Chemistry equations in Markdown to PDF
Reaction arrows, equilibria, charges and subscripts are written in LaTeX notation and typeset with the conventions of chemistry texts.
Reaction equations and equilibria, the Arrhenius and Nernst equations, pH and buffers, Michaelis-Menten kinetics, radioactive decay, the ideal gas law and Beer-Lambert. Toggle: math.
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Markdown · 50 lines# Chemistry and life sciences
## Reactions and equilibrium
$ \mathrm{2\,H_2 + O_2 \longrightarrow 2\,H_2O} \qquad \mathrm{N_2 + 3\,H_2 \rightleftharpoons 2\,NH_3} \qquad \mathrm{CaCO_3 \overset{\Delta}{\longrightarrow} CaO + CO_2} $
For $a\mathrm{A} + b\mathrm{B} \rightleftharpoons c\mathrm{C} + d\mathrm{D}$ the equilibrium constant and the reaction quotient are
$ K_c = \frac{[\mathrm{C}]^c\,[\mathrm{D}]^d}{[\mathrm{A}]^a\,[\mathrm{B}]^b} \qquad \Delta G = \Delta G^{\circ} + RT \ln Q \qquad \Delta G^{\circ} = -RT \ln K $
## Kinetics
Rate laws, the Arrhenius equation and the half-life of a first-order process:
$ r = k\,[\mathrm{A}]^m [\mathrm{B}]^n \qquad k = A\, e^{-E_a / RT} \qquad \ln \frac{k_2}{k_1} = -\frac{E_a}{R} \left( \frac{1}{T_2} - \frac{1}{T_1} \right) \qquad t_{1/2} = \frac{\ln 2}{k} $
Michaelis-Menten enzyme kinetics and its linearized form:
$ v = \frac{V_{\max}\,[\mathrm{S}]}{K_m + [\mathrm{S}]} \qquad \frac{1}{v} = \frac{K_m}{V_{\max}} \cdot \frac{1}{[\mathrm{S}]} + \frac{1}{V_{\max}} $
## Acids, bases and electrochemistry
$ \mathrm{pH} = -\log_{10} [\mathrm{H^+}] \qquad \mathrm{pH} = \mathrm{p}K_a + \log_{10} \frac{[\mathrm{A^-}]}{[\mathrm{HA}]} \qquad K_w = [\mathrm{H^+}][\mathrm{OH^-}] = 10^{-14} \text{ at } 25\ ^\circ\mathrm{C} $
$ E = E^{\circ} - \frac{RT}{nF} \ln Q \qquad \Delta G^{\circ} = -nFE^{\circ} \qquad \mathrm{Zn} + \mathrm{Cu^{2+}} \longrightarrow \mathrm{Zn^{2+}} + \mathrm{Cu} $
## Gases and solutions
$ pV = nRT \qquad \left( p + \frac{a n^2}{V^2} \right)(V - nb) = nRT \qquad A = \varepsilon\, \ell\, c \qquad \Pi = i\, c\, R\, T $
## Nuclear and radiological
$ N(t) = N_0\, e^{-\lambda t} \qquad A(t) = \lambda N(t) \qquad E = \Delta m\, c^2 \qquad {}^{14}_{6}\mathrm{C} \longrightarrow {}^{14}_{7}\mathrm{N} + e^- + \bar{\nu}_e $
## Population and pharmacology
Logistic growth, and the one-compartment model with first-order elimination:
$ \frac{\mathrm{d}N}{\mathrm{d}t} = rN \left( 1 - \frac{N}{K} \right) \qquad C(t) = \frac{D}{V_d}\, e^{-k_e t} \qquad t_{1/2} = \frac{0.693\, V_d}{\mathrm{CL}} \qquad \mathrm{AUC} = \int_0^{\infty} C(t)\,\mathrm{d}t = \frac{D}{\mathrm{CL}} $
Hardy-Weinberg equilibrium for two alleles with frequencies $p$ and $q$:
$ p^2 + 2pq + q^2 = 1, \qquad p + q = 1 $
| Quantity | Symbol | Typical value |
|:---------|:------:|:--------------|
| Gas constant | $R$ | $8.314\ \mathrm{J\,mol^{-1}\,K^{-1}}$ |
| Faraday constant | $F$ | $96\,485\ \mathrm{C\,mol^{-1}}$ |
| Avogadro constant | $N_A$ | $6.022 \times 10^{23}\ \mathrm{mol^{-1}}$ |
| Half-life of carbon-14 | $t_{1/2}$ | $5{,}730$ years |
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