This appendix includes the background knowledge and equation derivation originally in the supporting information of the Binding Curve Viewer paper.
In the competitive binding experiment, the binding of the protein and ligand and the binding of the protein and inhibitor are described by the following equations,
The \(K_\mathrm{d}\) is the dissociation constant of the protein and ligand. The \(K_\mathrm{i}\) is the dissociation constant of the protein and inhibitor. At equilibrium, the total concentration of the protein (\([\mathrm{P}]_0\)) is the sum of the equilibrium concentration of the protein (\([\mathrm{P}]_\mathrm{eq}\)), the equilibrium concentration of the protein-ligand complex (\([\mathrm{PL}]_\mathrm{eq}\)), and the equilibrium concentration of the protein-inhibitor complex (\([\mathrm{PI}]_\mathrm{eq}\)).
At equilibrium,
Equation 2 can be written as
We substitute equation 3 into equation 1 and obtain
We multiple \(\frac{\left[\mathrm{L}\right]_\mathrm{eq}}{\left[\mathrm{PL}\right]_\mathrm{eq}}\) on both sides of equation 4 and obtain
Equation 5 can be transformed into equation 6
When 50% of the “initial binding” of the protein and ligand is inhibited, the concentration of the free competing inhibitor (\([\mathrm{I}]_\mathrm{eq}\)) is defined as the \(\mathrm{IC}_{50}\) and the concentration of the total competing inhibitor (\([\mathrm{I}]_0\)) is defined as the apparent \(\mathrm{IC}_{50}\). The initial binding means the equilibrium concentration of the protein-ligand complex in the blank control in the competitive binding of either association or dissociation. In association, the blank control was the mixture of the protein and the solution with ligand and no inhibitor. In dissociation, the blank control was the mixture of the equilibrated protein and ligand and the solution without inhibitor. The blank control is important to eliminate the equilibrium concentration change of the protein-ligand complex upon the volume change after mixing. At the equilibrium state of 50% inhibition of the protein-ligand binding, the concentration of the protein-ligand complex (\([\mathrm{PI}]_\mathrm{eq\textnormal{-}50}\)) can be written as
In this work, we used the Wang equation to simulate the theoretical inhibition curve, and estimated the \(\mathrm{IC}_{50}\) and apparent \(\mathrm{IC}_{50}\), without the restrictions of concentrations.
At the equilibrium state of 50% inhibition of the protein-ligand binding, if \(\left[\mathrm{L}\right]_0\gg\left[\mathrm{P}\right]_0\) and \(\left[\mathrm{I}\right]_0\gg\left[\mathrm{P}\right]_0\), or strictly speaking, \(\left[\mathrm{L}\right]_0\gg\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}\) and \(\left[\mathrm{I}\right]_0\gg\left[\mathrm{PI}\right]_\mathrm{{eq\textnormal{-}50}}\), \(\left[\mathrm{L}\right]_\mathrm{{eq\textnormal{-}50}}=\left[\mathrm{L}\right]_0-\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}\approx\left[\mathrm{L}\right]_0\) and \(\mathrm{IC}_{50}=\left[\mathrm{I}\right]_\mathrm{{eq\textnormal{-}50}}=\left[\mathrm{I}\right]_0-\left[\mathrm{PI}\right]_\mathrm{{eq\textnormal{-}50}}\approx\left[\mathrm{I}\right]_0\), equation 7 approximately equals
Thus, \(\mathrm{IC}_{50}\) is almost equal to \([\mathrm{I}]_0\). From equation 13 in Appendix 1, we know that in the absence of the inhibitor and when \(\left[\mathrm{L}\right]_0\gg\left[\mathrm{P}\right]_0\), the equilibrium concentration of the protein-ligand complex (\([\mathrm{PL}]_\mathrm{{eq\textnormal{-}0}}\)) equals
At the time of 50% inhibition of the protein-ligand binding, \(\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}0}}=2\times\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}\), so
Thus, we obtain the Cheng-Prusoff equation generalized in the competitive binding (equation 8), the \([\mathrm{I}]_0\) in equation 8 is the apparent \(\mathrm{IC}_{50}\), which approximately equals the \(\mathrm{IC}_{50}\) in the condition of \(\left[\mathrm{I}\right]_0\gg\left[\mathrm{PI}\right]_\mathrm{{eq\textnormal{-}50}}\). The apparent \(\mathrm{IC}_{50}\) can be estimated by the theoretical inhibition curve.
If we substitute equation 5 by \(\left[\mathrm{L}\right]_\mathrm{eq}=\left[\mathrm{L}\right]_0-\left[\mathrm{PL}\right]_\mathrm{eq}\), we obtain
We multiple \(\frac{1}{\left[\mathrm{L}\right]_0}\) on both sides of equation 9 and obtain
At the equilibrium state of 50% inhibition, equation 10 can be written as
We name the equation (6) in the original paper the “Lin-Riggs equation”, which was derived in the context of the competitive inhibition of the protein and labelled nucleic acid. In contrast to \(\frac{\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}}{\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}0}}}=0.5\) in the previous section, \(\frac{\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}}{\left[\mathrm{L}\right]_0}=0.5\) in the competitive inhibition of the protein and labelled nucleic acid. Thus, equation 11 can be converted to
The usage condition of the Lin-Riggs equation is \(\left[\mathrm{L}\right]_0\approx\left[\mathrm{PL}\right]_\mathrm{eq}\) and \(\left[\mathrm{I}\right]_0\gg\left[\mathrm{PI}\right]_\mathrm{eq}\). In this condition, \(\mathrm{IC}_{50}=\left[\mathrm{I}\right]_\mathrm{{eq\textnormal{-}50}}=\left[\mathrm{I}\right]_0-\left[\mathrm{PI}\right]_\mathrm{{eq\textnormal{-}50}}\approx\left[\mathrm{I}\right]_0\), we can thus use equation 13 to calculate the apparent \(K_\mathrm{i}\),
The \([\mathrm{I}]_0\) in equation 13 is the apparent \(\mathrm{IC}_{50}\), which approximately equals the \(\mathrm{IC}_{50}\). Thus, equation 13 is essentially the same as the Lin-Riggs equation. The apparent \(\mathrm{IC}_{50}\) can be estimated by the theoretical inhibition curve.
It is worth noting that the experimental conditions were different between the calculations using the Cheng-Prusoff equation and the Lin-Riggs equation, because the \([\mathrm{PL}]_\mathrm{{eq\textnormal{-}0}}\) should be greater than the half of the \([\mathrm{L}]_0\) in the calculations using the Lin-Riggs equation. Namely, in the conditions of \([\mathrm{P}]_0 = 50\ \mathrm{nM}\) and \(K_\mathrm{d} = 50\ \mathrm{nM}\), \([\mathrm{P}]_0 = 5\ \mathrm{nM}\) and \(K_\mathrm{d} = 50\ \mathrm{nM}\), and \([\mathrm{P}]_0 = 5\ \mathrm{nM}\) and \(K_\mathrm{d} = 5\ \mathrm{nM}\), the \([\mathrm{PL}]_\mathrm{{eq\textnormal{-}0}}\) was smaller than \(\frac{\left[\mathrm{L}\right]_0}{2}\). When generating the theoretical inhibition curve with increasing \([\mathrm{L}]_0\), the range of the \([\mathrm{L}]_0\) was also restricted, because the \([\mathrm{PL}]_\mathrm{{eq\textnormal{-}0}}\) should be greater than the half of the \([\mathrm{L}]_0\).
We used the Wang’s group equation (equation 14) to calculate the \(K_\mathrm{i}\). At the equilibrium state of 50% inhibition, \(\frac{\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}50}}}{\left[\mathrm{PL}\right]_\mathrm{{eq\textnormal{-}0}}}=0.5\). The apparent \(\mathrm{IC}_{50}\) can be estimated by the theoretical inhibition curve.
For the details of the calculation, see the original paper or the function calc_ki in our script ki_app_calc.py