# Michaelis-Menten kinetics

### Michaelis-Menten kinetics

In biochemistry, Michaelis–Menten kinetics is one of the simplest and best-known models of enzyme kinetics. It is named after German biochemist Leonor Michaelis and Canadian physician Maud Menten. The model takes the form of an equation describing the rate of enzymatic reactions, by relating reaction rate $v$ to $\left[S\right]$, the concentration of a substrate S. Its formula is given by

$v = \frac\left\{d \left[P\right]\right\}\left\{d t\right\} = \frac\left\{ V_\max \right\}\left\{K_m + \left[S\right]\right\}$.

Here, $V_\max$ represents the maximum rate achieved by the system, at maximum (saturating) substrate concentrations. The Michaelis constant $K_m$ is the substrate concentration at which the reaction rate is half of $V_\max$. Biochemical reactions involving a single substrate are often assumed to follow Michaelis–Menten kinetics, without regard to the model's underlying assumptions.

## Model

In 1903, French physical chemist Victor Henri found that enzyme reactions were initiated by a bond between the enzyme and the substrate.[1] His work was taken up by German biochemist Leonor Michaelis and Canadian physician Maud Menten, who investigated the kinetics of an enzymatic reaction mechanism, invertase, that catalyzes the hydrolysis of sucrose into glucose and fructose.[2] In 1913, they proposed a mathematical model of the reaction.[3] It involves an enzyme E binding to a substrate S to form a complex ES, which in turn is converted into a product P and the enzyme. This may be represented schematically as



E + S \, \overset{k_f}{\underset{k_r} \rightleftharpoons} \, ES \, \overset{k_\mathrm{cat}} {\longrightarrow} \, E + P

where $k_f$, $k_r$, and $k_\mathrm\left\{cat\right\}$ denote the rate constants,[4] and the double arrows between S and ES represent the fact that enzyme-substrate binding is a reversible process.

Under certain assumptions – such as the enzyme concentration being much less than the substrate concentration – the rate of product formation is given by

$v = \frac\left\{d \left[P\right]\right\}\left\{d t\right\} = V_\max \frac\left\{K_m + \left[S\right]\right\} = k_\mathrm\left\{cat\right\} \left[E\right]_0 \frac\left\{K_m + \left[S\right]\right\}$

The reaction rate increases with increasing substrate concentration $\left[S\right]$, asymptotically approaching its maximum rate $V_\max$, attained when all enzyme is bound to substrate. It also follows that $V_\max = k_\mathrm\left\{cat\right\} \left[E\right]_0$, where $\left[E\right]_0$ is the enzyme concentration. $k_\mathrm\left\{cat\right\}$, the turnover number, is the maximum number of substrate molecules converted to product per enzyme molecule per second.

The Michaelis constant $K_m$ is the substrate concentration at which the reaction rate is at half-maximum, and is an inverse measure of the substrate's affinity for the enzyme—as a small $K_m$ indicates high affinity, meaning that the rate will approach $V_\max$ more quickly.[5] The value of $K_m$ is dependent on both the enzyme and the substrate, as well as conditions such as temperature and pH.

The model is used in a variety of biochemical situations other than enzyme-substrate interaction, including antigen-antibody binding, DNA-DNA hybridization, and protein-protein interaction.[5][6] It can be used to characterise a generic biochemical reaction, in the same way that the Langmuir equation can be used to model generic adsorption of biomolecular species.[6] When an empirical equation of this form is applied to microbial growth, it is sometimes called a Monod equation.

## Applications

Parameter values vary wildly between enzymes:[7]

Enzyme $K_m$ (M) $k_\text\left\{cat\right\}$ (1/s) $k_\text\left\{cat\right\}/K_m$ (1/M.s)
Chymotrypsin 1.5 × 10−2 0.14 9.3
Pepsin 3.0 × 10−4 0.50 1.7 × 103
Tyrosyl-tRNA synthetase 9.0 × 10−4 7.6 8.4 × 103
Ribonuclease 7.9 × 10−3 7.9 × 102 1.0 × 105
Carbonic anhydrase 2.6 × 10−2 4.0 × 105 1.5 × 107
Fumarase 5.0 × 10−6 8.0 × 102 1.6 × 108

The constant $k_\text\left\{cat\right\}/K_m$ is a measure of how efficiently an enzyme converts a substrate into product. It has a theoretical upper limit of 108 – 1010 /M.s; enzymes working close to this, such as fumarase, are termed superefficient.[8]

Michaelis–Menten kinetics have also been applied to a variety of spheres outside of biochemical reactions,[4] including alveolar clearance of dusts,[9] the richness of species pools,[10] clearance of blood alcohol,[11] the photosynthesis-irradiance relationship, and bacterial phage infection.[12]

## Derivation

Applying the law of mass action, which states that the rate of a reaction is proportional to the product of the concentrations of the reactants (i.e.[E][S]), gives a system of four non-linear ordinary differential equations that define the rate of change of reactants with time $t$:[13]

In this mechanism, the enzyme E is a catalyst, which only facilitates the reaction, so that its total concentration, free plus combined, $\left[E\right] + \left[ES\right] = \left[E\right]_0$ is a constant. This conservation law can also be observed by adding the second and third equations above.[13][14]

### Equilibrium approximation

In their original analysis, Michaelis and Menten assumed that the substrate is in instantaneous chemical equilibrium with the complex, and thus $k_f \left[E\right] \left[S\right] = k_r \left[ES\right]$.[3][14] Combining this relationship with the enzyme conservation law, the concentration of complex is[14]

$\left[ES\right] = \frac\left\{K_d + \left[S\right]\right\}$

where $K_d = k_r / k_f$ is the dissociation constant for the enzyme-substrate complex. Hence the velocity $v$ of the reaction – the rate at which P is formed – is[14]

$v = \frac\left\{d \left[P\right]\right\}\left\{d t\right\} = \frac\left\{V_\max \right\}\left\{K_d + \left[S\right]\right\}$

where $V_\max = k_\mathrm\left\{cat\right\} \left[E\right]_0$ is the maximum reaction velocity.

An alternative analysis of the system was undertaken by British botanist G. E. Briggs and British geneticist J. B. S. Haldane in 1925.[15] They assumed that the concentration of the intermediate complex does not change on the time-scale of product formation – known as the quasi-steady-state assumption or pseudo-steady-state-hypothesis. Mathematically, this assumption means $k_f \left[E\right] \left[S\right] = k_r \left[ES\right] + k_\mathrm\left\{cat\right\} \left[ES\right]$. Combining this relationship with the enzyme conservation law, the concentration of complex is[14]

$\left[ES\right] = \frac\left\{K_m + \left[S\right]\right\}$

where

$K_m = \frac\left\{k_r + k_\mathrm\left\{cat\right\}\right\}\left\{k_f\right\}$

is known as the Michaelis constant, where $k_r$, $k_\mathrm\left\{cat\right\}$, and $\left\{k_f\right\}$ are, respectively, the constants for substrate unbinding, conversion to product, and binding to the enzyme. Hence the velocity $v$ of the reaction is[14]

$v = \frac\left\{d \left[P\right]\right\}\left\{d t\right\} = \frac\left\{V_\max \right\}\left\{K_m + \left[S\right]\right\}$

### Assumptions and limitations

The first step in the derivation applies the law of mass action, which is reliant on free diffusion. However, in the environment of a living cell where there is a high concentration of proteins, the cytoplasm often behaves more like a gel than a liquid, limiting molecular movements and altering reaction rates.[16] Whilst the law of mass action can be valid in heterogeneous environments,[17] it is more appropriate to model the cytoplasm as a fractal, in order to capture its limited-mobility kinetics.[18]

The resulting reaction rates predicted by the two approaches are similar, with the only difference being that the equilibrium approximation defines the constant as $K_d$, whilst the quasi-steady-state approximation uses $K_m$. However, each approach is founded upon a different assumption. The Michaelis–Menten equilibrium analysis is valid if the substrate reaches equilibrium on a much faster time-scale than the product is formed or, more precisely, that [14]

$\epsilon_d = \frac\left\{k_\mathrm\left\{cat\right\}\right\}\left\{k_r\right\} \ll 1$

By contrast, the Briggs–Haldane quasi-steady-state analysis is valid if [13][19]

$\epsilon_m = \frac \left\{\underset\left\{k_\left\{r_1\right\}\right\} \left\{\rightleftharpoons\right\}\right\} \, ES \, \overset\left\{k_\left\{f_2\right\}\right\} \left\{\underset\left\{k_\left\{r_2\right\}\right\} \left\{\rightleftharpoons\right\}\right\} \, E + P$

In general, the assumption of irreversibility is a good one in situations where one of the below is true:
1. The concentration of substrate(s) is very much larger than the concentration of products:

$\left[S\right] \gg \left[P\right]$

This is true under standard in vitro assay conditions, and is true for many in vivo biological reactions, particularly where the product is continually removed by a subsequent reaction.
2. The energy released in the reaction is very large, that is

$\Delta\left\{G\right\} \ll 0$

In situations where neither of these two conditions hold (that is, the reaction is low energy and a substantial pool of product(s) exists), the Michaelis–Menten equation breaks down, and more complex modelling approaches explicitly taking the forward and reverse reactions into account must be taken to understand the enzyme biology.

## Determination of constants

The typical method for determining the constants $V_\max$ and $K_m$ involves running a series of enzyme assays at varying substrate concentrations $\left[S\right]$, and measuring the initial reaction rate $v_0$. 'Initial' here is taken to mean that the reaction rate is measured after a relatively short time period, during which it is assumed that the enzyme-substrate complex has formed, but that the substrate concentration held approximately constant, and so the equilibrium or quasi-steady-state approximation remain valid.[19] By plotting reaction rate against concentration, and using nonlinear regression of the Michaelis–Menten equation, the parameters may be obtained.[20]

Before computing facilities to perform nonlinear regression became available, graphical methods involving linearisation of the equation were used. A number of these were proposed, including the Eadie–Hofstee diagram, Hanes–Woolf plot and Lineweaver–Burk plot; of these, the Hanes–Woolf plot is the most accurate.[20] However, while useful for visualization, all three methods distort the error structure of the data and are inferior to nonlinear regression.[21] Nonetheless, their use can still be found in modern literature.[22]

In 1997 Santiago Schnell and Claudio Mendoza derived a closed form solution for the time course kinetics analysis of the Michaelis–Menten kinetics.[23] The solution, known as the Schnell-Mendoza equation, has the form:

$\frac\left\{K_M\right\} = W \left\left[ F\left(t\right) \right\right]\,$

where W[] is the Lambert-W function and where F(t) is

$F\left(t\right) = \frac\left\{K_M\right\} = W \left\left[ F\left(t\right) \right\right]- \frac\left\{V_\max\right\}\left\{k_\left\{cat\right\} K_M\right\}\ \frac\left\{W \left\left[ F\left(t\right) \right\right]\right\}\left\{1+W \left\left[ F\left(t\right) \right\right]\right\}\,$

where W[] is again the Lambert-W function.