Learning Objectives

• To understand the correlation between bonding and the properties of solids.
• To classify solids as ionic, molecular, covalent (network), or metallic, where the general order of increasing strength of interactions.

Fluorine has the highest e-neg, SO HF will experience the strongest H bonding and needs the most energy to weaken the i.m.f. And boil The End. Chemical Bond A bond results from the attraction of nuclei for electrons All atoms trying to achieve a stable octet IN OTHER WORDS the p+ in one nucleus are attracted to the e- of another. Burdett the wavefunctions for the bonding and antibonding combinations are particularly simple. IJ, = 2+ (Vl+cp,) (17) 6, = 2-g ('PI-V.). All conjugated organic systems are open to an analogous treatment. The secular deter- minant for ally1 4, the three orbital problem, is just. Chemical Bonding and Molecular Geometry Figure 7.1 Nicknamed “buckyballs,” buckminsterfullerene molecules (C60) contain only carbon atoms. Here they are shown in a ball-and-stick model (left). These molecules have single and double carbon-carbon bonds arranged to.

Crystalline solids fall into one of four categories. All four categories involve packing discrete molecules or atoms into a lattice or repeating array, though network solids are a special case. The categories are distinguished by the nature of the interactions holding the discrete molecules or atoms together. Based on the nature of the forces that hold the component atoms, molecules, or ions together, solids may be formally classified as ionic, molecular, covalent (network), or metallic. The variation in the relative strengths of these four types of interactions correlates nicely with their wide variation in properties.

In ionic and molecular solids, there are no chemical bonds between the molecules, atoms, or ions. The solid consists of discrete chemical species held together by intermolecular forces that are electrostatic or Coulombic in nature. This behavior is most obvious for an ionic solid such as (NaCl), where the positively charged Na⁺ ions are attracted to the negatively charged (Cl^-) ions. Even in the absence of ions, however, electrostatic forces are operational. For polar molecules such as (CH_2Cl_2), the positively charged region of one molecular is attracted to the negatively charged region of another molecule (dipole-dipole interactions). For a nonpolar molecule such as (CO_2), which has no permanent dipole moment, the random motion of electrons gives rise to temporary polarity (a temporary dipole moment). Electrostatic attractions between two temporarily polarized molecules are called London Dispersion Forces.

Hydrogen bonding is a term describing an attractive interaction between a hydrogen atom from a molecule or a molecular fragment X–H in which X is more electronegative than H, and an atom or a group of atoms in the same or a different molecule, in which there is evidence of bond formation. (See the IUPAC Provisional Recommendation on the definition of a hydrogen bond.) Dots are employed to indicate the presence of a hydrogen bond: X–H•••Y. The attractive interaction in a hydrogen bond typically has a strong electrostatic contribution, but dispersion forces and weak covalent bonding are also present.

In metallic solids and network solids, however, chemical bonds hold the individual chemical subunits together. The crystal is essential a single, macroscopic molecule with continuous chemical bonding throughout the entire structure. In metallic solids, the valence electrons are no longer exclusively associated with a single atom. Instead these electrons exist in molecular orbitals that are delocalized over many atoms, producing an electronic band structure. The metallic crystal essentially consists of a set of metal cations in a sea of electrons. This type of chemical bonding is called metallic bonding.

Ionic Solids

You learned previously that an ionic solid consists of positively and negatively charged ions held together by electrostatic forces. The strength of the attractive forces depends on the charge and size of the ions that compose the lattice and determines many of the physical properties of the crystal.

The lattice energy (i.e., the energy required to separate 1 mol of a crystalline ionic solid into its component ions in the gas phase) is directly proportional to the product of the ionic charges and inversely proportional to the sum of the radii of the ions. For example, NaF and CaO both crystallize in the face-centered cubic (fcc) sodium chloride structure, and the sizes of their component ions are about the same: Na⁺ (102 pm) versus Ca²⁺ (100 pm), and F⁻ (133 pm) versus O²⁻ (140 pm). Because of the higher charge on the ions in CaO, however, the lattice energy of CaO is almost four times greater than that of NaF (3401 kJ/mol versus 923 kJ/mol). The forces that hold Ca and O together in CaO are much stronger than those that hold Na and F together in NaF, so the heat of fusion of CaO is almost twice that of NaF (59 kJ/mol versus 33.4 kJ/mol), and the melting point of CaO is 2927°C versus 996°C for NaF. In both cases, however, the values are large; that is, simple ionic compounds have high melting points and are relatively hard (and brittle) solids.

Chemical Bonding In Solids Burdett Pdf Answers

Molecular Solids

Molecular solids consist of atoms or molecules held to each other by dipole–dipole interactions, London dispersion forces, or hydrogen bonds, or any combination of these. The arrangement of the molecules in solid benzene is as follows:

Because the intermolecular interactions in a molecular solid are relatively weak compared with ionic and covalent bonds, molecular solids tend to be soft, low melting, and easily vaporized ((ΔH_{fus}) and (ΔH_{vap}) are low). For similar substances, the strength of the London dispersion forces increases smoothly with increasing molecular mass. For example, the melting points of benzene (C₆H₆), naphthalene (C₁₀H₈), and anthracene (C₁₄H₁₀), with one, two, and three fused aromatic rings, are 5.5°C, 80.2°C, and 215°C, respectively. The enthalpies of fusion also increase smoothly within the series: benzene (9.95 kJ/mol) < naphthalene (19.1 kJ/mol) < anthracene (28.8 kJ/mol). If the molecules have shapes that cannot pack together efficiently in the crystal, however, then the melting points and the enthalpies of fusion tend to be unexpectedly low because the molecules are unable to arrange themselves to optimize intermolecular interactions. Thus toluene (C₆H₅CH₃) and m-xylene [m-C₆H₄(CH₃)₂] have melting points of −95°C and −48°C, respectively, which are significantly lower than the melting point of the lighter but more symmetrical analog, benzene.

Self-healing rubber is an example of a molecular solid with the potential for significant commercial applications. The material can stretch, but when snapped into pieces it can bond back together again through reestablishment of its hydrogen-bonding network without showing any sign of weakness. Among other applications, it is being studied for its use in adhesives and bicycle tires that will self-heal.

Covalent Network Solids

Covalent solids are formed by networks or chains of atoms or molecules held together by covalent bonds. A perfect single crystal of a covalent solid is therefore a single giant molecule. For example, the structure of diamond, shown in part (a) in Figure (PageIndex{1}), consists of sp3 hybridized carbon atoms, each bonded to four other carbon atoms in a tetrahedral array to create a giant network. The carbon atoms form six-membered rings.

The unit cell of diamond can be described as an fcc array of carbon atoms with four additional carbon atoms inserted into four of the tetrahedral holes. It thus has the zinc blende structure described in Section 12.3, except that in zinc blende the atoms that compose the fcc array are sulfur and the atoms in the tetrahedral holes are zinc. Elemental silicon has the same structure, as does silicon carbide (SiC), which has alternating C and Si atoms. The structure of crystalline quartz (SiO₂), shown in Section 12.1, can be viewed as being derived from the structure of silicon by inserting an oxygen atom between each pair of silicon atoms.

All compounds with the diamond and related structures are hard, high-melting-point solids that are not easily deformed. Instead, they tend to shatter when subjected to large stresses, and they usually do not conduct electricity very well. In fact, diamond (melting point = 3500°C at 63.5 atm) is one of the hardest substances known, and silicon carbide (melting point = 2986°C) is used commercially as an abrasive in sandpaper and grinding wheels. It is difficult to deform or melt these and related compounds because strong covalent (C–C or Si–Si) or polar covalent (Si–C or Si–O) bonds must be broken, which requires a large input of energy.

Other covalent solids have very different structures. For example, graphite, the other common allotrope of carbon, has the structure shown in part (b) in Figure (PageIndex{1}). It contains planar networks of six-membered rings of sp2 hybridized carbon atoms in which each carbon is bonded to three others. This leaves a single electron in an unhybridized 2pz orbital that can be used to form C=C double bonds, resulting in a ring with alternating double and single bonds. Because of its resonance structures, the bonding in graphite is best viewed as consisting of a network of C–C single bonds with one-third of a π bond holding the carbons together, similar to the bonding in benzene.

To completely describe the bonding in graphite, we need a molecular orbital approach similar to the one used for benzene in Chapter 9. In fact, the C–C distance in graphite (141.5 pm) is slightly longer than the distance in benzene (139.5 pm), consistent with a net carbon–carbon bond order of 1.33. In graphite, the two-dimensional planes of carbon atoms are stacked to form a three-dimensional solid; only London dispersion forces hold the layers together. As a result, graphite exhibits properties typical of both covalent and molecular solids. Due to strong covalent bonding within the layers, graphite has a very high melting point, as expected for a covalent solid (it actually sublimes at about 3915°C). It is also very soft; the layers can easily slide past one another because of the weak interlayer interactions. Consequently, graphite is used as a lubricant and as the “lead” in pencils; the friction between graphite and a piece of paper is sufficient to leave a thin layer of carbon on the paper. Graphite is unusual among covalent solids in that its electrical conductivity is very high parallel to the planes of carbon atoms because of delocalized C–C π bonding. Finally, graphite is black because it contains an immense number of alternating double bonds, which results in a very small energy difference between the individual molecular orbitals. Thus light of virtually all wavelengths is absorbed. Diamond, on the other hand, is colorless when pure because it has no delocalized electrons. Table (PageIndex{2}) compares the strengths of the intermolecular and intramolecular interactions for three covalent solids, showing the comparative weakness of the interlayer interactions.

Carbon: An example of an Covalent Network Solid

In network solids, conventional chemical bonds hold the chemical subunits together. The bonding between chemical subunits, however, is identical to that within the subunits, resulting in a continuous network of chemical bonds. One common examples of network solids are diamond (a form of pure carbon) Carbon exists as a pure element at room temperature in three different forms: graphite (the most stable form), diamond, and fullerene.

Diamonds

The structure of diamond is shown at the right in a 'ball-and-stick' format. The balls represent the carbon atoms and the sticks represent a covalent bond. Be aware that in the 'ball-and-stick' representation the size of the balls do not accurately represent the size of carbon atoms. In addition, a single stick is drawn to represent a covalent bond irrespective of whether the bond is a single, double, or triple bond or requires resonance structures to represent. In the diamond structure, all bonds are single covalent bonds ((sigma) bonds). The 'space-filling' format is an alternate representation that displays atoms as spheres with a radius equal to the van der Waals radius, thus providing a better sense of the size of the atoms.

Notice that diamond is a network solid. The entire solid is an 'endless' repetition of carbon atoms bonded to each other by covalent bonds. (In the display at the right, the structure is truncated to fit in the display area.)

Questions to consider

• What is the bonding geometry around each carbon?
• What is the hybridization of carbon in diamond?
• The diamond structure consists of a repeating series of rings. How many carbon atoms are in a ring?
• Diamond are renowned for its hardness. Explain why this property is expected on the basis of the structure of diamond.

Graphite

The most stable form of carbon is graphite. Graphite consists of sheets of carbon atoms covalently bonded together. These sheets are then stacked to form graphite. Figure (PageIndex{3}) shows a ball-and-stick representation of graphite with sheets that extended 'indefinitely' in the xy plane, but the structure has been truncated for display purposed. Graphite may also be regarded as a network solid, even though there is no bonding in the z direction. Each layer, however, is an 'endless' bonded network of carbon atoms.

Questions to consider

Chemical Bonding In Solids Burdett Pdf Answer

• What is the bonding geometry around each carbon?
• What is the hybridization of carbon in graphite?
• The a layer of the graphite structure consists of a repeating series of rings. How many carbon atoms are in a ring?
• What force holds the carbon sheets together in graphite?
• Graphite is very slippery and is often used in lubricants. Explain why this property is expected on the basis of the structure of graphite.
• The slipperiness of graphite is enhanced by the introduction of impurities. Where would such impurities be located and why would they make graphite a better lubricant?

Fullerenes

Until the mid 1980's, pure carbon was thought to exist in two forms: graphite and diamond. The discovery of C₆₀ molecules in interstellar dust in 1985 added a third form to this list. The existence of C₆₀, which resembles a soccer ball, had been hypothesized by theoreticians for many years. In the late 1980's synthetic methods were developed for the synthesis of C₆₀, and the ready availability of this form of carbon led to extensive research into its properties.

The C₆₀ molecule (Figure (PageIndex{4}); left), is called buckminsterfullerene, though the shorter name fullerene is often used. The name is a tribute to the American architect R. Buckminster Fuller, who is famous for designing and constructing geodesic domes which bear a close similarity to the structure of C₆₀. As is evident from the display, C₆₀ is a sphere composed of six-member and five-member carbon rings. These balls are sometimes fondly referred to as 'Bucky balls'. It should be noted that fullerenes are an entire class of pure carbon compounds rather than a single compound. A distorted sphere containing more than 60 carbon atoms have also been found, and it is also possible to create long tubes (Figure (PageIndex{4}); right). All of these substances are pure carbon.

Chemical Bonding In Solids Burdett Pdf Printable

Questions to Consider

• What is the bonding geometry around each carbon? (Note that this geometry is distorted in (C_{60}).)
• What is the hybridization of carbon in fullerene?
• A single crystal of C60 falls into which class of crystalline solids?
• It has been hypothesized that C60 would make a good lubricant. Why might C60 make a good lubricant?

Chemical Bonding In Solids Burdett Pdf Free

Format

Häftad (Paperback)

Språk

Engelska

Antal sidor

336

Utgivningsdatum

1995-05-01

Upplaga

illustrated ed

Förlag

OUP USA

Illustrationer

figs.tabs. bibliog.

Dimensioner

233 x 162 x 21 mm

Vikt

558 g

Antal komponenter

1

ISBN

9780195089929

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'I found the critical re-inspection of familiar concepts such as ionic radii and close packing of spheres most interesting. The author does away with Pauling's rules and the classification of bond types as introduced by Van Arkel and Ketelaar.'--Wolfgang Sachtler, Northwestern University<br>

1: Molecules 1.1: The H2 Molecule: Molecular Orbitial Approach 1.2: The H2 Molecule: Localized Approach 1.3: Energy Levels of HHe 1.4: Energy Levels of Linear Conjugated Molecules 1.5: Energy Levels of Cyclic Polyenes 1.6: Energy Differences and Moments 1.7: The Jahn-Teller Effects 2: From Molecules to Solids 2.1: The Solid as a Giant Molecule 2.2: Some Properties of Solids from the Band Picture 2.3: Two Atom Cells 2.4: The Peierls Distortion 2.5: Other One-Dimensional Systems 2.6: Second Order Peierls Distortions 3: More Details Concerning Energy Bands 3.1: The Brillouin Zone 3.2: The Fermi Surface 3.3: Symmetry Considerations 4: The Electronic Structure of Solids 4.1: Oxides with the NaCl, TiO2 and MoO2 Structures 4.2: The Diamond and Zincblende Structures 4.3: 'Localization' of 'Delocalized' Orbitals in Solids 4.4: The Structure of NbO 4.5: Chemical Bonding in Ionic Compounds 4.6: The Transition Metals 4.7: The Free-Electron Model 4.8: Compounds between Transition Metals and Main Group Elements 4.9: The Nickel Arsenide and Related Structures 4.10: Molecular Metals 4.11: Division into Electronic Types 5: Metals and Insulators 5.1: The Importance of Structure and Composition 5.2: The Structures of Calcium and Zinc 5.3: Geometrical Instabilities 5.4: Importance of Electron-Electron Interactions 5.5: Transition Metal and Rare Earth Oxides 5.6: Effect of Doping 5.7: Superconductivity in the C60 Series 5.8: High-Temperature Superconductors 6: The Structures of Solids and Pauling's Rules 6.1: General Description of Ion Packings 6.2: The First Rule 6.3: The Second Rule 6.4: The Third Rule 6.5: The Fifth Rule 6.6: The Description of Solids in Terms of Pair Potentials 6.7: More About the Orbital Description of Silicates 7: The Structures of Some Covalent Solids 7.1: Electron Counting 7.2: Change of Structure with Electron Count 7.3: Structures of Soem AX2 Solids 7.4: Structures Derived from Simple Cubic or Rocksalt 7.5: The Stability of the Rocksalt and Zincblende Structures 7.6: The Structures of the Spinels 7.7: Distortions of the Cadmium Halide Structure: Jahn-Teller Considerations 7.8: Distortions of the Cadmium Halide Structure: Trigonal Prismatic Coordination 7.9: Distortions of the Cadmium Halide Structure: t2g Block Instabilities 7.10: The Rutile Versus Cadmium Halide Versus Pyrite Structures 7.11: Second Order Structural Changes 8: More About Structures 8.1: The Structures of the Elements 8.2: The Structures of Some Main Group Intermetallic Compounds 8.3: The Hume-Rothery Rules 8.4: Pseudopotential Theory 8.5: The Structures of the First Row Elements 8.6: The Coloring Problem 8.7: Structural Stability and Band Gap