Model

Simulating the Science: RCA, RCT, and Beyond

RCA Model

Overview

This year, Lambert iGEM is utilizing rolling circle amplification (RCA) with padlock probes as one of the methods to detect circulating microRNAs (miRNA) in blood in order to diagnose coronary artery disease (CAD).

This reaction can be summarized in 4 steps:

  • Hybridization: miRNA binds to a padlock probe (Graugnard et al., 2010)
  • Ligation: SplintR, an enzyme, circularizes the miRNA to the padlock probe (Jin et al., 2016; Lohman et al., 2013)
  • Amplification: phi29 DNA polymerase uses the hybridized miRNA as a primer to begin amplification and create DNA rolling circle product (RCP) reporters (Esteban et al., 1993; Macdonald et al., 1994)
  • Detection: We are testing two different reporting mechanisms for RCA
    • Fluorophores and quenchers bind to the RCPs, decreasing fluorescence
    • Lettuce aptamers bind to RCPs, causing fluorescence

Development

To assist in corroborating and interpreting RCA reactions, Lambert iGEM incorporated a deterministic ordinary differential equations (ODE) system to simulate the reaction process. Our model converted several reactions in the RCA system into ODEs to correlate fluorescence, caused by RCP-fluorophore-quencher or RCP-aptamer reactions, to the initial miRNA concentration. Lambert iGEM also reached out to Dr. Mark Styczynski from the Georgia Institute of Technology to aid in the identification of parameters and initial steps for creating our models. He recommended useful functionalities on MATLAB and research tools to find important rate constants.

Signaling Pathway

The team used MATLAB’s SimBiology software to diagram each reaction using the Law of Mass Action and Michaelis-Menten equations. The Mass Action equations are used to diagram the collision of reactants in a solution, which is needed for most reactants in our reaction pathways (Zi, 2012). On the other hand, when enzymes are utilized, Michaelis-Menten equations are needed to properly diagram catalytic enzyme kinetics (Park, 2022; Zi, 2012). The pathway begins with the introduction of miRNA into the system and ends with either RCP-quencher-fluorophore (RFQ) (see Fig. 1) or RCP-aptamer activity (see Fig. 2) as the final reporter.

Figure 1. RCA reaction pathway with an RCP-quencher-fluorophore reporter system in MATLAB Simbiology
Figure 2. RCA reaction pathway with an RCP-aptamer reporter system in MATLAB Simbiology

Biochemical Reactions

The model contains a total of 7 biochemical reactions (see Fig. 1) for the RCP-fluorophore-quencher reporting mechanism and 4 biochemical reactions (see Fig. 2) for the RCP-aptamer reporting mechanism. The first 3 reactions, shown below, are identical for both reporter mechanisms:

Reactions Description
\(M + P \xrightarrow{k}MP\) Input miRNA (M) binds to the complementary arms of free padlock probes (P) to form miRNA-padlock probe complexes (MP)
\(MP + SplR \Longleftrightarrow MP_{circularized}\) miRNA-padlock probe complexes (MP) are ligated by SplintR ligase (SplR) to circularized complexes (MP_circularized)
\(MP_{circularized} + phi29 \Longleftrightarrow R_{free}\) Circularized miRNA-padlock probe complexes (MP_circularized) are extended by phi29 DNA polymerase (phi29) to create free DNA rolling circle products, or RCPs (R_free)

RCA with RCP-fluorophore-quencher reporters includes an additional 4 reactions:

Reactions Description
Free RCPs (R_free) bind to free fluorophores (F_free) to form RCP-fluorophore complexes (RF)
Free RCPs (R_free) bind to free quenchers (Q_free) to form RCP-quenchers complexes (RQ)
RCP-fluorophore complexes (RF) bind to free quenchers (Q_free) to form RCP-quencher-fluorophore complexes (RFQ)
RCP-quencher complexes (RQ) bind to free fluorophores (F_free) to form RCP-quencher-fluorophore complexes (RFQ)

Alternatively, RCA with RCP-aptamer reporters includes 1 more reaction:

Reactions Description
\(R_{free} + apt \xrightarrow{k_{rcpapt}} RCPapt\) Free RCPs (R_free) bind to free aptamers (apt) to form RCP-aptamer complexes (RCPapt)

Initial Values of Species

In order to simulate our reactions, our team needed to input quantities to initialize each component in our model. The initial value of each species was obtained from RCA wetlab protocols:

Variable Species Initial Value Units
M miRNA 0.5 picomoles
P padlock probes 0.05 picomoles
SplR SplintR 25 molecules
phi29 phi29 DNA polymerase 12.5 molecules
R_free free RCP 0 molecules
F_free free fluorophores 180664245 molecules
Q_free free quenchers 361328490 molecules
RF bound RCP-fluorophores 0 picomoles
RQ bound RCP-quenchers 0 picomoles
RFQ bound RCP-fluorophores-quenchers 0 picomoles
apt free lettuce aptamers 10 micromoles
RCPapt bound RCP-aptamers 0 picomoles

Parameters

Rate constants and degradation rates are required to input into our Mass Action Laws and Michaelis-Menten equations. These values were derived from literature or estimated if the values could not be found. The value of each parameter is shown below:

Variable Reaction Estimated Values Units
Mdeg rate constant for miRNA degradation 0.000019254 1/second
k_padlock rate constant for miRNA-padlock binding 32000 1/(moles*second)
Vmcircular maximal rate of reaction needed for Michaelis-Menten enzyme kinetics for MP-SplintR binding 0.008 moles/second
Kmcircular Michaelis-Menten constant for MP-SplintR binding 1 moles
Vmphi29 maximal rate of reaction needed for Michaelis-Menten enzyme kinetics for MP_circular-phi29 binding 112 moles/second
Kmphi29 Michaelis-Menten constant for MP_circular-phi29 binding 31 moles
RCPdeg rate constant for free RCP degradation 0 1/second
k1 forward reaction rate constant for free RCP and free fluorophore binding 1e12 1/(moles*second)
k2 backward reaction rate constant for free RCP and free fluorophore binding 0 1/second
k3 forward reaction rate constant for free RCP and free quencher binding 1e12 1/(moles*second)
k4 backward reaction rate constant for free RCP and free quencher binding 0 1/second
k5 forward reaction rate constant for bound RF and free quencher binding 1e12 1/(moles*second)
k6 backward reaction rate constant for bound RF and free quencher binding 0 1/second
k7 forward reaction rate constant for bound RQ and free fluorophore binding 1e12 1/(moles*second)
k8 backward reaction rate constant for bound RQ and free fluorophore binding 0 1/second
k_rcpapt rate constant for free RCP and free lettuce aptamer binding 1e7 1/(moles*second)

Ordinary Differential Equations

As mentioned previously, Lambert iGEM incorporated the Mass Action Kinetic Laws and Michaelis-Menten Equations to represent the reactions for the RCA model. We generated 12 ordinary differential equations for RCP-fluorophore-quencher reporters and 9 ODEs for RCP-aptamer reporters. The first six ODEs are identical for both reporting mechanisms, as shown below:

Ordinary Differential Equations
\(\frac{d[M]}{dt} = -(k_{padlock}[M][P] - M_{deg}[M])\)
\(\frac{d[P]}{dt} = -k_{padlock}[M][P]\)
\(\frac{d[SplR]}{dt} = -\frac{V_{mcircular}[MP]}{K_{mcircular} + [MP]}\)
\(\frac{d[MP]}{dt} = k_{padlock}[M][P] - \frac{V_{mcircular}[MP]}{K_{mcircular} + [MP]}\)
\(\frac{d[MP_{circular}]}{dt} = \frac{V_{mcircular}[MP]}{K_{mcircular} + [MP]} - \frac{V_{mphi29}[MP_{circular}]}{K_{mphi29} + [MP_{circular}]}\)
\(\frac{d[phi29]}{dt} = - \frac{V_{mphi29}[MP_{circular}]}{K_{mphi29} + [MP_{circular}]}\)

We designed 6 more equations to diagram the RCP-Fluorophore-Quencher reporting mechanism:

Ordinary Differential Equations
\(\frac{d[R_{free}]}{dt} = \frac{V_{mphi29}[MP_{circular}]}{K_{mphi29} + [MP_{circular}]} -(RCP_{deg}[R_{free}]) - (k_1[R_{free}][F_{free}] - k_2[RF]) - (k_3[R_{free}][Q_{free}] - k_4[RQ])\)
\(\frac{d[F_{free}]}{dt} = -(k_1[R_{free}][F_{free}] - k_2[RF]) - (k_7[F_{free}][RQ] - k_8[RFQ])\)
\(\frac{d[Q_{free}]}{dt} = -(k_3[R_{free}][Q_{free}] - k_2[RQ]) - (k_5[Q_{free}][RF] - k_6[RFQ])\)
\(\frac{d[RF]}{dt} = -(k_1[R_{free}][F_{free}] - k_2[RF]) - (k_5[Q_{free}][RF] - k_6[RFQ])\)
\(\frac{d[RQ]}{dt} = -(k_3[R_{free}][Q_{free}] - k_4[RQ]) - (k_7[F_{free}][RQ] - k_8[RFQ])\)
\(\frac{d[RFQ]}{dt} = -(k_7[F_{free}][RQ] - k_8[RFQ]) + (k_5[Q_{free}][RF] - k_6[RFQ])\)

We also designed 3 additional equations to account for the RCP-aptamer reporting mechanism:

Ordinary Differential Equations
\(\frac{d[R_{free}]}{dt} = \frac{V_{mphi29}[MP_{circular}]}{K_{mphi29}+MP_{circular}} - RCPdeg[R_{free}] - k_{rcpapt}[R_{free}][apt]\)
\(\frac{d[apt]}{dt} = -k_{rcpapt}[R_{free}][apt]\)
\(\frac{d[RCPapt]}{dt} = k_{rcpapt}[R_{free}][apt]\)

Assumptions

Our RCA ODE model assumes all rate constants remain constant due to a lack of external environmental factors. Thus, this model replicates only the miRNA-padlock probe binding process to simulate RCP production and RCP-quencher-fluorophore/RCP-aptamer binding. The model also assumes the total quantity of padlock probes, SplintR ligase, phi29 DNA polymerase, fluorophores, and quenchers is known initially and remain constant over time. Finally, DNA polymerase activity is expected to remain the same regardless of the primer, miRNA, or dNTP concentration.

Results

After developing a complete set of ODEs, we utilized Simbiology’s Model Analyzer to simulate the quantity of bound RCP-quencher-fluorophore (RFQ) complexes (see Fig. 3) and bound RCP-aptamers (see Fig. 4) over 60 minutes with 0.5 picomoles of miRNA initially. As bound RFQ increases, the amount of free RCP decreases, dimming the fluorescence of the system. Alternatively, as bound RCP-aptamers increase, the system increases in fluorescence.

RCA RFQ over Time
Figure 3. Simulation results of bound RFQ in molecules over 60 minutes

RCA RCP-Aptamer over Time
Figure 4. Simulation results of bound RCP-Aptamers in molecules over 60 minutes

Initially, the bound RCP-fluorophore-quencher complexes are produced at a relatively quick exponential increase. Over time, the RFQ binding rate slows as the graph reaches an asymptote at .0001 picomoles of bound RFQ (see Fig. 3). On the other hand, bound RCP-aptamer is initially produced slowly, but the binding rate eventually becomes constant, allowing the graph to become linear over time (see Fig. 4). To help our hardware team interpret fluorescence measurements back to miRNA quantities, we plotted various initial miRNA concentrations to free fluorophores (see Fig. 5) and bound RCP-aptamers (see Fig. 6), which are analogues to free fluorophores, after a fixed time of 60 minutes and found the curve of best fit for each.

Our hardware team characterized our frugal hardware, Micro-Q, with varying concentrations of fluorophores, and they determined a curve of best-fit to relate fluorophore concentration to relative fluorescence units (RFUs). Thus, our modeling team connected miRNA concentration to fluorophore concentration (see Fig. 5 and 6), while our hardware team correlated fluorophore concentrations to fluorescence in RFUs. Together, our modeling simulations and hardware graphs enable CADlock to accurately calculate miRNA concentrations by quantifying the fluorescence with Micro-Q.

miRNA vs RFQ
Figure 5. Relationship between miRNA concentrations ranging from 0 to 25 picomoles and RFQ binding in molecules and based on the deterministic ODE system after 60 minutes

miRNA vs RCP-Aptamer
Figure 6. Relationship between miRNA concentrations ranging from 0 to 5 picomoles and RCP-aptamer binding in molecules and based on the deterministic ODE system after 60 minutes

To experimentally assess the effectiveness of the RFQ reporting system, our wetlab team measured the fluorescence of varying linear probe complements, which are produced as rolling circle products in RCA, with constant quantities of quenchers and fluorophores. Our hardware team experimentally tested differing fluorophore concentrations on our plate reader, and we found a line of best fit between fluorophore concentration and RFUs: \(RFU = .908[fluorophores]\), where fluorophores were measured in micromolar concentrations (µM). Using this regression line, we derived a conversion rate between fluorophores concentration and fluorescence. Then, we modeled only the RFQ reporting system section of our overall model with different initial RCP concentrations to see how bound RFQ and free fluorophores changed, and we related initial RCP concentrations to fluorescence in RFUs (see Fig. 7). The negative logarithmic shape of our model is almost identical to our wetlab results, corroborating our experimentation (see Fig. 8 & 9). The variation in the scales of the two graphs can be attributed to micropipetting errors or differences in the plate reader used.

Modeled RCA RFQ to RFUs Reporter System
Figure 7. Modeled relation between free RCP in micromoles and fluorescence in RFUs from plate reader

Wet-Lab Complement Results
Figure 8. Wetlab experimental results correlating linear probe complements to fluorescence in RFUs from plate reader
Wet-Lab Complement Results with Modeling
Figure 9. Wetlab experimental results overlaid on ODE Model Simulation, showing a close match between Ordinary Differential Equation Model vs. Experimentation for Rolling Circle Amplification with Linear Probe Reporter Sensing Mechanism

After relating complement concentrations to fluorescence, we applied the same conversion rate to ultimately correlate initial miRNA concentrations to fluorescence in RFUs on our plate reader depending on whether we use RFQ reporters (see Fig. 10) or RCP-aptamer reporters (see Fig. 11). As seen by the wetlab experimentation, the concentration of miRNA versus fluorescence follows a negative logarithmic trend when RFQs are utilized (see Fig. 12), exactly as predicted by the model (see Fig. 10). Thus, our model strongly validates our RCA wetlab experimentation with RFQ reporters.

miRNA vs RFUs with RFQ Reporter Model
Figure 10. Modeled relationship between miRNA concentrations ranging from 0 to 25 picomoles with RFQ reporters and fluorescence in RFUs from plate reader

miRNA vs RFUs with RFQ Reporter Reporter Wet-Lab
Figure 11. Modeled relationship between fluorescence in RFUs from plate reader and miRNA concentrations ranging from 0 to 5 picomoles with RCP-Aptamer Reporter

miRNA vs RFUs with RCP-Aptamer Reporter Model
Figure 12. Experimental relationship between miRNA concentrations ranging from 0 to 25 picomoles with RFQ reporters and fluorescence in RFUs from plate reader

Although every plate reader will input different RFU values relative to the blank, sensitivity, and gain of the machinery, these charts can help CADlock users confirm the shape of their graphs when they test their own miRNAs in laboratories.

RCT Model

Overview

Along with the rolling circle amplification (RCA) mechanism, our team utilizes rolling circle transcription (RCT) to detect circulating microRNAs (miRNAs) in blood. This reaction follows 4 main steps:

  • Hybridization: miRNA binds to a padlock probe (Graugnard et al., 2010)
  • Ligation: SplintR circularizes the miRNA to the padlock probe (Jin et al., 2016; Lohman et al., 2013)
  • Amplification: T7 RNA polymerase uses the hybridized miRNA as a primer to begin amplification and create RNA Broccoli aptamer reporters (Esteban et al., 1993; Macdonald et al., 1994)
  • Detection: The Broccoli aptamers bind to fluorophores, inducing fluorescence (Chandler et al., 2018)

Development

RCA and RCT follow the same pathway until the padlock probe amplification: RCA requires phi29 DNA polymerase to produce DNA rolling circle products (RCP), whereas RCT employs T7 RNA polymerase to create RNA Broccoli aptamers (Chandler et al., 2018). To accommodate this change, we applied the same ODE equations as were applied in RCA but modified the rate constant values. Since RCT utilizes RNA aptamers as a reporting mechanism rather than DNA RCP, we used the Gibbs free energy equation to derive the aptamer binding affinity from rate constants found in existing literature (see Fig. 14) (Thevendran et al., 2020).

\[\Delta{G^\circ} = - RT\ln{K_{eq}} \longrightarrow K_{eq} = \frac{1}{k_{apt}} \longrightarrow k_{apt} = e^{-\frac{\Delta{G^\circ}}{RT}}\]

Figure 13. Deriving the aptamer binding affinity using the Gibbs free energy equation


The RCT model serves the same purpose as the RCA model, which is to assist our team in interpreting and designing our RCT experimentation. Using Dr. Styczynski’s advice, we incorporated deterministic ODE equations to model the reactions throughout the pathway. With an initial miRNA concentration input, our model predicts the final RNA and aptamer-fluorophore complex concentrations, which should support our future experimental data.

Signaling Pathway

Like RCA, the team utilized MATLAB’s SimBiology software to diagram each reaction in the RCT reaction and aptamer-fluorophore binding using the Law of Mass Action and Michaelis-Menten Equations (Zi, 2012). The pathway begins with the introduction of miRNA into the system and ends with the final aptamer-fluorophore complex activity (see Fig. 13).

SimBiology Pathway
Figure 14. RCT reaction pathway with a Broccoli aptamer-fluorophore reporting system in MATLAB Simbiology

Biochemical Reactions

The model contained a total of 4 biochemical reactions (see Fig. 14), described below:

Reactions Description
\(M + P \xrightarrow{k} MP\) Input miRNA (M) binds to the complementary arms of free padlock probes (P) to form miRNA-padlock probe complexes (MP)
\(MP + SplR \Longleftrightarrow MP_{circularized}\) miRNA-padlock probe complexes (MP) are ligated by SplintR ligase (SplR) to circularized complexes (MP_circularized)
\(MP_{circularized} + T7_{poly} \Longleftrightarrow aptamer\) Circularized miRNA-padlock probe complexes (MP_circularized) are extended by T7 RNA polymerase (T7poly) to create a Lettuce aptamer (aptamer)
\(aptamer + fluorophore \xrightarrow{k_{apt}} aptfluorophore\) The aptamers (aptamer) bind to free fluorophores (fluorophore) to form aptamer-fluorophore complexes (aptfluorophore)

Initial Values of Species

In order to simulate our reactions, our team needed to input values to initialize each component in our model. The initial quantity of each species was obtained from RCT wetlab protocols:

Variable Species Initial Value Units
M miRNA 0.5 picomoles
P padlock probes 0.05 picomoles
SplR SplintR 25 molecules
T7poly T7 RNA polymerase 40 molecules
aptamer broccoli aptamer 0 molecules
fluorophore free fluorophores 180664245 molecules
aptfluorophore bound aptamer-fluorophores 0 molecules

Parameters

Rate constants and degradation rates are required to input into our Mass Action Laws and Michaelis-Menten equations. These values were derived from literature or estimated if the values could not be found. The value of each parameter is shown below:

Variable Reaction Estimated Values Units
Mdeg rate constant for miRNA degradation 0.000019254 1/second
k_padlock rate constant for miRNA-padlock binding 32000 1/(moles*second)
Vmcircular maximal rate of reaction needed for Michaelis-Menten enzyme kinetics for MP-SplintR binding 0.008 moles/second
Kmcircular Michaelis-Menten constant for MP-SplintR binding 1 mole
VmT7 maximal rate of reaction needed for Michaelis-Menten enzyme kinetics for MP_circular-T7 binding 14 mole/minute
KmT7 Michaelis-Menten constant for MP_circular-T7 binding 1.8 mole
aptdeg rate constant for aptamer degradation 0.004111193242 1/second
k_apt rate constant for the binding affinity of broccoli aptamers 89.92 1/mole*nanosecond

Ordinary Differential Equations

Lambert iGEM incorporated the Mass Action Kinetic Laws and Michaelis-Menten Equations to represent the reactions for the RCT model and generated 9 ODEs, as shown below:

Ordinary Differential Equations
\(\frac{d[M]}{dt} = -(k_{padlock}[M][P]) - (M_{deg}[M])\)
\(\frac{d[P]}{dt} = -(k_{padlock}[M][P])\)
\(\frac{d[SplR]}{dt} = -\frac{V_{mcircular}[MP]}{K_{mcircular}+[MP]}\)
\(\frac{d[MP]}{dt} = (k_{padlock}[M][P]) - (\frac{V_{m circular}[MP]}{K_{m circular}+[MP]})\)
\(\frac{d[MP_{circular}]}{dt} = (\frac{(V_{m circular}[MP]}{K_{m circular}+[MP])}-\frac{(V_{mT7}[MP_{circular}]}{K_{mT7}[MP_{circular}]})\)
\(\frac{d[T7_{poly}]}{dt} = -(\frac{V_{mT7}[MP_{circular}]}{K_{mT7}+[MP_{circular}]})\)
\(\frac{d[aptamer]}{dt} = -(apt_{deg}[aptamer])-(k_{fluorophore}[aptamer][fluorophore])+(\frac{V_{mT7}[MP_{circular}]}{K_{mT7}+[MP_{circular}]})\)
\(\frac{d[{aptfluorophore}]}{dt} = (k_{fluorophore}[aptamer][fluorophore])\)
\(\frac{d[fluorophore]}{dt} = -(k_{fluorophore}[aptamer][fluorophore])\)

Assumptions

All rate constants remain constant regardless of external environmental factors. Thus, this model simulates only the miRNA-padlock binding process to estimate aptamer production and aptamer-fluorophore binding. The total quantity of padlock probes, SplintR ligase, T7 RNA polymerase, and fluorophores is known and does not change over time. RNA polymerase activity also remains constant regardless of primers, miRNA, or NTP concentration.

Results

After developing a set of ODE equations, we utilized SimBiology’s Model Analyzer to simulate the number of bound aptamer-fluorophore complexes over 60 minutes with 0.5 picomoles of miRNA initially (see Fig. 15).

aptfluorophore MATLAB Graph
Figure 15. Simulation results of bound aptamer-fluorophores in molecules over 60 minutes

Initially, the concentration of aptamer-fluorophore complexes is relatively low. However, as the reaction progresses, the rate of aptamer-fluorophore production steadily increases and reaches a constant rate. Hypothetically, as the quantity of bound aptamer-fluorophore increases, the entire system dims increasingly, showing an inverse relationship. We currently lack adequate wetlab results for RCT to validate, adjust, and improve our model, but we will be able to use our ODE system to drive future experimentation with RCT.

Future Plans

In the future, we hope to gather further data to calibrate our parameters and fit our experimentation better. Furthermore, Lambert iGEM is currently planning to continue research next year. To prepare for future models, our team is planning to submit to an Institutional Review Board (IRB) to access deidentified data related to microRNAs (miRNAs) and coronary artery disease (CAD). An IRB will allow our team to legally handle and use data that would otherwise be protected information. By submitting an IRB application, a review board will look over the purpose and use of the data we are requesting and determine whether our project threatens the protection of the patients. We expect IRB approval since we seek deidentified data and our work does not threaten the privacy of human subjects. After clearance, our team hopes to develop a random-forest supervised machine learning model to assess the risk of patients for CAD based on medical, geographic, and socioeconomic parameters.

References

Chandler, M., Lyalina, T., Halman, J., Rackley, L., Lee, L., Dang, D., ... & Afonin, K. A. (2018). Broccoli fluorets: split aptamers as a user-friendly fluorescent toolkit for dynamic RNA nanotechnology. Molecules, 23(12), 3178. https://doi.org/10.3390/molecules23123178
Esteban, J. A., Salas, M., & Blanco, L. (1993). Fidelity of phi 29 DNA polymerase. Comparison between protein-primed initiation and DNA polymerization. Journal of Biological Chemistry, 268(4), 2719-2726. https://doi.org/10.1016/S0021-9258(18)53833-3
Graugnard, E., Cox, A., Lee, J., Jorcyk, C., Yurke, B., & Hughes, W. L. (2010). Kinetics of DNA and RNA hybridization in serum and serum-SDS. IEEE Transactions on Nanotechnology, 9(5), 603-609. https://doi.org/10.1109/TNANO.2010.2053380
Jin, J., Vaud, S., Zhelkovsky, A. M., Posfai, J., & McReynolds, L. A. (2016). Sensitive and specific miRNA detection method using SplintR Ligase. Nucleic Acids Research, 44(13), e116-e116. https://doi.org/10.1093/nar/gkw399
Lohman, G. J., Zhang, Y., Zhelkovsky, A. M., Cantor, E. J., & Evans Jr, T. C. (2013). Efficient DNA ligation in DNA–RNA hybrid helices by Chlorella virus DNA ligase. Nucleic Acids Research, 42(3), 1831-1844. https://doi.org/10.1093/nar/gkt1032
Macdonald, L. E., Durbin, R. K., Dunn, J. J., & McAllister, W. T. (1994). Characterization of two types of termination signal for bacteriophage T7 RNA polymerase. Journal of Molecular Biology, 238(2), 145-158. https://doi.org/10.1006/jmbi.1994.1277
Park, C. (2022). Visual interpretation of the meaning of k cat/KM in enzyme kinetics. Journal of Chemical Education, 99(7), 2556-2562. https://doi.org/10.1021/acs.jchemed.1c01268
Thevendran, R., Navien, T. N., Meng, X., Wen, K., Lin, Q., Sarah, S., ... & Citartan, M. (2020). Mathematical approaches in estimating aptamer-target binding affinity. Analytical Biochemistry, 600, 113742. https://doi.org/10.1016/j.ab.2020.113742
Zi, Z. (2012). A tutorial on mathematical modeling of biological signaling pathways. Computational Modeling of Signaling Networks, 41-51. https://doi.org/10.1007/978-1-61779-833-7_3