[go: up one dir, main page]

CN113125552B - A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces - Google Patents

A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces Download PDF

Info

Publication number
CN113125552B
CN113125552B CN202010027371.4A CN202010027371A CN113125552B CN 113125552 B CN113125552 B CN 113125552B CN 202010027371 A CN202010027371 A CN 202010027371A CN 113125552 B CN113125552 B CN 113125552B
Authority
CN
China
Prior art keywords
frequency
reaction
ligand
tested
constant
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN202010027371.4A
Other languages
Chinese (zh)
Other versions
CN113125552A (en
Inventor
王雪凤
许鹏程
于海涛
李昕欣
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shanghai Institute of Microsystem and Information Technology of CAS
Original Assignee
Shanghai Institute of Microsystem and Information Technology of CAS
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Institute of Microsystem and Information Technology of CAS filed Critical Shanghai Institute of Microsystem and Information Technology of CAS
Priority to CN202010027371.4A priority Critical patent/CN113125552B/en
Publication of CN113125552A publication Critical patent/CN113125552A/en
Application granted granted Critical
Publication of CN113125552B publication Critical patent/CN113125552B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/02Analysing fluids
    • G01N29/022Fluid sensors based on microsensors, e.g. quartz crystal-microbalance [QCM], surface acoustic wave [SAW] devices, tuning forks, cantilevers, flexural plate wave [FPW] devices
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/02Analysing fluids
    • G01N29/036Analysing fluids by measuring frequency or resonance of acoustic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N5/00Analysing materials by weighing, e.g. weighing small particles separated from a gas or liquid
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/01Indexing codes associated with the measuring variable
    • G01N2291/014Resonance or resonant frequency
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/02Indexing codes associated with the analysed material
    • G01N2291/024Mixtures
    • G01N2291/02416Solids in liquids

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Acoustics & Sound (AREA)
  • Investigating Or Analyzing Materials Using Thermal Means (AREA)
  • Measuring Or Testing Involving Enzymes Or Micro-Organisms (AREA)

Abstract

The invention discloses a method for measuring kinetic and thermodynamic parameters on a solid-liquid interface, which is characterized in that the kinetic and thermodynamic parameters (a binding/dissociation equilibrium constant K A/KD, gibbs free energy delta G DEG, surface coverage theta, a binding/dissociation rate constant K a/kd and a reaction activation energy E a) of a nucleic acid aptamer and a ligand thereof on the solid-liquid interface are obtained by analyzing and calculating the output frequency-time curve of a micro-cantilever sensor according to the frequency-time curve corresponding to ligand solutions with different concentrations to be measured and the frequency-time curve of ligand solutions with other concentrations to be measured at two different temperatures. The method overcomes the defects of expensive instruments, complicated operation, single parameter measurement and the like of the traditional method, has the advantages of high sensitivity, low cost, simple and quick operation, no need of marking and correction, capability of effectively avoiding systematic errors, one-time measurement of related parameters and the like, and is suitable for measuring dynamics and thermodynamic parameters of various nucleic acid aptamers and ligands thereof.

Description

Method for measuring dynamic and thermodynamic parameters on solid-liquid interface
Technical Field
The invention relates to the technical field of molecular dynamics/thermodynamics, in particular to a method for measuring dynamics and thermodynamic parameters of biochemical reaction on a solid-liquid interface.
Background
Nucleic acid aptamer (Nucleic ACID APTAMER) is an artificially synthesized RNA or DNA receptor molecule, and various target substances (small molecules, proteins and even cells) can be used as ligands. The nucleic acid aptamer has stable chemical property, is easy to synthesize, can be modified according to requirements, has high specificity and affinity for the ligand, and has become a common molecular recognition element in the development and application of biosensors.
When the biosensor is used for detecting an object to be detected in a solution, the occurrence place of the biosensor is a solid-liquid interface no matter the reaction occurs, the energy is transferred and the signal is converted. Therefore, the kinetics/thermodynamics of biochemical reaction on the solid-liquid interface can be quantitatively researched, the biosensing mechanism can be researched, the sensor performance can be perfected, the interface design and material optimization can be evaluated, and the design and the manufacture of the biosensor can be guided. While there is a lot of work to study the kinetics and thermodynamic behavior of aptamer and its ligand in solution, the diffusion layer on the solid-liquid interface and the steric effect of the capture probe will generate energy barriers, and the parameters obtained from the solution cannot describe the kinetics and thermodynamic behavior of biochemical reaction on the interface, while the kinetics and thermodynamic research methods on the solid-liquid interface are often limited by factors such as signal markers and temperature change range, so the development of biological interface sensing, especially the biological sensing system based on the reaction of aptamer and ligand, is highly needed to provide a method for rapidly measuring the kinetics and thermodynamic parameters of aptamer and ligand on the solid-liquid interface, so as to systematically study the kinetics and thermodynamic mechanism and physicochemical process on the solid-liquid interface.
In view of the foregoing, it is desirable to provide a method for determining kinetic and thermodynamic parameters at a solid-liquid interface to solve the above-mentioned problems.
Disclosure of Invention
In view of the limitations of the traditional method for measuring dynamic and thermodynamic parameters on an interface, the invention aims to provide a more direct, convenient and comprehensive method, which can directly and quickly obtain the required dynamic and thermodynamic parameters according to a frequency-time curve, and utilizes a micro-cantilever sensor as a detection platform to track the occurrence of a reaction on a solid-liquid interface in real time, so that a plurality of dynamic/thermodynamic parameters are extracted at one time, the modification or marking of an object to be measured is not needed, the mass sensitivity calibration is not needed, the measurement efficiency is improved, the measurement error is effectively avoided, and the measurement cost is reduced.
The invention is realized by the following technical scheme:
the invention provides a method for measuring dynamic and thermodynamic parameters on a solid-liquid interface, which comprises the following steps:
S100, providing a frequency-time curve diagram corresponding to each of a plurality of ligand solutions with different concentrations to be detected and a frequency-time curve diagram of another ligand solution with different concentrations to be detected at two different temperatures, wherein the ligand solutions with different concentrations to be detected at least comprise three ligand solutions with different concentrations to be detected;
S200, calculating to obtain dynamic and thermodynamic parameters on a solid-liquid interface according to frequency-time graphs corresponding to the ligand solutions with different concentrations to be detected, wherein the parameters at least comprise a binding equilibrium constant K A, a dissociation equilibrium constant K D, a Gibbs free energy delta G, a surface coverage theta, a binding rate constant K a and a dissociation rate constant K d;
s300, calculating to obtain the reaction activation energy E a according to a frequency-time curve diagram of the ligand solution with the other concentration to be detected at the two different temperatures.
Further, according to the frequency-time graphs corresponding to the ligand solutions with different concentrations to be detected, kinetic and thermodynamic parameters on the solid-liquid interface are calculated, wherein the parameters at least comprise a binding equilibrium constant K A, a dissociation equilibrium constant K D, a gibbs free energy Δg °, a surface coverage θ, a binding rate constant K a, and a dissociation rate constant K d, and the steps include:
S201, reading to obtain frequency change values delta f corresponding to the concentrations of the ligands to be detected according to the frequency-time graphs corresponding to the ligand solutions to be detected;
S202, calculating to obtain a reactive binding equilibrium constant K A according to frequency change values Deltaf corresponding to the concentrations of the multiple different ligands to be detected;
S203, calculating to obtain a dissociation equilibrium constant K D of the reaction according to the binding equilibrium constant K A of the reaction;
S204, calculating to obtain gibbs free energy delta G DEG of the reaction according to the binding equilibrium constant K A of the reaction;
S205, calculating to obtain surface coverage theta corresponding to the concentration of various ligands to be detected according to the binding equilibrium constant K A of the reaction;
s206, calculating to obtain a combination rate constant k a of the reaction according to the frequency-time curve graphs and the corresponding surface coverage theta corresponding to the ligand solutions with different concentrations to be detected;
S207, calculating to obtain a dissociation rate constant k d according to the combination rate constant k a of the reaction.
Further, the calculating the binding equilibrium constant K A according to the frequency change value Δf corresponding to the concentrations of the plurality of different ligands to be detected includes:
according to the frequency change value delta f corresponding to the concentration of the multiple different ligands to be detected, the method passes through the formula The binding equilibrium constant K A of the reaction was calculated.
Wherein [ L ] is the concentration of the ligand to be detected, and A is a constant reflecting the number of maximum reaction sites on the interface.
Further, the calculating the dissociation equilibrium constant K D of the reaction according to the binding equilibrium constant K A of the reaction includes:
The dissociation equilibrium constant K D for the reaction is calculated by equation K D=1/KA based on the binding equilibrium constant K A for the reaction.
Further, the calculating gibbs free energy Δg° of the reaction according to the binding equilibrium constant K A of the reaction includes:
The gibbs free energy Δg° of the reaction is calculated from the formula Δg° = -RTlnK A according to the binding equilibrium constant K A of the reaction.
Where R is the ideal gas constant, r= 8.314J/(mol·k), and T is the absolute temperature (K) at which the experiment was performed.
Further, the calculating the surface coverage θ corresponding to the concentrations of the plurality of different ligands to be detected according to the binding equilibrium constant K A of the reaction includes:
According to the binding equilibrium constant K A of the reaction, the reaction is carried out by the formula And calculating to obtain the surface coverage theta corresponding to the concentration of the various ligands to be detected.
Further, the calculating the binding rate constant k a according to the frequency-time graph and the corresponding surface coverage θ corresponding to each of the ligand solutions with different concentrations to be measured includes:
S2061, reading and obtaining the slope b of the frequency-time curve corresponding to the concentration of the ligand to be detected according to the frequency-time curve corresponding to the ligand solution to be detected;
s2062, according to the slope b of the frequency-time curve corresponding to the concentrations of the multiple different ligands to be detected, the frequency change value delta f corresponding to the concentrations of the multiple different ligands to be detected and the corresponding surface coverage theta, passing through the formula The binding rate constant k a of the reaction was calculated.
Further, the calculating the dissociation rate constant k d according to the binding rate constant k a of the reaction includes:
From the binding rate constant k a of the reaction, the dissociation rate constant k d is calculated by the formula k d=ka/KA.
Further, the two different temperatures include a first preset temperature T 1 and a second preset temperature T 2, and calculating, according to a frequency-time graph of another ligand solution to be measured at the two different temperatures, a reaction activation energy E a includes:
S301, obtaining a frequency-time curve slope b 1 at the first preset temperature T 1 and a frequency-time curve slope b 2 at the second preset temperature T 2 according to the frequency-time curve graph of the ligand solution with the other concentration to be detected at the two different temperatures;
S302, calculating to obtain an activation energy E a according to the first preset temperature T 1, the second preset temperature T 2, the frequency-time curve slope b 1 at the first preset temperature T 1 and the frequency-time curve slope b 2 at the second preset temperature T 2.
Further, the calculating the activation energy E a according to the first preset temperature T 1, the second preset temperature T 2, the frequency-time curve slope b 1 at the first preset temperature T 1, and the frequency-time curve slope b 2 at the second preset temperature T 2 includes:
According to the first preset temperature T 1, the second preset temperature T 2, the slope b 1 of the frequency-time curve at the first preset temperature T 1 and the slope b 2 of the frequency-time curve at the second preset temperature T 2, the method is as follows The activation energy E a was calculated.
Where R is the ideal gas constant, r= 8.314J/(mol·k).
The implementation of the invention has the following beneficial effects:
1. the method can directly and quickly obtain the required dynamics and thermodynamic parameters according to the frequency-time curve, and the determination method of the required data curve is simple, convenient and quick, does not need complex instrument operation, and can directly detect the ligand in the solution without marking the ligand based on the micro-weighing detection mode of the micro-cantilever sensor;
2. the method provided by the invention can extract a plurality of kinetic and thermodynamic parameters at one time according to the data acquired by one micro-cantilever sensor, so that systematic errors caused by a plurality of tests and a plurality of instruments are avoided;
3. The method provided by the invention does not need to calibrate the mass sensitivity of the micro-cantilever sensor, simplifies the experimental steps and improves the measurement efficiency;
4. The micro-cantilever sensor used in the invention has extremely high sensitivity, overcomes the limitation that other methods can only detect macromolecules, and is used for researching the interaction mechanism of small molecules with low molecular weight and the nucleic acid aptamer thereof on an interface.
Drawings
In order to more clearly illustrate the embodiments of the invention or the technical solutions and advantages of the prior art, the following description will briefly explain the drawings used in the embodiments or the description of the prior art, and it is obvious that the drawings in the following description are only some embodiments of the invention, and other drawings can be obtained according to the drawings without inventive effort for a person skilled in the art.
FIG. 1 is a flow chart of a method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to an embodiment of the present invention.
Fig. 2 is a flowchart of step S200 provided in an embodiment of the present invention.
Fig. 3 is a flowchart of step S300 provided in an embodiment of the present invention.
Fig. 4 is a schematic diagram of a detection system based on a micro-cantilever sensor according to an embodiment of the present invention.
FIG. 5 shows frequency-time curves obtained from the reaction of Adenosine Triphosphate (ATP) and its aptamer at the solid-liquid interface at different ATP concentrations [ L ] at the same temperature.
FIG. 6 is a graph of [ L ]/[ delta ] f [ L ] for calculating the binding/dissociation equilibrium constant K A/KD, the Gibbs free energy ΔG DEG using the data obtained in FIG. 5, according to an example of the present invention.
FIG. 7 is a graph of b- [ L ]. DELTA.f/θ for calculating a surface coverage θ, a binding rate constant k a, and a dissociation rate constant k d using the data obtained in FIG. 5, provided by an embodiment of the present invention.
FIG. 8 is a graph showing the frequency versus time for the measurement of the same ATP concentration at different temperatures, respectively, in accordance with an embodiment of the present invention.
The reference numerals correspond to 1-buffer solution, 2-ligand solution, 3-sample injection valve, 4-reaction cavity, 41-sample injection port, 42-sample outlet, 5-detection cavity, 6-micro cantilever beam chip, 7-temperature control device, 8-constant pressure pump, 9-waste liquid outlet, 10-computer and 11-data collector.
Detailed Description
The present invention will be described in further detail with reference to examples for the purpose of making the objects, technical solutions and advantages of the present invention more apparent. It will be apparent that the described embodiments are only some, but not all, embodiments of the invention. All other embodiments, which can be made by those skilled in the art based on the embodiments of the invention without making any inventive effort, are intended to be within the scope of the invention.
The invention provides a method for measuring dynamic and thermodynamic parameters on a solid-liquid interface, referring to fig. 1 to 8, the method for measuring the dynamic and thermodynamic parameters on the solid-liquid interface comprises the following steps:
S100, providing a frequency-time curve diagram corresponding to each of a plurality of ligand solutions with different concentrations to be detected and a frequency-time curve diagram of another ligand solution with different concentrations to be detected at two different temperatures, wherein the ligand solutions with different concentrations to be detected at least comprise three ligand solutions with different concentrations to be detected;
S200, calculating to obtain dynamic and thermodynamic parameters on a solid-liquid interface according to frequency-time graphs corresponding to the ligand solutions with different concentrations to be detected, wherein the parameters at least comprise a binding equilibrium constant K A, a dissociation equilibrium constant K D, a Gibbs free energy delta G, a surface coverage theta, a binding rate constant K a and a dissociation rate constant K d;
s300, calculating to obtain the reaction activation energy E a according to a frequency-time curve diagram of the ligand solution with the other concentration to be detected at the two different temperatures.
Further, according to the frequency-time graphs corresponding to the ligand solutions with different concentrations to be detected, kinetic and thermodynamic parameters on the solid-liquid interface are calculated, wherein the parameters at least comprise a binding equilibrium constant K A, a dissociation equilibrium constant K D, a gibbs free energy Δg °, a surface coverage θ, a binding rate constant K a, and a dissociation rate constant K d, and the steps include:
S201, reading to obtain frequency change values delta f corresponding to the concentrations of the ligands to be detected according to the frequency-time graphs corresponding to the ligand solutions to be detected;
S202, calculating to obtain a reactive binding equilibrium constant K A according to frequency change values Deltaf corresponding to the concentrations of the multiple different ligands to be detected;
S203, calculating to obtain a dissociation equilibrium constant K D of the reaction according to the binding equilibrium constant K A of the reaction;
S204, calculating to obtain gibbs free energy delta G DEG of the reaction according to the binding equilibrium constant K A of the reaction;
S205, calculating to obtain surface coverage theta corresponding to the concentration of various ligands to be detected according to the binding equilibrium constant K A of the reaction;
s206, calculating to obtain a combination rate constant k a of the reaction according to the frequency-time curve graphs and the corresponding surface coverage theta corresponding to the ligand solutions with different concentrations to be detected;
S207, calculating to obtain a dissociation rate constant k d according to the combination rate constant k a of the reaction.
As shown in fig. 2, the calculating the binding equilibrium constant K A according to the frequency change value Δf corresponding to the concentrations of the plurality of different ligands to be detected includes:
according to the frequency change value delta f corresponding to the concentration of the multiple different ligands to be detected, the method passes through the formula The binding equilibrium constant K A of the reaction was calculated. Wherein [ L ] is the concentration of the ligand to be detected, and A is a constant reflecting the number of maximum reaction sites on the interface.
The calculating the dissociation equilibrium constant K D of the reaction according to the binding equilibrium constant K A of the reaction includes:
The dissociation equilibrium constant K D for the reaction is calculated by equation K D=1/KA based on the binding equilibrium constant K A for the reaction.
The calculation of the Gibbs free energy ΔG DEG of the reaction according to the binding equilibrium constant K A of the reaction comprises:
The gibbs free energy Δg° of the reaction is calculated from the formula Δg° = -RTlnK A according to the binding equilibrium constant K A of the reaction.
Where R is the ideal gas constant, r= 8.314J/(mol·k), and T is the absolute temperature (K) at which the experiment was performed.
The calculating the surface coverage theta corresponding to the concentration of the ligands to be detected according to the binding equilibrium constant K A of the reaction comprises the following steps:
According to the binding equilibrium constant K A of the reaction, the reaction is carried out by the formula And calculating to obtain the surface coverage theta corresponding to the concentration of the various ligands to be detected.
The calculating a binding rate constant k a of the reaction according to the frequency-time curve graphs corresponding to the ligand solutions with different concentrations to be detected respectively comprises:
S2061, reading and obtaining the slope b of the frequency-time curve corresponding to the concentration of the ligand to be detected according to the frequency-time curve corresponding to the ligand solution to be detected;
s2062, according to the slope b of the frequency-time curve corresponding to the concentrations of the multiple different ligands to be detected, the frequency change value delta f corresponding to the concentrations of the multiple different ligands to be detected and the corresponding surface coverage theta, passing through the formula The binding rate constant k a of the reaction was calculated.
The calculating the dissociation rate constant k d according to the binding rate constant k a of the reaction includes:
From the binding rate constant k a of the reaction, the dissociation rate constant k d is calculated by the formula k d=ka/KA.
As shown in fig. 3, the two different temperatures include a first preset temperature T 1 and a second preset temperature T 2,
The calculating reaction activation energy E a according to the frequency-time curve graph of the ligand solution with the other concentration to be measured at the two different temperatures comprises:
S301, obtaining a frequency-time curve slope b 1 at the first preset temperature T 1 and a frequency-time curve slope b 2 at the second preset temperature T 2 according to the frequency-time curve graph of the ligand solution with the other concentration to be detected at the two different temperatures;
S302, calculating to obtain an activation energy E a according to the first preset temperature T 1, the second preset temperature T 2, the frequency-time curve slope b 1 at the first preset temperature T 1 and the frequency-time curve slope b 2 at the second preset temperature T 2.
Further, the calculating the activation energy E a according to the first preset temperature T 1, the second preset temperature T 2, the frequency-time curve slope b 1 at the first preset temperature T 1, and the frequency-time curve slope b 2 at the second preset temperature T 2 includes:
According to the first preset temperature T 1, the second preset temperature T 2, the slope b 1 of the frequency-time curve at the first preset temperature T 1 and the slope b 2 of the frequency-time curve at the second preset temperature T 2, the method is as follows The activation energy E a was calculated. Where R is the ideal gas constant, r= 8.314J/(mol·k).
As shown in fig. 4 to 8, a method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to the present invention specifically comprises:
1) An amino-modified aptamer (sequence 5'-ACCTGGGGGAGTATTGCGGAGGAAGGTTTT-NH 2 -3') was conjugated to polydopamine microspheres.
2) Uploading to the detection area of the micro-cantilever chip by a micro-printer.
3) The micro-cantilever beam chip is put into a detection system for sealing treatment, and the micro-cantilever beam sensor has the advantages of low cost, small volume and good repeatability by adopting a detection chip based on the micro-cantilever beam technology, can directly detect the ligand in the solution without marking the ligand, and outputs continuous signals in real time so as to realize complete tracking of the reaction process.
4) As shown in fig. 4, the sample channel of the sample valve 3 is turned into the buffer solution 1, the constant pressure pump 8 is started, the system becomes negative pressure, the buffer solution fills the detection cavity 5 through the sample inlet 41, flows out from the sample outlet 42, and finally is discharged through the waste liquid outlet 9. And applying negative pressure at the tail end of the sampling pipe by using a constant pressure pump, so that the buffer solution flows into a main flow channel of the reaction cavity. The gas residue in the system is reduced by utilizing a negative pressure sample injection mode, and the sample injection is rapid.
5) The method comprises the steps of recording signals acquired by a data acquisition unit in real time by a computer, observing the reaction progress through the signals, namely adding ATP solution (dissolved in a binding buffer solution) with a certain concentration (L 1) into a system after resonance frequency is stable, recording a frequency-time curve and frequency change Deltaf 1, adding dissociation solution into the system after frequency is stable, carrying out interface regeneration, detecting the addition of other two concentration systems (L 2 and L 3) by the same method after the frequency is restored to an initial baseline level, and respectively obtaining the frequency-time curve and frequency change (Deltaf 2 and Deltaf 3) under the two concentrations, as shown in figure 5. The frequency-time curve graph corresponding to the ligand solution to be measured is obtained by sequentially adding the ligand solution to be measured, the measuring method is simple, convenient and quick, complex instrument operation is not needed, sample injection is only needed after the output frequency is stable, multiple groups of experimental data are extracted at one time by using one micro-cantilever sensor, and system errors caused by multiple experiments and multiple instruments are avoided.
6) As shown in FIG. 6, the frequency change Δf corresponding to the different ligand concentrations [ L ] in FIG. 5 is read and is taken into the formulaThe binding equilibrium constant K A=7.42ⅹ10-3M-1 is obtained by [ L ]/Δf=2.85x10 -3[L]+3.85ⅹ10-9.
7) The resulting K A was taken into the formula K D=1/KA and the dissociation equilibrium constant K D =1.3 μm was calculated.
8) Bringing the obtained K A into the formula DeltaG DEG= -RTlnK A, calculating the Gibbs free energy DeltaG DEG= -33.5kJ/mol.
9) Bringing the resulting K A into the formulaThe surface coverage θ at each ATP concentration [ L ] was calculated.
10 In FIG. 5, the slope b of the frequency-time curve after addition of the different ligand concentrations [ L ] to the system is read, combined with the frequency variation Δf and the surface coverage θ, and brought into the formulaIn (1) to obtainI.e. k a=660M-1s-1.
11 The resulting k a is taken into the formula k d=ka/KA and the dissociation rate constant k d,kd=0.00089s-1 is calculated as shown in fig. 7.
12 As shown in fig. 8, under different conditions of T 1 (299K) and T 2 (293K), ATP solutions of the same concentration l=1μm were added to the system, and the slopes b 1 and b 2 were read, respectively, and were brought into the formulaThe activation energy E a =38.0 kJ/mol was calculated.
The embodiment of the invention has the following beneficial effects:
1. the method can directly and quickly obtain the required dynamics and thermodynamic parameters according to the frequency-time curve, and the determination method of the required data curve is simple, convenient and quick, does not need complex instrument operation, and can directly detect the ligand in the solution without marking the ligand based on the micro-weighing detection mode of the micro-cantilever sensor;
2. the method provided by the invention can extract a plurality of kinetic and thermodynamic parameters at one time according to the data acquired by one micro-cantilever sensor, so that systematic errors caused by a plurality of tests and a plurality of instruments are avoided;
3. The method provided by the invention does not need to calibrate the mass sensitivity of the micro-cantilever sensor, simplifies the experimental steps and improves the measurement efficiency;
4. The micro-cantilever sensor used in the invention has extremely high sensitivity, overcomes the limitation that other methods can only detect macromolecules, and is used for researching the interaction mechanism of small molecules with low molecular weight and the nucleic acid aptamer thereof on an interface.
While the invention has been described with respect to preferred embodiments thereof, it will be understood by those skilled in the art that various modifications and additions may be made without departing from the scope of the invention. Those skilled in the art will appreciate that many modifications, adaptations and variations of the present invention can be made using the techniques disclosed herein without departing from the spirit and scope of the invention, and that many modifications, adaptations and variations of the present invention are within the scope of the invention as defined by the appended claims.

Claims (10)

1.一种测定固液界面上动力学及热力学参数的方法,其特征在于,包括以下步骤:1. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface, characterized in that it comprises the following steps: S100.提供多种不同待测浓度配体溶液各自对应的频率-时间曲线图和两种不同温度下另一待测浓度的配体溶液的频率-时间曲线图,所述多种不同待测浓度的配体溶液至少为三种不同待测浓度的配体溶液;S100. Provide a frequency-time graph corresponding to each of a plurality of ligand solutions of different concentrations to be tested and a frequency-time graph of another ligand solution of a concentration to be tested at two different temperatures, wherein the plurality of ligand solutions of different concentrations to be tested are at least three ligand solutions of different concentrations to be tested; S200.根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图,计算得到固液界面上动力学及热力学参数,所述参数至少包括结合平衡常数KA、解离平衡常数KD、吉布斯自由能△G°、表面覆盖度θ、结合速率常数ka和解离速率常数kdS200. Calculating the kinetic and thermodynamic parameters at the solid-liquid interface according to the frequency-time curves corresponding to the plurality of ligand solutions of different concentrations to be tested, wherein the parameters at least include the binding equilibrium constant KA , the dissociation equilibrium constant KD , the Gibbs free energy △G°, the surface coverage θ, the binding rate constant ka and the dissociation rate constant kd ; S300.根据所述两种不同温度下另一待测浓度的配体溶液的频率-时间曲线图,计算得到反应活化能EaS300. Calculate the reaction activation energy E a according to the frequency-time curve of another ligand solution of the concentration to be tested at the two different temperatures; 所述频率-时间曲线图包括以下方式获取:The frequency-time curve diagram includes the following acquisition methods: 将微悬臂梁芯片放入检测系统中并进行密封处理;微悬臂梁传感器采用微称重检测模式;The micro-cantilever chip is placed in the detection system and sealed; the micro-cantilever sensor adopts a micro-weighing detection mode; 将进样阀的进样通道转入缓冲液中,开启恒压泵,系统变为负压,缓冲液通过进样口,将检测腔体充满,再从出样口流出,最终通过废液口排出;The injection channel of the injection valve is transferred into the buffer solution, and the constant pressure pump is turned on. The system becomes negative pressure, and the buffer solution passes through the injection port, fills the detection cavity, and then flows out from the outlet, and finally discharged through the waste liquid port; 实时记录数据采集器采集到的信号;Record the signals collected by the data collector in real time; 当谐振频率稳定后,向体系中加入[L]1浓度的ATP溶液,记录频率-时间曲线及频率变化;待频率稳定后,向体系加入解离溶液,界面再生;待频率恢复到初始基线水平后,用同样的方法检测[L]2和[L]3的两个浓度体系,分别得到[L]2浓度和[L]3浓度下的频率-时间曲线和频率变化。When the resonant frequency stabilizes, ATP solution with a concentration of [L] 1 is added to the system, and the frequency-time curve and frequency change are recorded; after the frequency stabilizes, dissociation solution is added to the system to regenerate the interface; after the frequency returns to the initial baseline level, the two concentration systems of [L] 2 and [L] 3 are detected using the same method, and the frequency-time curves and frequency changes at [L] 2 and [L] 3 concentrations are obtained, respectively. 2.根据权利要求1所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图,计算得到固液界面上动力学及热力学参数,所述参数至少包括结合平衡常数KA、解离平衡常数KD、吉布斯自由能△G°、表面覆盖度θ、结合速率常数ka和解离速率常数kd包括:2. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 1, characterized in that the kinetic and thermodynamic parameters at the solid-liquid interface are calculated based on the frequency-time curves corresponding to the plurality of ligand solutions with different concentrations to be tested, and the parameters at least include binding equilibrium constant KA , dissociation equilibrium constant KD , Gibbs free energy △G°, surface coverage θ, binding rate constant ka and dissociation rate constant kd, including: S201.根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图,读取得到多种不同待测配体浓度对应的频率变化值△f;S201. Reading frequency change values △f corresponding to the various different concentrations of the ligand to be tested according to the frequency-time curves corresponding to the various different concentrations of the ligand to be tested; S202.根据所述多种不同待测配体浓度对应的频率变化值△f,计算得到反应的结合平衡常数KAS202. Calculate the binding equilibrium constant K A of the reaction according to the frequency change values △f corresponding to the various concentrations of the ligands to be tested; S203.根据所述反应的结合平衡常数KA,计算得到反应的解离平衡常数KDS203. Calculate the dissociation equilibrium constant K D of the reaction according to the binding equilibrium constant K A of the reaction; S204.根据所述反应的结合平衡常数KA,计算得到反应的吉布斯自由能△G°;S204. Calculate the Gibbs free energy ΔG° of the reaction according to the binding equilibrium constant KA of the reaction; S205.根据所述反应的结合平衡常数KA,计算得到多种不同待测配体浓度对应的表面覆盖度θ;S205. Calculating the surface coverage θ corresponding to various different concentrations of the ligand to be tested according to the binding equilibrium constant KA of the reaction; S206.根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图和对应的表面覆盖度θ,计算得到反应的结合速率常数kaS206. Calculate the binding rate constant ka of the reaction according to the frequency-time curves and the corresponding surface coverage θ corresponding to the plurality of ligand solutions with different concentrations to be tested; S207.根据所述反应的结合速率常数ka,计算得到解离速率常数kdS207. Calculate the dissociation rate constant k d according to the association rate constant ka of the reaction. 3.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述多种不同待测配体浓度对应的频率变化值△f,计算得到反应的结合平衡常数KA包括:3. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the binding equilibrium constant KA of the reaction is calculated based on the frequency change values Δf corresponding to the multiple different concentrations of the ligand to be tested, comprising: 根据所述多种不同待测配体浓度对应的频率变化值△f,通过公式计算得到反应的结合平衡常数KAAccording to the frequency change values △f corresponding to the various concentrations of the ligands to be tested, the formula Calculate the binding equilibrium constant KA of the reaction; 其中,[L]为待测配体浓度,A为反映界面上最大反应位点数的常数。Where [L] is the concentration of the ligand to be tested, and A is a constant reflecting the maximum number of reactive sites on the interface. 4.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述反应的结合平衡常数KA,计算得到反应的解离平衡常数KD包括:4. The method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the step of calculating the dissociation equilibrium constant K D of the reaction based on the binding equilibrium constant KA of the reaction comprises: 根据所述反应的结合平衡常数KA,通过公式KD=1/KA计算得到反应的解离平衡常数KDAccording to the binding equilibrium constant KA of the reaction, the dissociation equilibrium constant KD of the reaction is calculated by the formula KD = 1/ KA . 5.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述反应的结合平衡常数KA,计算得到反应的吉布斯自由能△G°包括:5. The method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the Gibbs free energy ΔG° of the reaction is calculated based on the binding equilibrium constant KA of the reaction, comprising: 根据所述反应的结合平衡常数KA,通过公式△G°=-RTlnKA计算得到反应的吉布斯自由能△G°;According to the binding equilibrium constant K A of the reaction, the Gibbs free energy ΔG° of the reaction is calculated by the formula ΔG°=-RTlnKA ; 其中,R为理想气体常数,R=8.314J/(mol·K) ,T为实验进行的绝对温度(K)。Where R is the ideal gas constant, R=8.314J/(mol·K), and T is the absolute temperature (K) at which the experiment is conducted. 6.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述反应的结合平衡常数KA,计算得到多种不同待测配体浓度对应的表面覆盖度θ包括:6. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the surface coverage θ corresponding to a plurality of different concentrations of the ligand to be tested is calculated based on the binding equilibrium constant KA of the reaction and comprises: 根据所述反应的结合平衡常数KA,通过公式计算得到多种不同待测配体浓度对应的表面覆盖度θ。According to the binding equilibrium constant KA of the reaction, The surface coverage θ corresponding to various different concentrations of the ligand to be tested was calculated. 7.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图和对应的表面覆盖度θ,计算得到反应的结合速率常数ka包括:7. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the binding rate constant ka of the reaction is calculated based on the frequency-time curves and the corresponding surface coverage θ corresponding to the plurality of ligand solutions with different concentrations to be tested, comprising: S2061.根据所述多种不同待测浓度配体溶液各自对应的频率-时间曲线图,读取得到多种不同待测配体浓度对应的频率-时间曲线斜率b;S2061. According to the frequency-time curves corresponding to the various ligand solutions with different concentrations to be tested, the slopes b of the frequency-time curves corresponding to the various ligand solutions with different concentrations to be tested are read; S2062.根据所述多种不同待测配体浓度对应的频率-时间曲线斜率b、所述多种不同待测配体浓度对应的频率变化值△f和对应的表面覆盖度θ,通过公式计算得到反应的结合速率常数kaS2062. According to the frequency-time curve slope b corresponding to the plurality of different ligand concentrations to be tested, the frequency change value △f corresponding to the plurality of different ligand concentrations to be tested and the corresponding surface coverage θ, the formula The association rate constant ka of the reaction was calculated. 8.根据权利要求2所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述反应的结合速率常数ka,计算得到解离速率常数kd包括:8. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 2, characterized in that the dissociation rate constant kd is calculated based on the association rate constant ka of the reaction, comprising: 根据所述反应的结合速率常数ka,通过公式kd=ka/KA计算得到解离速率常数kdAccording to the association rate constant ka of the reaction, the dissociation rate constant kd is calculated by the formula kd = ka / KA . 9.根据权利要求1所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述两种不同温度包括第一预设温度T1和第二预设温度T29. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 1, characterized in that the two different temperatures include a first preset temperature T1 and a second preset temperature T2 , 所述根据所述两种不同温度下另一待测浓度的配体溶液的频率-时间曲线图,计算得到反应活化能Ea包括:The step of calculating the reaction activation energy Ea according to the frequency-time curve of another ligand solution of the concentration to be tested at the two different temperatures comprises: S301.根据所述两种不同温度下另一待测浓度的配体溶液的频率-时间曲线图,得到所述第一预设温度T1下的频率-时间曲线斜率b1和所述第二预设温度T2下的频率-时间曲线斜率b2S301. According to the frequency-time curves of another ligand solution of the concentration to be tested at the two different temperatures, obtain the slope b1 of the frequency-time curve at the first preset temperature T1 and the slope b2 of the frequency-time curve at the second preset temperature T2 ; S302.根据所述第一预设温度T1、所述第二预设温度T2、所述第一预设温度T1下的频率-时间曲线斜率b1和所述第二预设温度T2下的频率-时间曲线斜率b2,计算得到活化能EaS302. Calculate activation energy E a according to the first preset temperature T 1 , the second preset temperature T 2 , the slope b 1 of the frequency-time curve at the first preset temperature T 1 , and the slope b 2 of the frequency-time curve at the second preset temperature T 2 . 10.根据权利要求9所述的一种测定固液界面上动力学及热力学参数的方法,其特征在于,所述根据所述第一预设温度T1、所述第二预设温度T2、所述第一预设温度T1下的频率-时间曲线斜率b1和所述第二预设温度T2下的频率-时间曲线斜率b2,计算得到活化能Ea包括:10. A method for determining kinetic and thermodynamic parameters at a solid-liquid interface according to claim 9, characterized in that the activation energy Ea is calculated based on the first preset temperature T1 , the second preset temperature T2 , the slope b1 of the frequency-time curve at the first preset temperature T1 , and the slope b2 of the frequency-time curve at the second preset temperature T2 , comprising: 根据所述第一预设温度T1、所述第二预设温度T2、所述第一预设温度T1下的频率-时间曲线斜率b1和所述第二预设温度T2下的频率-时间曲线斜率b2,通过公式计算得到活化能EaAccording to the first preset temperature T 1 , the second preset temperature T 2 , the slope b 1 of the frequency-time curve at the first preset temperature T 1 , and the slope b 2 of the frequency-time curve at the second preset temperature T 2 , the formula The activation energy E a is calculated; 其中,R为理想气体常数,R=8.314J/(mol·K)。Where R is the ideal gas constant, R=8.314J/(mol·K).
CN202010027371.4A 2020-01-10 2020-01-10 A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces Active CN113125552B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010027371.4A CN113125552B (en) 2020-01-10 2020-01-10 A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010027371.4A CN113125552B (en) 2020-01-10 2020-01-10 A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces

Publications (2)

Publication Number Publication Date
CN113125552A CN113125552A (en) 2021-07-16
CN113125552B true CN113125552B (en) 2025-03-25

Family

ID=76770890

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010027371.4A Active CN113125552B (en) 2020-01-10 2020-01-10 A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces

Country Status (1)

Country Link
CN (1) CN113125552B (en)

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102008044506A1 (en) * 2008-09-09 2010-03-11 Kinomics Gmbh Determination of equilibrium constants in solution using multi-step kinetics
TWI472740B (en) * 2011-11-14 2015-02-11 Nat Univ Chung Cheng Method for obtaining binding kinetic rate constants using fiber optics particle plasmon resonance (foppr) sensor
EP2783018B1 (en) * 2011-11-23 2016-09-07 The Governing Council Of The University Of Toronto Versatile and sensitive biosensor
CN104897508B (en) * 2014-03-06 2018-09-28 中国科学院上海微系统与信息技术研究所 A method for testing thermodynamic parameters of functional materials
CN105891041A (en) * 2016-04-08 2016-08-24 中国科学院上海微系统与信息技术研究所 A test method for the performance of CO2 sensing materials
CN106442679B (en) * 2016-09-20 2018-10-26 德州学院 Combined between a kind of detection molecules can and binding kinetics sensing device and method
CN110376356B (en) * 2019-07-25 2021-06-29 吉林大学 A method for rapid determination of mineral flotation thermodynamics and process kinetic parameters

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
IN-PLANE MODE RESONANT CANTILEVER SENSOR TO DETECT KINETIC/THERMODYNAMIC PARAMETERS FOR APTAMER-LIGAND BINDING;Xuefeng Wang 等;IEEE MEMS 2020, Vancouver, CANADA;20200122;全文 *
Resonant-Cantilever Detected Kinetic/Thermodynamic Parameters for Aptamer-Ligand Binding on Liquid-Solid Interface;Xuefeng Wang 等;analytical chemistry;20200617;全文 *

Also Published As

Publication number Publication date
CN113125552A (en) 2021-07-16

Similar Documents

Publication Publication Date Title
Liu et al. Trends in miniaturized biosensors for point-of-care testing
Bakhshpour et al. Quartz crystal microbalance biosensor for label-free MDA MB 231 cancer cell detection via notch-4 receptor
Piletsky et al. Molecularly imprinted polymers in clinical diagnostics—Future potential and existing problems
Hu et al. Four aspects about solid‐state nanopores for protein sensing: fabrication, sensitivity, selectivity, and durability
KR100583233B1 (en) Biomaterial Measurement System and Method
CN102519912B (en) Method for detecting object to be detected by using surface plasmon resonance (SPR) biosensor
JP5855246B2 (en) Determination of active concentration by calibration-free analysis
Zhang et al. Sensitive detection of carcinoembryonic antigen in exhaled breath condensate using surface acoustic wave immunosensor
CN107085022B (en) Preparation and Application of Molecularly Imprinted Electrochemical Sensor of 3-Nitrotyrosine
Zhang et al. A miniaturized photoacoustic device with laptop readout for point-of-care testing of blood glucose
CN103543081A (en) Portable sensing system for early diagnosing liver cancer and functional modification method of portable sensing system
Anand et al. Detecting glycated hemoglobin in human blood samples using a transistor-based nanoelectronic aptasensor
Chen et al. Application of displacement principle for detecting heavy metal ions and EDTA using microcantilevers
Chen et al. Proximity hybridization-induced competitive rolling circle amplification to construct fluorescent dual-sensor for simultaneous evaluation of glycated and total hemoglobin
Yu et al. Nanopore electrochemical measurement for single molecular interactions and beyond
CN113125552B (en) A method for determining kinetic and thermodynamic parameters at solid-liquid interfaces
Erdoğan et al. Preparation of concanavalin a imprinted surface plasmon resonance based biosensors
CN107543814B (en) A kind of biological sensing system based on 45 ° of double drive symmetrical structure bullet light modulations
CN100362337C (en) Optical fiber surface plasmon wave nucleic acid sensor system and detection method for detecting single nucleotide polymorphism
Phansi et al. Kinetic thermometric methods in analytical chemistry
Ranjbari et al. The role of electrochemical biosensors in monitoring Apolipoprotein B-100 as a diagnostic tool for cardiovascular disease
Yang et al. A micro-pressure sensor-based analytic platform and its application in thrombin quantification
Rashid All Molecular-Based Electrochemical Biosensors Depend on a Highly Specific System for Detecting or Tracking the Target Molecule
Altintas Molecular imprinting technology in advanced biosensors for diagnostics
Weiss et al. Chip-based scanning nano-calorimeter for protein stability analysis in biosensor membranes

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant