Physical Chemistry of Drugs. Summary
This document contains statements, formulae, units and data tables which you are supposed to know.
Objectives
- Understand the underlying quantitative principles governing the behavior of therapeutic agents including:
- stability and storage of a therapeutic formulation,
- dissolution of drug crystals and powders and crystallization of drug metabolites
- chemical and physical determinants of bioavailability including drug permeation to the blood stream and crossing of the blood brain barrier;
- protonation and deprotonation, acid-base equilibrium and its role in permeability and solubility
- tautomerization and sterioisomerization and their role in adverse effects
- biological membranes, osmosis, and tonicity of drug solutions
- drug-receptor binding thermodynamics, relationship between a therapeutic dose or concentration and the binding energetics
- the molecular energetics and three dimensional structure of drug-protein complexes
- off-target protein-drug binding including carriers and polypharmacology
- kinetics including drug-binding kinetics, and drug diffusion
- Understand research literature about therapeutics that uses the following methods: calorimetry, X-ray crystallography, NMR, chromatography, mass spectrometry.
Drugs
- Drugs by size of the molecule of active ingredient
- Small molecules : from one atom (Xe) to about a four hundred non-hydrogen (a.k.a. heavy) atoms (the median is 24 heavy atoms, 99% of small drugs are between 5 to 70 heavy atoms)
- Peptide and natural products : peptides are aminoacid chains from 2 aminoacids to around 30 amino acids.
- Proteins : from 50 to thousands aminoacids (e.g. insulin, antibodies, growth factors )
- Vaccines
- Engineered viruses and reprogrammed/engineered cells (emerging)
By numbers from a set of active ingredients of the US-approved therapeutics as present in Drugbank on Jan 1, 2017:
- Small molecules: 1585
- 158 Unique Proteins/peptides (peptides and proteins from 8 amino acids to 2332 amino acids for Antihemophilic Factor).
- Median: 174 amino acids with 1400 atoms (compare with the median 24 atoms for small molecules)
- An average amino acid contributes about 8 heavy atoms.
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Figure. Distribution of small molecule drugs by the number of non-hydrogen (a.k.a. heavy) atoms Source: approved drugs from Drugbank, www.drugbank.ca |
Drugs by state of matter or phase
- gas (inhalers)
- liquid solutions
- micro-crystals or powder formulated with excipients
Units, scales, force, energy, temperature
- The basic SI units : kilogram, meter, second
- Temperature: measure of energy: Absolute temperature in Kelvin, K, and Celsius, C: K = C + 273.15
- The kinetic energy of a point mass m at velocity v is ( mv2 )/2
- Energy in the SI system is measured in Joules ( J ≡ kg m2 s-2 ), see the previous statement
- 1 calorie = 4.184J is the energy needed to increase 1g of water by 1 degree, 1 kcal is the same for 1kg (1L) of water
- 1 Calorie (or food calorie, note the capital 'C') is 1kcal
- 1 electron-volt = 1.6×10−19 joule : 1eV of 1 mole of particles ≅ 100 kJ
- Gas constant converts temperature to energy: R = 8.314 J K-1 mol-1 ; R = 1.986 cal K−1 mol−1* RT at 300K is 2.5 kJ/mol or 0.6 kcal/mol
- Force: F = ma .Units of force: Newton: N ≡ kg m s-2
- Work ≡ Force * Distance . Newton*meter = kg m2 s-2 has the same units as energy.
- Work changes the energy, without work the energy is conserved
- Heat is another form of energy
- The Avogadro number of a molecule is called one mole
- NA ≈ 6.* 1023 (btw: 6=2*3 , exact value is 6.022 * 1023 )
Moving Molecules, Gas Law
- PV = nRT ; R = 8.314 J K-1 mol-1
- Pressure is Force per unit area (P=F/A). SI Unit is pascal: 1Pa = Nm-2 or ; 1bar = 105 Pa ≅ 1atm = 760 mmMercury
- P Δ V = P • Area Δ X = F Δ X = WORK .
- Newton's law: F = m * a ( F and a are vectors)
- Conservation of Momentum = P ≡ ∑ m v = const without force.
- The total Momentum is conserved without external force, if the force is applied it is changed according to: ∂ P / ∂t = F (another form of Newton's 2nd law (3)).
- Mean energy of molecules and velocities: 1/2 mv2 = 3/2 kB T for 1 molecule, use molar mass and R instead of kB for 1 mole. The mean velocity is vrms = Sqrt( 3RT / M ), M is molar mass.
- Nitrogen (N2 molecules) move at speeds around 500 m/s at room temperature or ≅ 1120 Miles/hour . 100 times heavier molecule moves 10 times slower.
- 1 m/s = 2.237 Miles/hour
- Boltzman constant kB is defined as the Gas constant divided by the Avogadro number: R/NA
Thermodynamics
- A very large number of moving molecules can be described with average variables (parameters), such as P,V,T,concentrations, energies, etc.
- First law of thermodynamics: The increase in internal energy of a closed system is equal to the difference of the heat supplied to the system and the work done by it: ΔU = Q - W .
- Second law of thermodynamics: Heat cannot spontaneously flow from a colder location to a hotter location.
Heat Capacity
Additional reading: a good review of heat capacity and degrees of freedom here
- Heat capacity C ≡ Q/ΔT
- C depends on the amount of substance and the process (e.g. constant volume or pressure)
- CV = ΔU/ΔT , CV is the slope of the U(T) function
- Another form of the equation: UT = UT0 + CV (T - T0 ), with small ΔT or relatively constant CP in the range of temperatures involved.
- CP = ΔH/ΔT , where H is enthalpy H ≡ U + PV , CP is the slope of the H(T) function
- Another form of the equation: HT = HT0 + CP (T - T0 ) , with small ΔT or relatively constant CP in the range of temperatures involved.
- For CP or CV changing with T, use an integral over temperature range.
Degrees of Freedom and Energy Distribution
- Molecule consists of atoms connected by covalent bonds. Covalent bonds typically do not break at room temperature.
- Molecules and atoms in molecules can move, rotate and vibrate.
- Each degree of freedom carries on average energy 1/2 RT / NAvogadro. 1 mole of 1 degree of freedom carries 1/2 RT
- Each vibrational degree of freedom carries an additional 1/2 RT for potential energy. The total energy per one mole of vibrational degrees of freedom is RT.
- Effective temperature calculation: Since vibrational energy of one DOF is RT, Teffective = Emole /R .Example problem: E = 1eV = 100 kJ. What temperature it corresponds to? T = E/R = 11,500K
Calculating Degrees of Freedom of Molecules in Gas Phase
- Two general approaches:
- 3*Natoms - Nconstraints
- 6 (3 rigid body translations and rotations) + Ninternal_rotations_vibrations
- for a single molecule: one atom: 3 DOF, two atoms (02 N2 etc.) 5 if the bond is NOT excited, 6(7) if excited :
Heat Capacity
Covalent Bond Energies
Bond | Length(Å) | Energy (kJ/mol)
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Br-Br | 2.28 | -193
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C-Br | 1.94 | -288
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C-C | 1.54 | -348
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C=C | 1.34 | -614
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C≡C | 1.20 | -839
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C-Cl | 1.77 | -330
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C-F | 1.35 | -488
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C-H | 1.09 | -413
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C-I | 2.14 | -216
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C-N | 1.47 | -308
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C-O | 1.43 | -360
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C-S | 1.82 | -272
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Cl-Cl | 1.99 | -243
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F-F | 1.42 | -158
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H-Br | 1.41 | -366
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H-C | 1.09 | -413
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H-Cl | 1.27 | -432
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H-F | 0.92 | -568
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H-H | 0.74 | -436
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H-I | 1.61 | -298
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H-N | 1.01 | -391
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H-O | 0.96 | -366
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I-I | 2.67 | -151
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N≡N | 1.10 | -945
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N-N | 1.45 | -170
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O-O | 1.48 | -145
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O=O | 1.21 | -498
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Some rules for the bond energies:
- bond energies of stable bonds are negative;
- the higher the bond order, the lower the bond energy (note that the bond energy is negative, the lower, the more favorable);
- we define the bond energy as the energy required to form a bond from elements (opposite sign to what is required to break a bond);
- note that some textbooks use the term bond energy as "the bond-breaking energy", rather than "bond-forming" energy;
- energy is released when bonds form;
- energy is absorbed when bonds break;
- many chemistry textbooks mislead students into thinking that "Chemical bonds store energy". Reality is opposite;
Chemical reaction, burning
- Balance of bond energies dominates in the heats of chemical reaction
- A simple rule:
- heat produced/exothermic_reaction ≡ bonds formed or stronger bonds
- heat absorbed/endothermic_reaction ≡ bonds broken or weaker bonds
- Example: 2H2 + O2 => 2H2O : before 3 bonds, after 4 bonds (see table for details). Bonds gained: heat produced.
- Example with equal number of bonds but different strength: H2(g) + Br2(g) -> 2 HBr (g). Two for two, but Br2 bond is weak: 2*(-366) -((-436)+(-193)) = -103 (kJ/m): exothermic reaction
Energy comparisons for one photon in electon-volts (eV). 1 eV = 1.6 10-19 J .
- 210 MeV: the average energy released in fission of one Pu-239 atom
- 200 MeV: the average energy released in nuclear fission of one U-235 atom
- 17.6 MeV: the average energy released in the fusion of deuterium and tritium to form He-4; this is 0.41 PJ per kilogram of product produced
- 1 MeV (1.602×10−13 J): about twice the rest energy of an electron
- 13.6 eV: the energy required to ionize atomic hydrogen; molecular bond energies are on the order of 1 eV to 10 eV per bond
- 1.6 eV to 3.4 eV: the photon energy of visible light
- 25 meV: the thermal energy kBT at room temperature; one air molecule has an average kinetic energy 38 meV
- 230 µeV: the thermal energy kBT of the cosmic microwave background
Math background
Basic facts
- e = 2.71828. The number e is an important mathematical constant, approximately equal to 2.71828
- ln ≡ loge
- Pythagorean theorem: in a right-angled triangle with sides a,b, and hypotenuse c : a² + b² = c²
- Area of a circle is πr² where r = radius of a circle
- Volume of a cylinder is πr²h where r = radius of circular face, h = height
- Volume of a sphere : (4/3)πr³
Weighted average
Simple average: A, B, C (N=3) Average = ( A + B + C )/N
Weighted average: A,B,C, WA WB WC .
Weighted_Average = (A*WA + B*WB + C*WC )/ ( WA + WB + WC )
Trigonometry
Use the trigonometric circle.
Note that angles are measured in radians or degrees ° ( e.g. π/2 is 90° , π is 180° etc.).
DO NOT TRY TO use calculator for a trigonometry question to calculate cos( π/ 2 ) , - the calculator will give you an answer as if it is the number of degrees. The degree is usually explicitly stated with the ° symbol,
the presence of π in the formula means that the value is in radian units.
sin( 0 ) = sin( π ) = sin( 2π )=0 | cos( 0 ) = cos ( 2π) = 1.; cos( π ) = -1
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sin( ½π ) = 1. | cos( ±½π ) = 0.
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sin( -α ) = - sin( α ) | cos( -α ) = cos( α )
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Logarithms
Definition:
loga (x) = y means x = ay
formula | example
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log(xy) = log(x) + log(y) |
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log(x/y) = log(x) - log(y) |
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log(1/y) = -log(y) | log10 (0.01) = log10 (1/100) = -log10 (100) = -2
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log(xp ) = p log(x) | log10 1000 = log10 103 = 3 log10 10 = 3
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ln(x)≡loge (x) = 2.3 log10 (x) |
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Derivatives
Notations
(rarely used Newton's notation is omitted):
df/dx , d2 f/dx2 | Leibniz | 1st and 2nd derivative
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f'(x), f''(x) | Lagrange | 1st and 2nd derivative
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∂f(x,y,z..)/∂x | Leibniz | partial derivative
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Differentiation rules
Type | Function | Derivative | Example
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Constant | f(x) = a | f'(x) = 0 | a' = 0
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Power | f(x) = xn | f'(x) = nxn-1 | (x2 )' = 2x
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Product | f • g | f' g + f g' |
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Quotient | f / g | ( f' g - f g' )/( g2 ) |
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Chain | f(g(x)) | (df/dg)(dg/dx) |
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Exponent | ex | ex |
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Exponent | eax | aex |
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Exponent | ax | ax • log(a) |
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Log | ln(x) | 1/x |
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Sin | sin(x) | cos(x) |
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Cos | cos(x) | -sin(x) |
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Integrals
Type | Function | Integral | Example
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Constant | a | ax + C |
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Power | xn | xn+1 /(n+1) + C |
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One over x | x-1 | ln(x) + C (x>0) |
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Exponential | ax | ax /ln(a) + C |
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Unit conversions and main constants
Celsius | Kelvin - 273.15
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Kelvin (K) | Celsius + 273.15
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1 kJ | 0.239 kcal
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1 kcal | 4.184 kJ
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1 eV | 1.6 × 10-19 joules
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1 L (liter) | 10-3 m3 |
1 meter/second | 2.237 Miles/hour
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1 Mile/hour | 0.44704 meter/second
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1 mole of sub. | MW gram (MW is in Daltons, of Da).
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1 g of sub. | 1/MW moles
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Physical Constants
abbrev. | definition | exact value, units | approximation
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c | speed of light | 299 792 458 m / s | 3 108
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G | Gravitational constant | 6.673×10−11 N·(m/kg)2 |
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g | acceleration of free fall | 9.8 m/s2 |
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h | Planck constant | 6.6260695 ×10−34 J·s | 6.626×10−34 |
ke | Coulomb's constant | 8.98755×109 N·m2 /C2 |
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NA | Avagadro constant | 6.02214129×1023 mol−1 | 6×1023 |
R | gas constant | 8.3144621 JK-1 mol-1 | 8.3
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Glossary
Root mean square value (rms)
If one has an array of N values of Xi, e.g. velocities of many molecules, the root mean square value can be calculated by the following process: (i) average the squared values, (ii) take a square root of the average:
Xrms = (( ∑ X²i )/ N )½