Published: Vol 8, Iss 15, Aug 5, 2018 DOI: 10.21769/BioProtoc.2957 Views: 22194
Reviewed by: Shyam SolankiTimothy S. ArtlipAnonymous reviewer(s)
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Abstract
This protocol can be applied to analyze the direct interaction between a soluble protein and a target ligand molecule using Isothermal Titration Calorimetry (ITC, Malvern). ITC allows the biophysical characterization of binding between label-free, non-immobilized and in-solution biomolecules by providing the stoichiometry of the interaction, the equilibrium binding constants and the thermodynamic parameters. ITC monitors heat changes (released and/or absorbed) caused by macromolecular interactions with no restrictions of buffer and molecular weight of the macromolecules.
Keywords: ITCBackground
Macromolecular interactions are critical cellular events as they form the basis for signal transduction pathways. Thus, macromolecular interactions are an essential field of research, as they allow a deeper understanding of the molecular mechanisms which underlie both physiological and pathophysiological processes, and the rational design of drugs able to modulate disease-causing macromolecular binding events.
In this context, Isothermal Titration Calorimetry (ITC) is a powerful technique for the characterization of macromolecular interactions. ITC determines the heat change that occurs upon the binding of two molecules. Heat can be absorbed (endothermic reaction) or released (exothermic reaction). ITC monitors such heat changes by determining the differential power, provided by heaters of the instrument to both the reference and the sample cells, needed for counteracting any temperature difference between the two cells during the binding reaction such that no difference in temperature arises between the reference and sample cells (Figure 1).
Figure 1. Principle of Isothermal Titration Calorimetry (ITC). A. Cartoon representation of an isothermal titration calorimetry instrument composed of: a reference cell filled with MilliQ water; a sample cell containing a biomolecule; and an automated injection syringe containing the other binding molecule (ligand) used to titrate the ligand into the sample cell. The sample and reference cells are surrounded by an adiabatic jacket. The system is able to detect temperature differences between the reference and sample cells and to maintain an absence of temperature difference between them (ΔT = 0) by supplying power to both the reference and the sample cell via two heaters. The output of the instrument is the power (μcal/sec) required to maintain ΔT = 0 between the reference and sample cells. B-D. The temperature difference between the reference and the sample cell, induced by the ligand–biomolecule binding, is converted into the power needed to bring the two cells back to the same temperature during the binding reaction. As the titration proceeds, the biomolecule in the sample cell becomes saturated with the ligand, so that less interactions occur and consequently the heat change decreases (C) until the biomolecule is fully saturated and the instrument detects only heat change due to the dilution of the ligand (D).
ITC provides important information about the nature of the macromolecular interaction: the binding stoichiometry (N); the thermodynamic parameters of the binding reaction (enthalpy, ∆H, entropy, ∆S, and Gibbs free energy, ∆G); the strength of the interaction (the equilibrium association constant KA, from which the more commonly used equilibrium dissociation constant KD can be derived).
Among the methods used to characterize macromolecular interactions, ITC has two major advantages: i) the biomolecules are free to move in solution and are not labelled, which insures a direct characterization of the binding event, unbiased by labelling and/or by limitation on molecule motions due to their immobilization on a surface; ii) ITC is the only method that allows a detailed characterization of the binding event by providing not only the binding affinity, but also other critical information, i.e., the binding stoichiometry and the thermodynamic parameters. This information can help significantly in the understanding of the molecular mechanism of the binding reaction, even when no structural data are yet available. Furthermore, they can be used as complementary data to validate structural results.
Recently, I presented crystallographic and functional data showing that the K+ inward rectifier KAT1 (K+ Arabidopsis thaliana 1) channel is regulated by the direct binding of 14-3-3 proteins (Saponaro et al., 2017). In particular, I identified a 14-3-3 mode III binding site at the very C-terminus of KAT1 and co-crystallized it with tobacco 14-3-3 proteins (14-3-3c) to describe the protein complex in atomic detail. The structural results were complemented/supported by measuring, through ITC, the interaction between a synthetic KAT1 C-terminal phosphopeptide (CPP) and 14-3-3c. ITC was employed to quantify the stoichiometry, the equilibrium binding affinity and the thermodynamic parameters of the 14-3-3c-CPP binding reaction.
The aim of this protocol is to provide a detailed description of the setting procedure of an ITC experiment, highlighting the crucial steps and related concerns, and providing, at the same time, a well-established strategy to overcome such problems. Moreover, the present protocol describes the analysis of an ITC measurement of the single binding event in a 14-3-3c/CPP interaction.
Materials and Reagents
Equipment
Software
Procedure
Data analysis
Calorimetric data were analysed with Origin software (version7, MicroCal, RRID:SCR_014212) and equations were described for the single-site binding model (Wiseman et al., 1989). It is worth noting that the procedure generally follows the “Instrument Handbook” of MicroCal VP-ITC system (Malvern Instruments Ltd).
Figure 2. ITC measurement of CPP–14-3-3c interaction. A. Raw ITC data of CPP (500 μM) binding to 14-3-3c (50 μM). The area of the negative heat changes (μcal/sec) during successive injections of 10 μl of CPP into the sample cell containing 14-3-3c was calculated by selecting the option “integrate all peaks” from the ITC main control list in order to measure the amount of heat released by each CPP injection of the titration. The area of the peaks is colored in red. B. The quantified heat changes (red filled circles), normalized per mole of CPP injected and plotted against the molar ratio of CPP : 14-3-3c, were fitted to a single-site binding model by selecting the option “One set of sites” in the model fitting list implemented in the software. This generates the fitting curve (blue line) that interpolates the heat changes (red filled circles), and the related values of stoichiometry (N, black labelled), association equilibrium constant (KA, orange labelled), enthalpy (∆H, green labelled), and entropy (∆S black labelled) of the binding reaction. All these values are shown in the blue dotted box. C. Final ITC figure composed by an upper panel (corresponding to panel A) and lower panel (corresponding to panel B). Lower panel shows also the schematic representation of the calculations performed by the software to obtain: ∆H as the difference between the initial H value and the plateau H value (green line with double arrowheads); KA, which is the slope value of the orange line that intercepts the exponential phase of the isothermal curve (blue line); N, which is to the molar ratio (CPP:14-3-3c) at the centre of the isothermal curve (indicated by the black dotted line).
Figure 2 summarizes the processing of the ITC raw data and their subsequent analysis by using a single-binding model needed to obtain the binding curve for the CPP–14-3-3c interaction. Panel A shows negative heat changes (μcal/sec) during successive injections of 10 μl of CPP (500 μM) into the sample cell containing 14-3-3c (50 μM). This behavior, according to the basic ITC principles described in the Background section and illustrated in Figure 1, indicates that the CPP–14-3-3c interaction releases heat, so that the binding reaction is exothermic.
The software automatically integrates the peaks. This operation is graphically represented in Figure 2, Panel A, by the peaks colored in red. A critical aspect in the data analysis is the correct assessment of the integration details: the baseline and the integration range. The software automatically sets the integration details and integrates the peaks. However, there are cases where the signal to noise ratio is low and the automatic calculation of the integration details is not accurate enough. In these cases, both the baseline and the integration range need to be manually adjusted, following the “Instrument Handbook” instructions of MicroCal VP-ITC.
Moreover, the software automatically normalizes the integrated peaks to the CPP concentration, and plots them against the molar ratio of CPP (titrant) : 14-3-3c (titrated molecule) (red filled circles in Figure 2, Panel B). In Panel B, the solid blue line interpolating the red circles represents a nonlinear least-squares fit to a single-site binding model (Wiseman et al., 1989). The software calculates the stoichiometry (N), the association equilibrium constant (KA), the enthalpy (∆H), and the entropy (∆S) of the binding reaction. In Figure 2, Panel B, these values are shown within the blue dotted box. N, KA, and ∆H are directly derived from the isothermal curve, and for this reason they yield a fitting error. On the other hand, ∆S, which is indirectly calculated, does not yield a fitting error.
The Gibbs free energy (∆G) is not calculated by the software, but it can be calculated by the operator (see below).
Figure 2C, which is composed by panels A and B, corresponds to the final ITC figure most commonly used for publication.
For a better comprehension of the operations performed by the software, panel C includes a graphic representation of how the software calculates, starting from the isothermal curve, ∆H, N, and KA.
The binding enthalpy (∆H), which is due to hydrogen bonds and van der Waals interactions, is calculated as the difference between the starting H value and the plateau H value (see green line in Figure 2C). As stated above, the ∆H value is normalized per mole of the titrant.
The stoichiometry (N) corresponds to the molar ratio at the center of the isothermal curve (see the black dotted line in Figure 2C).
Note: An accurate assessment of the concentration of the biomolecules is very important, because the stoichiometry parameter is extremely sensitive to their concentration.
The association equilibrium constant (KA) corresponds to the slope of the line that intercepts the exponential phase of the isothermal curve (see blue line in Figure 2C). It is possible to manually calculate the dissociation equilibrium constant (KD), which is the equilibrium constant more commonly used to describe the affinity of biomolecules, by using the following equation:
The binding entropy (∆S), which is due to the desolvation of biomolecules and eventually to conformational changes induced by the complex formation, is indirectly calculated using the following equation:
The Gibbs free energy (∆G) is indirectly calculated using the following equation:
Notes
Recipes
Acknowledgments
This protocol was adapted from Saponaro et al. (2017), and generally follows the “Instrument Handbook” of the MicroCal VP-ITC system (Malvern Instruments Ltd). This work was supported by Lincean Academy (Italian Science Academy), Giuseppe Levi foundation.
Conflicts of interest or competing interests: none.
References
Article Information
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© 2018 The Authors; exclusive licensee Bio-protocol LLC.
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