The Hill equation is commonly expressed in the following ways: : \begin{align}\theta &= {[\ce L]^n \over K_d + [\ce L]^n}\\ &= {[\ce L]^n \over (K_A)^n + [\ce L]^n}\\ &= {1 \over 1+\left({K_A \over [\ce L]}\right)^n}\end{align} , where • \theta is the fraction of the
receptor protein concentration that is bound by the
ligand, • [L]is the total
ligand concentration, • K_d is the apparent
dissociation constant derived from the
law of mass action, • K_A is the ligand concentration producing half occupation, • n is the Hill coefficient. The special case where n=1 is a
Monod equation.
Constants In pharmacology, \theta is often written as p_\ce{AR}, where A is the ligand, equivalent to L, and R is the receptor. \theta can be expressed in terms of the total amount of receptor and ligand-bound receptor concentrations: \theta = \frac\ce{[LR]}\ce{[R_{\rm total}]}. K_d is equal to the ratio of the dissociation rate of the ligand-receptor complex to its association rate (K_{\rm d} = {k_{\rm d} \over k_{\rm a}}). Kd is the equilibrium constant for dissociation. K_A is defined so that (K_A)^n = K_{\rm d} = {k_{\rm d} \over k_{\rm a}}, this is also known as the microscopic
dissociation constant and is the ligand concentration occupying half of the binding sites. In recent literature, this constant is sometimes referred to as K_D.
Gaddum equation The
Gaddum equation is a further generalisation of the Hill-equation, incorporating the presence of a reversible competitive antagonist. The Gaddum equation is derived similarly to the Hill-equation but with 2 equilibria: both the ligand with the receptor and the antagonist with the receptor. Hence, the Gaddum equation has 2 constants: the equilibrium constants of the ligand and that of the antagonist
Hill plot The Hill plot is the rearrangement of the Hill equation into a straight line. Taking the reciprocal of both sides of the Hill equation, rearranging, and inverting again yields: {\theta\over 1-\theta} = {[\ce L]^n \over K_d } = {[\ce L]^n \over (K_A)^n } . Taking the logarithm of both sides of the equation leads to an alternative formulation of the Hill-Langmuir equation: : \begin{align}\log\left( {\theta\over 1-\theta} \right) &= n \log{[\ce L]} - \log{K_d}\\ &= n \log{[\ce L]} - n \log{K_A} \end{align}. This last form of the Hill equation is advantageous because a plot of
\log\left( {\theta\over 1-\theta} \right) versus \log{[\ce L]} yields a
linear plot, which is called a
Hill plot. Because the slope of a Hill plot is equal to the Hill coefficient for the biochemical interaction, the slope is denoted by n_H. A slope greater than one thus indicates positively cooperative binding between the receptor and the ligand, while a slope less than one indicates negatively cooperative binding. Transformations of equations into linear forms such as this were very useful before the widespread use of computers, as they allowed researchers to determine parameters by fitting lines to data. However, these transformations affect error propagation, and this may result in undue weight to error in data points near 0 or 1.{{refn|group=nb|See
Propagation of uncertainty. The function f(\theta)=\log_{10}\left(\frac{\theta}{1-\theta}\right) propagates errors in \theta as \delta_f=\delta_\theta\frac{\mathrm{d}f}{\mathrm{d}\theta}=\frac{\delta_\theta}{(\ln10)\,\theta(1-\theta)}. Hence errors in values of \theta near 0 or 1 are given far more weight than those for \theta\approx0.5}} This impacts the parameters of linear regression lines fitted to the data. Furthermore, the use of computers enables more robust analysis involving
nonlinear regression. == Tissue response ==