Fundamental Interactions: 6 Forces
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1 Fundamental Interactions: 6 Forces In nuclear and high-energy physics 6 fundamental forces are recognized, which describe the structure of matter. - the strong interaction - the weak interaction act inside the nucleus, range < 10-5 nm ~ 1/10000 of the diameter of an atom - the electromagnetic interaction - gravitation - the super-strong interaction - the super-weak interaction source of all intermolecular forces! (ellman-feynman) very long-range between macroscopic objects, negligible between molecules very particular forces only used in nuclear physics (don't bother...) ellman-feynman theorem: "Once the spatial distribution of the electron clouds has been determined by solving the Schrödinger equation, the intermolecular forces may be calculated on the basis of straightforward classical electrostatics."
2 Fundamental Interactions: Details - the strong interaction: nuclear interaction (holds protons & neutrons in the nucleus together by exchange of pions), very fast (about the time a photon c travels through a proton ~ s), acts between "hadron" (nucleons, mesons, hyperons), not between "leptons" (electrons, myons, neutrinos) at a distance of < m Feynman diagrams neuton (n) time pion p n p W positron (e + ) antineutrino - the weak interaction: nuclear interaction (responsible for nuclear -decay / electron emission & and slow decay of elementary particles), time scale varies considerably ( s), interaction involves "leptons", depends on the parity (symmetry of translation & spin) of the particles, acts over distances << m (below strong interaction) (W: hypothetical particle mediating weak force) - the electromagnetic interaction: binds electrons to nucleus, binds atoms to molecules, responsible for all chemistry and biology, acts in electron-positron annihilation, time scale lies between strong and weak interaction, interaction is mediated by the photon, acts primarily between charged particles over infinite distance (in principle), is neutralized by opposite charge proton (p) - gravitation: longest known & least understood, negligible in molecular dimensions, but important for mesoscopic to macroscopic objects (like in buoyancy or droplet deformation), acts attractive between all matter, very long range (between galaxies, e.g.) w(r) = -G m 1 m 2 / r G = 6.67 x N m 2 kg -2 p p x photon n e e relative interaction strength: strong (15) : el.mag. (1/137) : weak (10-12 ) : gravitation (10-35 )
3 { { { { Pair Potentials - van der Waals: deviation of behavior of real gases from ideal gas law (pv = nrt): p a V b RT V2 { { excluded volume of atoms / molecules attractive intermolecular forces ( van der Waals forces) - Mie: general interaction "pair potential" to describe complex intermolecular interactions: w r A r n B r m repulsive term - Lennard-Jones: attractive term w / F w r A r 6 B r 12 very short-range "hard sphere" repulsion r long-range attractive van der Waals interaction
4 Long / Short-Range Forces and Strong / Weak Forces The interaction parameter X determines the strength of the interaction. the larger X the stronger the interaction strong w X r n weak w long-range w X r n short-range The exponent in the distance variable r determines the range of the interaction. the larger the exponent n the shorter the interaction range
5 Types of Interactions: Overview 1 type of interaction interaction energy w(r) J. Israelachvili; "Intermolecular and Surface Forces", Second Ed.; Academic Press Limited: London, 1995, p. 28
6 Types of Interactions: Overview 2 type of interaction interaction energy w(r) J. Israelachvili; "Intermolecular and Surface Forces", Second Ed.; Academic Press Limited: London, 1995, p. 28
7 Intermolecular Interactions: covalent: e.g. disulfide bonds S S red. ox. S S ionic: e.g. ammonium salts on mica N 3 mica -bonding: e.g. DNA double helix coordinative: e.g. transition metal complexes Co N 3 dipole-dipole: e.g. nitroaniline in zeolite 2 N NO 2 2 N NO 2 dispersion: e.g. alkyl chains µ µ charge transfer (CT): e.g. intercalation of trinitrofluorenone into triphenylene columns topological link: catenanes / rotaxanes endohedral fullerene complexes form anisotropy: liquid crystals ordered colloidal dispersions
8 Chemical Bonds: Covalent, Ionic, Metallic, Coordinative Chemical bonds: strong bonds between atoms to form molecules and extended solids. relates to cohesion within a covalent bonded material Examples in surface sciences: -covalent surface bonds: hydrosilylation of hydrogen terminated silicon surface (radical, thermal, photochem., catalytic): Si Si Si R R Si Si Si R R R R -ionic surface bonds: quaternary ammonium salts on mica: N N N mica -metallic surface bonds: interface between two metal layers: -coordinative surface bonds: CO adsorbates on d-transition metal surfaces (somewhere between covalent and coordinative):
9 Covalent Bond Sharing of valence electrons (in pairs) between two atoms (usually non-metals) leads to a covalent bond between these atoms molecules single bond: two s-orbitals overlap to form a -bond double bond: C C two sp 2 -orbitals overlap to form a -bond two p-orbitals overlap to form a -bond triple bond: C C two sp-orbitals overlap to form a -bond four p-orbitals overlap to form two -bonds bond type length (pm) energy (kj mol -1 ) C-C C=C C C equal distribution of bonding electrons between atoms leads to non-polar bond (-) localization of bonding electron pair towards one atom (more electronegative) leads to polar bond ( + -Cl - ) extreme case: ionic bond
10 Covalent Bond: VB and MO theory VB theory: In the valence bond (VB) theory resonance energy is gained by exchange of electrons between two atoms (orbital overlap). Bonding electrons are localized between two bonding atoms and are not distinguishable. description of bonding geometries by hybrid orbitals: four C valence electron orbitals: 2s 2p x 2p y 2p z four C sp3 hybrid orbitals (tetrahedral): sp 3 (e.g. C 4 ) MO theory: In the molecular orbital (MO) theory bonding electrons are not localized between two atoms of a bond, but distributed in a group of molecular orbitals over the entire molecule. quantum mechanical description by the Schrödinger equation: MO = E MO MO are generated by a linear combination of atomic orbitals (LCAO): MO = c 1 + c 2 + c c n n wave function of MO: MO ; atomic orbital (AO): n ( ) 1s (-) antibonding bonding 1s ( ) MO theory is basis for computational treatment of molecular structure (semi-empirical, ab-initio) frontier orbitals OMO / LUMO
11 Ionic Bond ionic bonds are formed by strong Coulomb interactions between two oppositely charged species (e.g. Na + Cl - ) the potential energy varies with the distance r between the two ions by 1/r (the force varies with 1/r 2 ) description by formal electron transfer from newly formed cation (usually metals) to newly formed anion (usually non-metals) "simplest bond" / extreme case of polar bond ionic bond is not localized / directed, but acts isotropically / radial-symmetrically around ions leads to extended aggregation and ionic crystals with one cation being surrounded by many anions and vice versa etc D
12 Metallic Bond metallic bond: attractive interactions / bonds in metals are mediated by free moving valence electrons (electron sea) between positively charged atoms over entire sample - electron sea: high electron mobility good thermal and electrical conductivity - metallic bond is weak (compared to covalent bond) ductile metals theoretical description of metallic bond by band theory:
13 Electrostatic Interactions The force F (Coulomb force) acting between two charges q 1 and q 2 separated by a distance r in vacuum ( 0 ) depends on the separation by 1/r 2. r q 1 q 2 F q 1 q 2 q 4 0 r 2 in medium F 1 q 2 with r 4 0 r r 2 (relative permittivity, dielectric constant) F / V F=1/r 2 V=1/r the electrostatic forces are additive: in a system of many charges the force on a single charge is obtained by summing all the interactions with the other charges - electrical work w e : potential energy V: w e or V r Fdr q 1 q r r r - electric potential: q r r w e or V = q 1 - electric field strength: E q r r 2 F = q 1 E
14 van der Waals Interactions Collection of attractive interactions between molecules based on dipole / dipole, dipole / induced-dipole, and induced-dipole / induced-dipole interaction (Keesom, Debye, London dispersion energies) dipole moment : equal charge q separated at a fixed distance r = q r -q +q r unit: debye (D) = C m induced dipole i : dipole induced in a polarizable molecule by electric field i = E - + : polarizability E : electric field E
15 Dipole / Dipole Interactions Interaction of freely rotating dipoles (liquid) depends on the thermal energy (kt) and is referred to as Keesom energy (Boltzmann distribution of orientations). preferred over 2 V 2 3 kt r 6 At 25 C the average interaction energy for pairs of molecules with µ = 1 D is about -1.4 kj mol -1 when the separation is 0.3 nm. The average molar kinetic energy at 25 C is 3/2 RT = 3.7 kj mol -1.
16 Dipole / Induced-Dipole Interactions A dipole near a polarizable molecule induces a dipole (charge dislocation) in the neutral molecule leading to an attractive interaction, the corresponding potential energy is referred to as Debye energy. µ - + ' V equal to 2 ' r ' is the polarizability volume given by ' = / 4 0 (unit: cm 3 ) The interaction energy is independent of the temperature because the induced dipole follows immediately the motion of the permanent dipole and is thus not affected by thermal motion, and it depends on 1/r 6 (like the dipole / dipole interaction). For a molecule with µ = 1 D (e.g. Cl) near a molecule with polarizability volume ' = cm 3 (e.g. benzene) the average interaction energy is about -0.8 kj mol -1 at a separation of 0.3 nm.
17 Induced-Dipole / Induced-Dipole Interactions Random fluctuations in a polarizable molecule lead to a temporary dipole which induces a corresponding dipole in a nearby molecule, leading to attractive dispersion interactions. The involved potential energy is called the London dispersion energy. parallel orientation anti-parallel orientation ' V I 1 I 2 3 r 6 I 1 I ' 2 ' r 6 I 1 I 2 I 1 I 2 I n is the ionization energy, with I = h, is the electronic absorption frequency In the case of two methane molecules with ' = cm 3 and I = 7 ev the dispersion energy becomes -5 kj mol -1 for a separation of 0.3 nm (comparable to the enthalpy of vaporization of methane vapor = 8.2 kj mol -1 ).
18 van der Waals Forces Between Macroscopic Objects The van der Waals forces between two macroscopic bodies can be calculated (as approximation) by integrating over the molecular / atom-atom vdw pair potential ( w(r) = -C / r 6 ) of all molecules / atoms in one body with all molecules / atoms in the other body. interaction free energies are expressed in terms of the amaker constant: A = 2 C 1 ~ J (in vacuum) with 1/2 being the atom density of body 1 / 2, C is the coefficient in the molecular / atomatom pair potential D
19 ydrogen Bonding highly polarized bond of hydrogen with heteroatom (e.g. -X - - +, X = O, N, F) provides strong protonic character to hydrogen (proton donor) can interact with electron donating group / atom / electron lone pair (proton acceptor) -mediated "bond" elongation of bond in -donor very short distance of and electron donor (-acceptor) for 2 O: O- = 0.10 nm, O... = nm, theoretical vdw radius O/ = 0.26 nm -bonding in 2 O: particular structure of ice hydrophobic effect (restructuring of -bonding network around hydrophobic solute is entropically unfavorable)
20 ydrogen Bonding: Proteins ydrogen bonding of the amide groups via N-...O=C leads to secondary and tertiary structures of proteins: - -helix (chiral, tubular structure) - -pleated sheet (extended flat structure) -pleated sheet a-helix
21 ydrogen Bonding: DNA The base pairing in the DNA double helix is mediated by hydrogen bonding between the nucleic acid moieties: - 2 -bonds between adenine and thymine - 3 -bonds between guanine and cytosine
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