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Molecules


Contents

Quantum Theory, Blackbody Radiation
Correspondence Principle
Uncertainty Principle
Complemetarity Principle
Exclusion Principle
Path Integral, Transition to Qunatum Theory
First Quantization, Schrodinger Equation
Quantum Interpretations
Hydrogen Atom
Covalent Bond, Hydrogen Molecule
Ionic Bond, Atomic Shells
Hydrogen Bond, Molecular Orbital
van der Waals Force, Dipole-Dipole Interaction
Physical Chemistry
Inorganic Chemistry
Organic Chemistry
Soft Matter
Nano-technology
The Future of Chemistry
References
Index

Quantum Theory1,2, Blackbody Radiation

Molecules are small objects not susceptible of direct observation even under the most powerful microscope. However, their properties can be deduced indirectly from experiments. These objects are different on the conceptual level as well. Classical physics can no longer offer a consistent description. It is replaced by quantum theory, which describes the objects only in term of probability, energy levels, and other quantum numbers. A well-defined orbit such as the path of a planet around the Sun becomes the probability of finding the object at a certain location in the microscopic world. Thus, all the illustrations related to these objects would be just a schematic diagram conveying some ideas, they should never be taken literally as the real thing.

Blackbody Radiation Historically, the quantum theory began with the attempt to account for the discrepancy between the theoretical and observational blackbody radiation. The classical theory of Rayleigh-Jeans failed to fit the observation of the radiation energy distribution from a blackbody at high frequency. In searching for a modification that would reduce the contribution of the high frequencies to the energy, Planck was led to make an assumption: The energy of the radiation with frequency is restricted to integral multiples of a basic unit hv (a quantum), i.e., E = nh where h = 6.625x10-27 erg-sec is the Planck constant and n is an integer. With this assumption, Planck obtained an exact fit to the observed distribution of radiation energy. According to classical theory, electromagnetic radiation is a wave phenomenon. The Planck's assumption endows a particle aspect to the same entity. Such wave-particle duality requires radical changes in the fundamental concepts of the properties of matter and energy. An introduction on the subject of "wave" can be found in the appendix: Wave, Sound, and Music.

Figure 12-01 Blackbody Radiation

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Correspondence Principle

The first difference is that whereas classical theory always deals with continuously varying quantities, quantum theory must also deal with discontinuous or indivisible processes (e.g., the unit of energy packed in a quantum). The second difference is that whereas classical theory completely determines the relationship between variables at an earlier time and those at a later time, quantum laws determine only probabilities of future events in terms of given conditions in the past.

The Correspondence Principle states that the laws of quantum physics must be so chosen that in the classical limit, where many quanta are involved (e.g., n is a large integer in E=nh), the quantum laws lead to the classical equations as an average. This requirement combined with indivisibility, and incomplete determinism define the quantum theory in an almost unique manner.

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Uncertainty Principle

The Uncertainty Principle is derived from three elements: the wave-particle duality, the indivisibility of energy and momentum transfers, and the lack of complete determinism. It states that for a pair of conjugate variables such as position/momentum
Uncertainty and time/energy (including the rest mass energy mc2), it is impossible to have a precisely determined value of each member of the pair at the same time. This statement is illustrated with a schematic diagram in Figure 12-02. The corresponding formula is: x px > , where denotes the uncertainty, x is the position of the point mass m along the x-axis, px = m vx is the momentum along the x-axis, vx is the velocity along the x-axis, and = h/2 = 1.054x10-27 erg-sec. A similar relation exists for the uncertainty of the time t and energy E, e.g.,

Figure 12-02 Uncertainty Principle [view large image]

t E > . In case of heavy mass (such as a macroscopic object), the uncertainties and thus the quantum effect becomes very small, classical physics is applicable once more.

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Complemetarity Principle

According to the uncertainty principle, the pair of conjugate variables such as the position and momentum of a particle is not well defined but exist only as opposing potentialities. These potentialities complement each other, since each is necessary in a complete description of the physical processes through which the particle manifests itself. This is referred as "principle of complementarity". The more general statement reads: At the quantum level, the most general physical properties of any system must be expressed in terms of complementary pairs of variables, each of which can be better defined only at the expense of a corresponding loss in the degree of definition of the other. In particular, particle and wave can be considered as one of those complementary pairs - no experiment can reveal both at once.

However, one experiment seems to contradict this principle. As shown in Figure 12-03g, the apparatus is similar to the
Matter and Wave "double-slit" experiment, but with a lens on the far side of the pinhole screen. The lens refocuses the spreading beams onto two mirrors, which reflect them onto two photon detectors tracking the path of the photons as particles. The interference pattern (wave property) is observed indirectly by placing wires in front of the lens at the "would be" positions of the dark fringes. It is argued that if the photons do not interfere, there will be no dark fringes and the wires will block some of the photons hitting the lens, reducing the photon count at the detectors. Since no such dip in the signal is seen, it implies that the light does form an interference pattern, violating the complementarity principle. Such claim has

Figure 12-03g Particle and Wave [view large image]

raised a storm of criticism initially in 2004, but the publication of the research in 2007 has forced a more cool-headed discussion now.

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Exclusion Principle

Exclusion Principle The Pauli Exclusion Principle states that identical fermions -- one type of fundamental matter with 1/2 integer spin quantum number -- cannot be in the same place at the same time and with the same orientation (i.e., cannot have the same quantum state). It is this Exclusion Principle that requires the electrons in an atom to occupy different energy levels instead of all congregating in the lowest energy level. Chemistry would be very different without this rule. The exclusion principle is also responsible for the degenerate pressure, which prevents the White Dwarf from complete collapse. The other type of matter, bosons (particles with integer spin quantum number), do not have this property. The boson gas can form Bose-Einstein condensate near absolution zero temperature. They are all in the same quantum state, and behave like a single entity. Figure 12-04 shows the bosons bunch together, while the fermions keep their distance at temperature a few hundreds billionths of a degree above absolution zero (nanoKelvin=nK). Superfluidity refers to frictionless flow of spin 0 boson, e.g.,

Figure 12-04 Fermions and Bosons

helium-4 at low temperature.

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Path Integral3, Transition to Quantum Theory

The transition from classical to quantum in theoretical physics is most elegantly prescribed by path integral. According to classical physics the movement from "here" at time t1 to "there" at time t2 in Figure 12-05 is through the shortest path (the dash line) in evaluating the Action. In quantum theory all paths are possible. Each possible route corresponds to a "history".
Path Integral Each history has associated with it a number, called the amplitude, which defines the probability of that particular path being followed. While the classical path (the dash line) occurs with higher probability, the probability for the other paths vary according to a weighting factor. The probability of going from "here" to "there" is the sum of the probability for all paths. This formulism was originally devised by Richard Feynman for his PhD thesis in early 1940s. Twenty years earlier the transition from classical to quantum had to be formulated with a postulation which can be shown to be equivalent to the method of path integral (see mathematical detail).

Figure 12-05 Path Integral
[view large image]

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First Quantization, Schrodinger Equation4

It was postulated that the momentum p and position q are no longer mere numbers but are operators satisfying the commutative relation:

(qp - pq) = i.

This is called the canonical quantization. The fact that the particle is endowed with wave property is referred to as first quantization. Actually only p is treated as an operator - a differential operator acting on the wave function (q), q remains to be a c-number. The commutative relation can be viewed as a mathematical statement for the Uncertainty Principle. Since it implies that p cannot be a function of q (because it would mean p and q can be determined precisely at the same time), p can be related to q only in the form of an operator such as - i d/dq, where i = . The commutative relation is the direct result of such interpretation. Application of this rule for p and q to the equation relating the total energy E to the kinetic energy p2/2m and the potential energy V(q), e.g., E = p2/2m + V(q), yields the time-independent Schrodinger Equation for one particle with mass m and interacting potential V (i.e., it describes the stationary states with well-defined energy E corresponding to E 0, and t in the uncertainty relation t E > ) :
Schrodinger Equation
For a given interacting potential V the problem is to find the Energy E and the corresponding wave function . The wave function is the probability amplitude of finding the particle at certain position (again do not confuse this amplitude with the state vector amplitude in superposition). The absolute square of the amplitude is the probability density. It turns out that the imaginary factory i in the quantization of p is crucial in describing a waveform for the case of E > V; otherwise, will be just an exponential function not compatible with observation. This form of Schrodinger Equation can be used to find out the structure of the atom or molecule. However, the generalization to system of many particles and more than one source of interaction becomes rapidly un-manageable and is solvable only through methods of approximation. The Schrödinger Equation for a poly-atomic molecule with N atomic nucleus and n electrons can be written down as :

{(2/2)[(/m) + (/Mk)] + E - (e2)[(1/2)(1/|ri - rj|) - (Zk/|ri - Rk|) + (1/2)(ZkZl/|Rk - Rl|)]} = 0

where m is the mass of electron, Mk is the mass of the kth atomic nucleus with number of positive charge Zk, E is the total energy of the system, and . Since the atomic nucleus move much slower than the electrons, the Born-Oppenheimer approximation can be adopted to separate the wave function into = electrons nuclei and the resulting equations are solved separately - the part for the electrons yields the electronic configuration while the vibrational and rotational states (of the nuclei) are obtained from the nuclear part. This method makes the equation more or less solvable but the task is still formidable with increasing number of particles. The Molecular Orbital Theory is used further to alleviate the computational difficulty in calculating the molecular structure (the nuclear part).

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Quantum Interpretations

In its January 22-28, 2011 issue, "NewScientist" has an article about various quantum interpretations with current status (as listed in Table 12-01 below). Only the most popular ones are included. The others with status such as uncertain, endangered, rare, highly contentious, and popularity limited, are left out.

Interpretation Feature Status
Copenhagen Measurement plays a key role in changing quantum states Healthy
Hidden Variables Hidden variables carry missing information about quantum states Challenged
Many Worlds All quantum possibilities play out in a multiplicity of universes Healthy
Penrose Outcome of experiments is a result of gravitational interactions Under investigation

Table 12-01 Status of Various Quantum Interpretations

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Hydrogen Atom5,6

Beside some idealized cases, analytical solution of the Schrodinger equation can be obtained only for hydrogen atom which has one electron with mass m, and charge e moving about an atomic nucleus. The energy levels are given by:

En = - me4 / (3222n2) = - 13.6 / n2 ev

where n is any integer from 1 to . Some of the energy levels are shown in Figure 12-07a while the probability density corresponding to different quantum states are shown in Figure 12-07b where n, l, and m are the total, orbital, and magnetic
Energy Levels Probability Density quantum number respectively; the probability densities have either spherical symmetry or rotational symmetry about the z axis. When the electron jumps from a higher energy level En+1 to a lower one En, a photon with frequency = (En+1 - En)/h is released (see the atomic transition series in Figure 12-07a). Excitation is the reversed process when the electron in energy level En absorbs a

Figure 12-07a Energy Levels
[view large image]

Figure 12-07b Probability Density [view large image]

photon with frequency . Incidentally, the semi-classical Bohr model of H atom can also account for such H atom structure as well. The theory
portrays the electron moving around the atomic nucleus similar to the Sun-Earth system but imposed a condition that the electron wave closed on itself to become standing wave.

The state of the electron in an atom is specified by four quantum numbers. The principal quantum number n determines the energy level; its value runs from 1, 2, 3, ... For each n, the orbital quantum number l = 0, 1, 2, ... (n-1); it is related to the magnitude of angular momentum. Then for each l, the magnetic quantum number m can be -l, -l+1, ...l-1, l; it is related to the z component of the angular momentum (see Figure 12-07a). The spin quantum number s is either +1/2 or -1/2.

For n = 1, l = 0, m = 0, there is only 2 possible quantum states for the electron, with s = +1/2 and -1/2 respectively.
For n = 2, l = 0, m = 0 and l =1, m = -1, 0, +1; there is a total of 2 + 6 = 8 possible quantum states. Therefore, it requires 2 electrons to complete the shell for n = 1, and 8 electrons to complete the shell for n = 2, ...and so on (see Table 13-01 in Topic Atom). The orbital quantum number l is often designated by a letter, s for l = 0, p for l = 1, d for l = 2, and f for l = 3 ...

The quantum number l is non-additive, (e.g., two of the quantum numbers l1, l2 are added as vectors, they can take on the values of l1+l2, l1+l2-1, ..., |l1-l2| ) while m is additive (e.g., m' = m1 + m2 only) and relates to an Abelian group (e.g., the two dimensional rotation about the z-axis). States having the same non-additive quantum numbers but differing from each other by their additive quantum numbers are said to belong to the same multiplet. The number of members of a multiplet is called its multiplicity. For a given multiplet l the multiplictiy is equal to 2l+1.

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Covalent Bond, Hydrogen Molecule7

H2 Wave Function Potential Curve When two hydrogen atoms approach each other, the final configuration depends on the spin of the two electrons (a consequence of the Exclusion Principle). If the spin of the two electrons is parallel as shown in the right side of Figure 12-08, the two atoms remain separated. However, if the spin of the two electrons is antiparallel as shown in the left side of Figure 12-08, the two atoms combine to form a hydrogen molecule. There is a high probability

Figure 12-08 H2 Wave Function
[view large image]

Figure 12-09 H2 Potential Curve [view large image]

of finding the electrons in between the atomic nuclei and this "electron cloud" tends to keep them from breaking up. This kind of binding is
called covalent bond, and is purely a quantum effect. Figure 12-09 shows the electronic energy as a function of inter-nuclear separation. It is usually referred to as potential curve. The potential curve can be derived either theoretically from the numerical solution of the Schrodinger equation or experimentally by analyzing the spectroscopic data. The potential curve UA is repulsive while US forms a potential well to keep the atomic nuclei within unless they absorb a quantum of light with energy more than the dissociation energy of 4.52 ev.

In presenting the potential curve for a diatomic molecule, one of the atomic nucleus is usually fixed at the origin of the coordinate frame. The other nucleus is then portrayed as vibrating and rotating inside the potential well as shown in Figure 12-10a. The vibration is restricted to discrete energy levels. Each of the vibrational energy level v is further split into a series of rotational energy levels J called vibrational band. Wave functions are shown in two vibrational energy levels in Figure 12-10b. According to classical physics, particle cannot penetrate the potential wall; however, in quantum there is a certain probability of infiltration (tunneling) outside the wall (see Figure 12-10b). In general, transitions are favored by superimposing an initial
Energy Levels Transition configuration of high probability with a final one of high probability as shown by the green line in Figure 12-10b. Transitions are also governed by selection rules, which usually allow transitions to occur only between change of the rotational or vibrational quantum number by an amount 1. The former is related to the initial and final states of the molecule, which favors the one step change in the rotational configuration. While the latter is linked to the oscillating state of the molecule, which occurs only at certain resonant energy so that the emitting or absorbing photon can carry only

Figure 12-10a Vibrational and Rotational Energy Levels [view large image]

Figure 12-10b Transition [view large image]

that amount - one step at a time.


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Ionic Bond8, Atomic Shells

Atomic Shells The most stable electron configuration of an atom consists of closed shells -- 2 for the n =1 shell; 8 for the n = 2 shell; ... (See Figure 12-11.) Thus He with 2 electrons and Ne with 10 electrons are among the most stable chemical elements. Atoms with incomplete outer shells tend to gain or lose electrons in order to attain stable configuration, becoming negative or positive ions in the process. For example, it requires 5.1 ev to ionize (remove) the outer shell electron from the sodium (Na); while adding an electron to the incomplete shell of chlorine (Cl) releases 3.8 ev. Thus the formation of a Na+ ion and a Cl- ion by the donation of one electron of Na to Cl requires just 5.1 - 3.8 = 1.3 ev.

 Figure 12-11 Atomic Shells [view large image]

Ionic Bond Figure 12-12 shows the decrease in potential energy as the Na+ and Cl- ions approaching each other. For very small separation of the ions, however, there is a strong repulsion due to the Exclusion Principle. The minimum in the potential curve occurs at r = 0.24 nm. At this separation the mutually attractive and repulsive forces on the ions exactly balance, and the system is in equilibrium with the creation of an ionic bond. To dissociate a NaCl molecule into Na and Cl atoms requires an energy of 4.2 ev, breaking it up into Na+ and Cl- ions requires an additional energy of 1.3 ev.

 Figure 12-12 Ionic Bond
[view large image]

Table 12-02 below shows the differences between ionic and covalent compounds.

Property Ionic Compounds Covalent Compounds
Elements metal - nonmetal nonmetal - nonmetal
Phase (at STP) solid (in crystal lattice) solid, liquid or gas
Hardness hard and brittle (salt) brittle and weak (sugar)
or soft and waxy (butter)
Melting/Boiling Points high low
Solubility mostly soluble in water solubility varies widely
Electrical Conductivity solid - nonconductor,
liquid or aqueous solution - conductor
insulators

Table 12-02 Properties of Ionic and Covalent Compounds

Note: STP - standard conditions of 0oC temperature and 1 atmospheric pressure (= 14.7 lb/sq-in = 101 kpa).

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Hydrogen Bond9, Molecular Orbital10

Orbitals Orbital Energy Levels It becomes very difficult to solve the Schrodinger equation numerically for molecule with many electrons. An approximate method called Molecular Orbital Theory (MO for short) has been developed for constructing reasonably accurate molecular structure (the wave functions and energy levels) with reasonably computational time. The MO starts with a linear combination of the wave functions for the electrons of each atom as shown in the left side of Figure 12-13a. The energy of the system is minimized with respect to the coefficients of the linear combination at different inter-atomic separation. The final result

Figure 12-13a Orbitals [vli]


Figure 12-13b Orbital Energy Levels [view large image]


yields the wave functions (probability amplitude) for the molecule as shown in the right side of Figure 12-13a as well as the molecular energy levels as shown in Figure 12-13b. The isosurface shown in Figure 12-13a is called atomic or molecular orbitals. It is defined as the surface
within which the probability of finding the electron has some definite value, say 90%. The molecular orbital designated with an " * " is the unstable antibonding state, otherwise, it is the stable bonding state. The + or - sign signifies a positive or
N<sub>2</sub> Orbital Image N<sub>2</sub> Orbital Calculated negative value for the wave function. Each orbital can accommodate two electrons with opposite spin direction. Recently (in 2005), a method has been developed to take image of a molecule by using a short laser pulse lasting just 3 x 10-14 second. Figure 12-14a shows a electron orbital of a nitrogen molecule as imaged by such technique. It agrees quite well with the orbital as calculated from theoretical models (Figure 12-14b). The colours represent the amplitude of the wave function - the electron is most likely to be found at the red and dark blue areas. Producing a three-dimensional image requires repeating the process at different angles, like a hospital CT scanner.

Figure 12-14a N2 Image [view large image]

Figure 12-14b N2 Model

H2O Energy Levels Hydrogen Bond In the H2O molecule, the electric field around the oxygen atom is stronger than that around the hydrogen. The electrons from the hydrogen atoms are drawn close to the oxygen. This leaves the hydrogen atoms positively charged at one end. The four pairs of valence electrons around the oxygen atom (six contributed by the O atom -- 2 in the 2s, 4 in the 2p states; and one each by the H atoms in the 1s state) occupy four sp3 orbitals that form a tetrahedral pattern. The energy levels for these four pairs of electrons are lower than the original levels in

Figure 12-15a H2O Energy Levels [view large image]

Figure 12-15b Hydrogen Bond [view large image]

separated atoms as shown in Figure 12-15a (MO1 - MO4). Since the positively charged atomic nucleus for the hydrogen is partially exposed, it often attracts to
other negatively charged orbitals such as the electron pairs of the oxygen atom in another H2O molecule (see Figure 12-15b).
Water This is called hydrogen bond. It is different from the covalent bond since there is no orbital overlap; it is not an ionic bond since there is no charge transfer from one atom to another. The strength of the hydrogen bond is about 10 times weaker than the covalent and ionic bonds. Hydrogen bonds are important in fixing properties such as solubilities, melting points, and boiling points, and in determining the form and stability of crystalline structures. Molecules

Figure 12-16 Water
[view large image]

such as water carrying hydrogen bonds are called polar molecules. They play a crucial role in biological systems.

    Water has some special properties crucial to the existence of life courtesy to the hydrogen bond:

  1. Heat Capacity - Water has high heat capacity (needs more heat to rise the temperature) and boiling point by virtue of the additional hydrogen bonds that keep the water molecules packed together with extra strength (see Figure 12-16a, white bar represents covalent bond, grey and blue bars for hydrogen bond). This property moderates the temperature of the environment. Lack of water turns the land into desert. The same hydrogen bonds also pull water up a tree, in a phenomenon called capillary action, and maintain surface tension, which enables small bugs to walk on water.
  2. Ice - When water cools to below 4oC, it suddenly becomes less dense. It is because the thermal agitation cannot overcome the hydrogen bonds and solid ice begins to form. The angle subtended by the two hydrogen atoms then increase from 105 to 109 degrees resulting a less tightly packed configuration (Figure 12-16b). That's why ice can float on water and protects the water beneath from frozen allowing fish to live in the polar regions or creatures under the icy surface of Europa (Figure 12-16f).
  3. Solution - Water is a good solvent able to dissolve many polar substances (Figure 12-16c). That's why water-based liquids, like blood, are perfect transporters of essential substances such as salt, sugars and hormones.
  4. Protein folding - Some amino acids are hydrophobic (repelled by water); while others are hydrophilic (attracted to water). In a a liquid environment such as the inside of cells, these properties dictate how a protein "assembles", or folds (Figure 12-16d). DNA too, depends on water. Experiments have shown that the double helix would fall to pieces without water. This is because water molecules help form hydrogen bonds between DNA's phosphate groups.
  5. DNA binding site - Some biochemists think that water molecules may play an active role in guiding enzymes to certain spots on the DNA (Figure 12-16e). It is found that water molecules spend more time around certain areas of DNA when cell divides. Such tendency seems to suggest that water is needed for the expression of genes - a process that is kick-started by binding the transcription factor to the gene switch.
  6. Origin of Water on Earth - Water molecules are one of the components in interstellar dust. It would be incorporated into the primordial Earth naturally. Water as many other gaseous materials are trapped by the Earth's gravity when it acquired a sufficient amount of mass. It might be in the form of solid when the temperature was too low in the very beginning, and in the form of gas when it was covered with magma produced by planetesimal impacts. Only in a very narrow window of temperature (from 0oC to 100oC) it turned into liquid state suitable for life. Later on more water are added via the impacts of comets, which contain a lot of water and the impacts occurred more often in the past.
  7. Search for ET - All known life on Earth depends on water. Typical enzymes, just like DNA, need to be surrounded by water to function properly. Nobody know if enzymes can function in another liquid, or there might be fundamentally different life-forms in other parts of the universe - a possibility that would not be ruled out by many scientists. Nevertheless, NASA has chosen the strategy of "Follow the Water" in its programs to search for extra-terrestrial life (to Europa for example, see Figure 12-16f).

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van der Waals Force11, Dipole-Dipole Interaction

All atoms and molecules -- even inert-gas such as those of helium and argon -- exhibit weak, short-range attractions for one another due to van der Waals forces. These forces are responsible for the condensation of gases into liquids and the freezing
Van der Waals Interaction Van der Waals, Nonpolar of liquids into solids. Such familiar aspects of the behavior of matter in bulk as friction, surface tension, viscosity, adhesion, cohesion, and so on also arise from van der Waals forces. The interaction is between dipole-dipole. It can be the interaction between a permanent and an induced dipole as shown in Figure 12-17 or between a time average dipole (due to fluctuations of charge) and an induced dipole as shown in Figure 12-18. The van der Waals interaction is about 10 times weaker than hydrogen

Figure 12-17 van der Waals Interaction [view large image]


Figure 12-18 van der Waals, Nonpolar
[view large image]

bond. The stronger hydrogen bond can be considered as interaction between permanent dipoles.


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Physical Chemistry

Before the development of high energy physics, it has been found convenient to divide natural phenomena into two broad classes: one consists of changes of an apparently permanent nature involving the transformation of one form of matter into another, while in the second are included temporary changes, general resulting from an alteration of external conditions. It is the study of the phenomena in these two categories, which constitute the sciences of chemistry and physics, respectively. The distinction between these aspects of the study of nature may be indicated in another way: chemistry may be said to deal with matter and its transformations, whereas physics is concerned with energy and its transformations. It is clearly not possible to draw a sharp distinction between the two points of view, for many problems in both physics and chemistry are concerned with interactions between energy and matter; it is these problems which constitute the fundamental basis of the subject of physical chemistry.

Followings are some selected topics in physical chemistry. Most of the phenomena were described originally from the macroscopic point of view. The microscopic interpretation is available only after the discovery of atomic structure. The modern subjects in physical chemistry such as quantum chemistry, and statistical mechanics take the microscopic point of view. They are presented elsewhere in this website (click the underlined subject above to see more).

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Inorganic Chemistry12

Inorganic chemistry is the branch of chemistry concerned with the properties and reactions of inorganic compounds. This includes all chemical compounds without the chains or rings of carbon atoms, which are termed organic compounds. Followings are some basic concepts of inorganic chemistry:

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Organic Chemistry


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Soft Matter

Soft matter is a subfield of condensed matter that is most imtimate to our daily life. Its predominant physical behaviors occur at an energy scale comparable with room temperature and therefore easily deformed by thermal stresses or thermal fluctuations. Soft matter is a misnomer because many materials in this class are not soft to the touch. It is better defined as
Soft Matter Length Scale "mesoscopic matter" since the size of the basic constituents ranges from a few nano-meters to about one micro-meters (Fiugre 12-35a) - at the boundary between quantum and classical objects (Figure 12-35b). It is the properties and interactions of these mesoscopic structures that determine the macroscopic

Figure 12-35a Soft Matter
[view large image]

Figure 12-35b Length Scale
[view large image]

behavior of the material; the quantum effect in the atomic or molecular scale are unimportant. Some examples for the soft matter are listed below.
Vesicle Emulsion
  • Micelles, Vesicles, and Emulsions -
    • Micelle is an aggregate of surfactant molecules dispersed in liquid. Surfactant is a class of organic chemicals call amphiphiles, which has a hydrophilic (water loving) head and a hydrophobic (water hating) tail (see surfactant for more detail).

Figure 12-35e Vesicle
[view large image]

Figure 12-35f Emulsion
[view large image]

    • Vesicle is a double layers sphere made from surfactant molecules with the hydrophilic heads facing the aqueous solutions on the outside and inside (Figure 12-35i).
Most vesicles have specialized functions depending on what materials they contain. For example, the living cell contains vesicles called Endoplasmic reticulum, Golgi complex, and Lysosomes for processing foods and removing wastes. The cell membrane is also a form of vesicle.
Emulsion Examples
    • Emulsion is formed from two immiscible liquids that do not separate readily as shown in the middle of Figure 12-35f. It is created when energy is added to the mixture (by shaking for example). Some emulsions like milk are quite stable and will take a long time to separate since the nano-size particles is small enough to be suspended by brownian movement. Others may part quite quickly like the salad dressing of oil and vinegar (figure 12-35g). The emulsion itself consists of small droplets of one liquid within the body of a second liquid. Emulsions can fail in four basic ways: (i) Coalescence is the forming of bigger spheres until the two liquid are separated completely. (ii) Flocculation is the forming of clumps instead of larger spheres. (iii) Creaming is for the less dense liquid to float to the top. (iv) Breaking is the combined action of coalescence and creaming (see Figure 12-35g).

Figure 12-35g Emulsion Examples [view large image]

Liquid Crystal Phase Liquid Crystal Examples
  • Liquid Crystals - Liquid crystals are in the "meso-phase" between solid and liquid. The transition can be induced by temperature (thermotropic) as shown in Figure 12-35h or by dissolving the material in a liquid. Liquid crystals have the ability of in a form of orderly orientation but yet are in dynamic motion. Such special property is the result of structural anisotropy, e.g., rod-shape (calamatic), disc-shaped (discotic), and board-like (sanidic), and forced alignment by interaction

Figure 12-35h Liquid Crystal Phase
[view large image]

Figure 12-35i Liquid Crystal Examples [view large image]

between the molecules. Actually, in the meso-phase the 3-dimensional ordering has been reduced to 1 or 2-dimensional ordering (Figure 12-35h). Figure 12-35i shows the various types of liquid crystals.

LC Display Liquid crystals find wide use in liquid crystal displays, which rely on an electric field to control its orientation. Polarization of the light depends in turn on the orientation so that it is either blocked or transmitted by a second polarization filter (polarizer) perpendicular to the first one (Figure 12-35j). The liquid crystal in this application is usually the nematic type (rod-shaped) in twisted form at relaxing state.

Figure 12-35j LC Display

Legend for Figure 12-35j: L - light, P1 - horizontal polarizer, P2 - vertical polarizer, E1, E2 - electrodes, LC - liquid crystals, G -grid, V - voltage supply, S - switch, I - image.

Biomolecules Organic Compounds
  • Biomolecules - The biomolecuels of life is made from organic compounds, but not all organic compounds are related to life. Figures 12-35k and 12-35l happen to show the same thing with different perspective. In general the biomolecules in a living system are more complicated. For examples:

    1. In the case of protein, it is not simply a polymer but a more complicated polymer makes from 20 different kinds of monomers (the amino acids). Every specific amino acid sequence gives a unique shape, and this in turn gives the molecule a single, well-defined function.

Figure 12-35k Bio-molecules

Figure 12-35l Organic Compounds [view large image]

2. DNA and RNA are also polymers made from nucleotides (the monomers). In a biological system the combination of the mono-mers cannot be at random. It has to be very specific and coiled up into chromosomes, otherwise the organism would not survive.
3. The photosynthesis in plants generates a simple CH2O molecule, which joins together to form the 5-carbon fructose (ribose) and 6-carbon glucose. These two kinds combine to give us the table sugar - the sucrose or disaccharide. More linkages of the glucose molecules would produce polysaccharides. There are three common polysaccharides in organisms: starch, glycogen, and cellulose. Glucose is the basic energy source in cells. Starch and glycogen are storage form of glucose in plant and animal cells, respectively, and cellulose is found in plant cell walls. Plants also possess other pathways to turn glucose into protein, lipid, and nucleotide.

4. The monomers in a cell's membrane are lipids, which form a kind of vesicle as mentioned earlier. However all kinds of opening (each guarded by special protein) are inserted over the surface for transporting materials in and out of the cell.

5. Polymer or surfactant solutions can form liquid crystal structures too (called lyotropic). Tobacco Mosaic Virus is an example of a biological material forming lyotropic liquid crystals at rather low concentration because the virus has a very elongated shape. See a long list of biomolecules on a Wikipedia website.

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Nano-technology

Traditionally, systems of interest to physicists have been divided into the macroscopic and the microscopic realms, where the latter implies atomic and molecular sizes or smaller. Recently, research in the intermediate (mesoscopic) domain has
Nano Domain achieved significant scientific successes. This field is characterized by the need to use the microscopic laws of quantum mechanics, while, on the other hand, the samples can be made and operated by essentially ordinary macroscopic methods. This involves linear size scales from a few to thousands of atoms, and reliable fabrication and analysis methods exist down to the scale of about fifty atoms. The term "nano" usually denotes the low end of this range. Figure 12-36a shows (left) scale of 10 micron with a circuit board element

Figure 12-36a Nano Domain
[view large image]

comparing to a human hair, and (right) 0.1 micron, where a small stat-of-the-art transistor is compared with one commercially available in 2001.

STM Methods based on extremely powerful scanning tunneling microscope (STM, Figure 12-36b) that allows control of both fabrication and analysis on the scale of single atoms are being developed. Controlling man-made molecular structures on the level of individual atoms (including position and orientation) is possible in principle, and physical measurements such as that of the local (atomic scale) density of electronic states near an appropriate defect in a superconductor have been made. A variety of surface probes can measure, for example, the local electrostatic potential on a sample's surface with a resolution approaching 10 nm.

Figure 12-36b STM [view large image]

MBE There are two distinct approaches to manufacture small-scale devices. Microelectronics starts with a large system and then divides it, reducing its dimensions by a variety of well-controlled methods. For example, shapes are printed onto the surface of silicon, which is then etched away to make microscopic wheels or micromotors. The smallest feature capability that can be achieved, appear to be around the 10 nm scale. Other methods work with individual atoms to make even smaller objects. An example of such large-scale preparation of high-quality materials is provided by the MBE (molecular-beam-epitaxy) method (Figure 12-36c), which can be used to grow individual lattice layers and extra-thin metallic layers.

Figure 12-36c MBE
[view large image]

Note: The RHEED (Reflection High Energy Electron Diffraction) in Figure 12-36c involves a high energy beam (3-100keV) directed at the sample surface at a grazing angle. The electrons are diffracted by the crystal structure of the sample and then impinge on a phosphor screen mounted opposite to the electron gun. It is used to examine patterns on a surface.

Nanotube The graphite phase of carbon provides some interesting nano materials such as carbon nanotubes and buckyballs (Figrure 13-36d). Nanotubes are produced by rolling a layer of two-dimensional graphite, called graphene, into a hollow cylinder parallel to the z axis and having a nanmeter-scale diameter. Graphene is a poor conductor, but the nanotube becomes metallic or semiconducting depending on the details of how exactly the graphene sheet is wound and connected to itself. Spherical fullerene (buckyball) contains 60 or 70 carbon atoms in the soccerball-like crystal of about 1 nm across. As of the early 21st century, the chemical and physical properties of fullerenes are still under heavy study. Fullerenes are not very reactive due to the stability of the graphite-like bonds, and are also sparingly soluble in many solvents. The buckyball has been used to run tests on determining the boundary between classical and quantum domains since its size is close to the transitional zone. Scientists are also working on building very small structures such as the nanorobot (Figure 12-36d), which can check out a patient's blood cells. The microgears were made by etching silicon in the same way as a microchip. Sixty of them would fit on the head of a pin.

Figure 12-36d Nano Objects
[view large image]

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The Future of Chemistry

Judging from the scant attention chemistry covered in the public media, it often evokes a perception that the time has passed for this branch of science. There is not much challenge left to attract bright young scientists into this field. Many chemistry departments are either closed or absorbed into other departments and renamed to something like "chemical biology" in
Future of Chemistry academic institutions. The strongly synthetic character of chemistry sets it apart from the "discovery" sciences such as physics, biology, astronomy and the Earth sciences. "Chemistry creates its object" as a French chemist wrote in 1860. The downside of this focus on making stuff is that chemists can be portrayed as inveterate tinkers - tweaking the molecular world to satisfy their curiosity, sometimes for fun and sometimes for profit. And it makes it especially hard to see where industrial chemistry ends and academic chemistry

Figure 12-37 Future of Chemistry [view large image]

begins. Recently in 2006, the Nature magazine asked many leading chemists what are the field's big questions. They have come up with six very important subjects in the arena of chemistry (Figure 12-37):
  1. How do we design molecules with specific functions and dynamic?
  2. What is the chemical basis of the cell?
  3. How do we make the materials needed for the future, in energy, aerospace or medicine?
  4. What is the chemical basis of thought and memory?
  5. How did life on Earth begin, and how and where might it begin on other world?
  6. How can we explore all the possible permutations of all the elements?
In this list, some items look suspiciously like industrial application, while the others can be categorized into interdisciplinary fields. As one chemist admits: there is no Holy Grail in chemistry; satisfaction comes from the chase, not the catch.

The year 2011 is designated as the International Year of Chemistry in honour of the 100th anniversary of Marie Curie receiving the Nobel Prize. The Nature magazine (6 January 2011) has listed ten priorities for the forthcoming decades by checking out ten leading chemists. Table 12-08 presents a summary of their choices.

Priority Brief Description Related Field(s)
Universal Science Base of all the innovations in the future Energy, public health, new materials
Better Living Fundamental to high living standard C, N, P cycles, energy-saving process
Greener Chemical Processes Chemical productions with minimal waste and hazard Minerals productions and substitutions
Production of polymers Mimic production of carbohydrate polymers in nature Bio-chemistry
Chemical self-assembly New and sophisticated ways to synthesize molecules Synthetic chemistry
Photosynthesis Replication Efficient, cheap and robust ways to mimic photosynthesis Bio-chemistry
Selective Interactions Greater control over inter-molecular interactions is required for the design of polymers Bio-chemistry, organic chemistry
Solar Power Generation of efficient photovoltaic material In plastics, paint or ceramics
Sustainable Living Development of energy, resources, ... to improve living standard Organic, inorganic, physical, polymer, material and bio chemistries
Catalyze Energy Production Development of better batteries, novel methods of energy production Material chemistry

Table 12-08 Ten Priorities in Chemistry


Scientific American (October 2011) does it a bit differently by listing 10 Unsolved Mysteries in Chemistry as summarized in Table 12-09 below :

Mystery Progress in Finding a Solution Prospect
How Did Life Begin? Theories on RNA world, clay catalysts, ... Testing of the theories in laboratory
How Do Molecules Form? Calculated structure for simple molecules Extension to more complicated molecules
How Does the Environment Influence Our Genes? Epigenetic marker can reactivate a gene via environmental influence Finding out the extent of the influence to reset the pluripotency of the cell
How Does the Brain Think and Form Memories? Memories are formed by increasing synaptic strength and growth of new synapses Finding out the process for memory recall
How Many Elements Exist? Synthetic elements created up to atomic number 118 Checking out the limit (if there's any) for super-heavy elements
Can Computers Be Made Out of Carbon? Graphene is excellent material for use in electronic circuitry Developing techniques for etching graphene circuits
How Do We Tap More Solar Energy? Experiment to mimic photosynthesis Finding an inexpensive catalyst
What Is the Best Way to Make Biofuels? Converting low-grade biomass (such as lignin and cellulose) into fuel Finding an inexpensive, efficient and easy to scale-up way
Can We Devise New Ways to Create Drugs? Picking out useful drugs from random assembly of molecules Finding better ways (such as using DNA as bar code) to pick out the useful drugs
Can We Continuously Monitor Our Own Chemistry? Some chemical sensors for detecting concentration of glucose (in the blood), ... etc. Developing new kinds of sensors (fast, cheap, sensitive) to detect contaminants, pollutants, pathogens (in bloodstream), ...

Table 12-09 Ten Unsolved Mysteries in Chemistry

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    References:

  1. Quantum Theory, Overview -- http://www.levity.com/mavericks/quantum.htm
  2. Quantum Theory, more detail -- http://www.srikant.org/core/node12.html
  3. Path Integral -- http://www.chem.unc.edu/lectures/2003Hermans/notes3/pathintegral.pdf
  4. Schrodinger Equation -- http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/schr.html#c1
  5. Hydrogen Atom, Schrodinger Equation -- http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/hydsch.html#c2
  6. Hydrogen Atom, Energy and Wave Functions -- http://www.kw.igs.net/~jackord/bp/i6.html
  7. Covalent Bond, Hydrogen Molecule -- http://hyperphysics.phy-astr.gsu.edu/hbase/molecule/hmol.html
  8. Ionic Bond -- http://207.10.97.102/chemzone/lessons/03bonding/mleebonding/ionic_bonds.htm
  9. Hydrogen Bond -- http://207.10.97.102/chemzone/lessons/03bonding/mleebonding/hydrogen_bonds.htm
  10. Molecular Orbitals -- http://www.chm.davidson.edu/ChemistryApplets/MolecularOrbitals/
  11. van der Waals Force -- http://207.10.97.102/chemzone/lessons/03bonding/mleebonding/van_der_waals_forces.htm
  12. Inorganic Compounds -- http://hyperphysics.phy-astr.gsu.edu/hbase/chemical/compound.html#c2
  13. Chemical Reactions -- http://boyles.sdsmt.edu/subhead/types_of_reactions.htm

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Index

Battery
Bell's inequality
Bose-Einstein condensate
Bosons
Casimir effect
Chemistry, future of
Complementarity Principle
Conjugate variables
Copenhagen interpretations
Correspondence Principle
Covalent bond, hydrogen molecule
de Broglie wavelength
Decoherence
Electrolyte
EPR paradox
Exclusion Principle
Fermions
First quantization, Schrodinger Equation
Hidden variables
Hydrogen atom
Hydrogen bond, molecular orbital
Inorganic chemistry
Ionic bond, atomic shells
Many worlds
Molecular Orbital theory
Orbitals
Organic chemitry
Oxidation
Path integral, transition to Qunatum Theory
Phase change
Physical chemistry
Planck
Potential curve
Probability density
Quantum interpretations
Quantum numbers
Quantum Theory, blackbody radiation
Reaction rate
Reality
Reduction
Schrodinger's cat
Surface tension
Solution
Thermochemistry
Uncertainty Principle
Vacuum
Valence
van der Waals force, dipole-dipole interaction
Wave
Wave function
Wave-particle duality


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