag is the time needed from the addition of BamHI to the midpoint of Δt. (h) Histogram of the time span for each transition (Δt). Dark blue curve is exponential fitting. (i) The distribution of the lag time (τlag). Dark blue curve is the fitting to Eq. (6).

    As the lag time, τlag, is the combined time for binding and digestion processes, the probability of τlag for the serial events at the single-molecule level can be described as shown in Eq. (6) (Ref. 56) :

    p(τlag)=k1k2(ek1τlagek2τlag)(k2k1).(6)
    Fitting Eq. (6) to the data with fixed k2 of 0.230s1 yielded k1 of 0.0286s1, which is nearly one-fold slower than k2 [Fig. 4(i)]. This is probably due to the low concentration of BamHI used in the reaction condition. These experiments demonstrated the successful measurement of kinetics of BamHI digestion at the single-molecule level using the dynamics of HJ as the reporter.

    4. Conclusion

    In summary, we developed a HJ-based platform to study the activity of restriction endonucleases at the single-molecule level using single-molecule FRET. This method allows the activity of different restriction endonucleases to be measured without extra work to change the fluorescent-labeled enzymes or substrates. Using BamHI as the representative example, we showed that both the enzyme-binding and the substrate-release events can be observed based on the distinct dynamics of HJ at the corresponding states. Since this new tool greatly simplifies the single-molecule studies of DNA-binding enzymes, we anticipate that it can be broadly applied to study more complicated and important enzymes and provides unprecedented information for the understanding of their functions.

    Conflict of Interest

    We have no conflict interest to declare.

    Acknowledgments

    Xin Wang and Jingyuan Nie contributed equally to this work. The authors greatly appreciate the financial support from National Natural Science Foundation of China (Grant Nos. 21522402, 11674153, 11374148, 11334004 and 21771103), the Fundamental Research Funds for the Central Universities (Nos. 020414380070, 020414380050 and 020414380058), Natural Science Foundation of Jiangsu Province (No. BK20160639) and the Shuangchuang Program of Jiangsu Province.