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Octet rule

The octet rule is a fundamental principle in chemistry stating that atoms of most elements tend to achieve a stable by surrounding themselves with eight electrons in their valence shell, similar to the configuration of , through the gain, loss, or sharing of electrons in chemical bonds. This rule provides a simple framework for predicting the formation of ionic and covalent bonds, as well as for drawing Lewis structures that represent molecular geometries and electron distributions. It applies primarily to main-group elements and underscores the drive toward electronic stability in chemical reactions. The concept originated in the early 20th century, building on earlier observations such as Richard Abegg's 1904 "rule of eight" regarding maximum and minimum valences, but it was formalized by American chemist in his seminal 1916 paper, "The Atom and the Molecule," published in the Journal of the . In this work, Lewis introduced the electron-pair theory of the and used dot notation to illustrate how atoms share electrons to complete their octets, revolutionizing the understanding of molecular structure. Lewis's ideas stemmed from his earlier 1902 cubical atom model, which envisioned electrons arranged at the corners of a to achieve stability, though he later refined this into the more general octet framework. The octet rule gained widespread acceptance through the efforts of , who between 1919 and 1921 elaborated on Lewis's model in a series of papers, coining the term "octet rule" and applying it mathematically to predict bonding arrangements, such as the formula for total valence electrons (e = 8n - 2p, where n is the number of atoms and p is the number of electron pairs). Langmuir's contributions, including the introduction of terms like "," helped integrate the rule into mainstream chemical theory during the . While highly effective for elements in periods 2 and 3, the rule has notable exceptions for elements with d orbitals (e.g., expanded octets in ) or those achieving only a duet (e.g., ), highlighting its status as a guideline rather than an absolute law.

Definition and Principles

Core Concept

The octet rule is a fundamental guideline in chemical bonding, positing that atoms of main-group elements tend to form bonds by gaining, losing, or sharing electrons to achieve eight electrons in their valence shell, thereby attaining a stable configuration akin to the (1s²2s²2p⁶) or (1s²2s²2p⁶3s²3p⁶). This principle, originally articulated as the "rule of eight" by in his 1916 paper, emphasizes that such an arrangement provides maximum stability by filling the outermost s and p orbitals. The rule's effectiveness stems from the energetic favorability of a complete octet, which lowers the overall of the compared to incomplete shells, as the filled subshells minimize repulsion and achieve a closed-shell structure. It applies primarily to s- and p-block elements in periods 2 and 3, where the valence electrons are limited to these orbitals, though it offers less predictive power for transition metals or heavier elements with available d orbitals. Electronegativity plays a crucial role in determining the bonding mechanism to reach this octet: when the electronegativity difference between atoms exceeds approximately 2, electrons are transferred to form ions in ionic bonds (e.g., one atom achieves octet by gaining electrons, the other by losing them); smaller differences lead to shared electron pairs in covalent bonds. The term "octet rule" was later coined by in to specifically denote this eight-electron criterion, setting it apart from prior valence theories that focused on combining capacities without reference to outer-shell electron counts.

Lewis Dot Structures

Lewis dot structures, also known as Lewis electron dot diagrams, provide a visual representation of the electrons in and how they are shared or transferred to form chemical bonds, aligning with the octet rule by illustrating arrangements that achieve electron configurations. In these diagrams, each is represented by its , with dots symbolizing electrons; typically, single bonds are depicted as lines or pairs of dots representing shared electron pairs between . The goal is to distribute electrons such that the central and surrounding attain an octet of eight electrons in their valence shells, except where exceptions apply. To construct a Lewis dot structure, first determine the total number of electrons available from all in the or , adjusting for any charge by adding electrons for anions or subtracting for cations. Next, identify the central —usually the least electronegative excluding —and draw a skeletal framework connecting it to surrounding with single bonds, allocating two electrons per bond. Then, distribute the remaining electrons as lone pairs to complete the octets around each , starting with the outer ; if electrons are insufficient, form multiple bonds by sharing additional pairs. Finally, verify that all satisfy the octet rule where applicable, ensuring the total electrons used match the initial count. The octet rule guides this process, aiming for eight valence electrons around each atom to mimic noble gas stability, represented by eight dots or equivalent bonds and lone pairs surrounding the atom's symbol. Hydrogen and helium are notable exceptions, requiring only a duet of two electrons for stability rather than an octet, as their valence shells are filled with just two electrons. These structures thus highlight how electron sharing in covalent bonds or transfer in ionic representations fulfills these electron requirements. For validation and selection among possible structures, calculate the formal charge on each atom using the formula: \text{Formal charge} = \text{valence electrons} - \left( \text{nonbonding electrons} + \frac{1}{2} \text{bonding electrons} \right) This metric assumes equal sharing of bonding electrons and helps identify the most stable form or preferred arrangement. When drawing Lewis structures, prioritize arrangements that minimize formal charges—ideally zero for neutral atoms—while satisfying octets, as lower formal charges indicate more realistic distributions. These diagrams serve as simplified models of , focusing on electron counts rather than spatial or , which are addressed through other theoretical tools.

Historical Context

Early Ideas

In the mid-19th century, chemists began observing consistent patterns in the formulas of inorganic compounds, suggesting that elements possess fixed capacities for combining with others. For instance, sodium consistently formed NaCl rather than NaCl₂, indicating a valence of one, while chlorine paired with one sodium atom, implying its own fixed valence. These empirical regularities were formalized by Edward Frankland in 1852, who proposed that each element has a characteristic "combining power" or valence, based on his synthesis of organometallic compounds like zinc ethyl, which revealed symmetrical formulas across organic and inorganic substances. By the early , these ideas evolved into more structured theories linking to atomic structure. In , Richard Abegg formulated Abegg's rule, stating that the difference between the maximum positive and minimum negative of an element is often eight units, as seen in elements like (maximum +7 in perchlorates, minimum -1 in chlorides). Abegg drew from electrochemical data to argue that this "counter-valence" of eight reflects an inherent stability limit in bonding capacity. Concurrent with Abegg's work, early atomic models began incorporating electron counts that hinted at octet-like arrangements. In 1902, proposed a cubic atom model, visualizing the atom as a with electrons positioned at its eight corners to explain periodicity and in a geometric framework. Similarly, J.J. Thomson's 1904 depicted atoms as spheres of positive charge embedded with multiple electrons, which Thomson explicitly connected to Abegg's rule by suggesting that chemical stability arises from specific electron configurations balancing positive and negative charges. These pre-quantum ideas collectively pointed toward a stable outer layer of eight electrons or units without invoking electronic shells, setting the stage for later precise articulation in 1916.

Lewis's Formulation

In 1916, published his seminal paper "The Atom and the Molecule" in the Journal of the , where he introduced the concept of the octet rule as a guiding for chemical . Independently in the same year, Walther Kossel proposed a similar applied to , emphasizing electron configurations. Lewis proposed that atoms achieve stability by attaining eight electrons in their shells, mimicking the configuration of , through either the transfer of electrons in ionic bonds or the sharing of electron pairs in covalent bonds. A key innovation in Lewis's formulation was the idea of shared electron pairs forming covalent bonds, where each atom contributes one electron to a pair that is jointly owned, allowing both to complete their octets. He envisioned the octet as eight electrons arranged at the corners of a cube surrounding the atomic kernel ( plus inner electrons), providing a geometric model for this stable configuration. This cubical octet represented a departure from earlier static electron models, emphasizing dynamic pairing to explain bond formation. Lewis's work unified ionic and covalent bonding under the principle of achieving electron configurations, resolving inconsistencies in prior theories by attributing bond stability to electron redistribution. For instance, he predicted the of (H₂O) as oxygen sharing two pairs with atoms to complete its octet, with the remaining four electrons as two s, accounting for the molecule's stability. Similarly, for (NH₃), forms three shared pairs with hydrogens and retains one , achieving an octet and explaining its tetrahedral electron arrangement. These insights laid the groundwork for modern theory, influencing subsequent developments in structural chemistry.

Examples

Ionic Compounds

In ionic compounds, the octet rule manifests through the complete transfer of electrons from metal atoms to atoms, resulting in the formation of cations and anions that achieve stable electron configurations resembling those of . Metal atoms, typically from the s-block, lose one or more electrons to form positively charged cations, emptying their valence but achieving an octet in their inner shell, akin to a core. For instance, a sodium atom () with 11 electrons and a valence of [Ne] 3s¹ loses its 3s electron to become Na⁺, which has the stable neon () configuration of 1s² 2s² 2p⁶. Conversely, atoms from the p-block gain these electrons to complete their valence octet. A chlorine atom () with 17 electrons and a valence of [Ne] 3s² 3p⁵ accepts one electron to form Cl⁻, achieving the () configuration of [Ne] 3s² 3p⁶. This is driven by the tendency to attain lower energy states through octet completion, leading to oppositely charged ions that are bound by strong electrostatic attractions. A classic example is (NaCl), where the ionic lattice consists of Na⁺ and Cl⁻ ions arranged in a repeating three-dimensional structure. Each Na⁺ ion is surrounded by six Cl⁻ ions, and vice versa, maximizing electrostatic interactions that stabilize the crystal. The Na⁺ cation attains a neon-like configuration (an octet in the n=2 ), while the Cl⁻ anion fulfills the octet rule in its , mirroring the electron configuration of . The of NaCl, arising from these Coulombic forces between ions, is sufficiently exothermic to overcome the endothermic costs of and electron attachment, rendering the compound stable under standard conditions. This arrangement exemplifies how the octet rule predicts the 1:1 in such binary ionic compounds. The octet rule generalizes to other ionic compounds involving s-block metals and p-block nonmetals, where the charges and ratios ensure octet completion for the anions. For example, magnesium () from group 2 loses two 3s electrons to form Mg²⁺ with a neon core configuration, while two chloride ions each gain one electron to achieve octets, yielding the formula MgCl₂. This pattern holds for alkali metals () forming +1 cations with halides () and alkaline earth metals (group 2) with oxides () or halides, predicting empirical formulas based on valence electron counts. Such compounds exhibit high points and in molten or aqueous states due to the ionic nature reinforced by octet-driven ion formation. The thermodynamic feasibility of this is illuminated by the Born-Haber cycle, which decomposes the formation of an ionic compound like NaCl from its elements into sequential steps: of the metal, of the nonmetal, of the gaseous metal atom, attachment of electrons to the gaseous nonmetal atom, and finally, the condensation of gaseous ions into the lattice. Although and are endothermic, the highly exothermic —stemming from electrostatic attractions—along with the step, results in an overall negative change, justifying the prevalence of octet-achieving in these systems. This cycle underscores the energy rationale behind the octet rule in ionic contexts without invoking shared electrons.

Covalent Compounds

In covalent bonding, atoms achieve stability by sharing valence electrons in pairs, allowing each atom to attain an octet configuration in its valence shell, as per the octet rule. This electron sharing forms covalent bonds, where the shared pair is counted toward the octet of both participating atoms, contrasting with the complete seen in . The mechanism involves overlapping atomic orbitals from each atom, creating a region of high between nuclei that holds the atoms together. A classic example is methane (CH₄), where the carbon atom, possessing four valence electrons, forms four single covalent bonds by sharing one electron pair with each of four hydrogen atoms. In the resulting Lewis structure, carbon is surrounded by eight electrons (four bonding pairs), satisfying its octet, while each hydrogen atom achieves a stable duet configuration with two electrons. Similarly, in ammonia (NH₃), the nitrogen atom shares three electron pairs with three hydrogen atoms, forming three single bonds and retaining one lone pair, which completes nitrogen's octet with eight electrons total. For multiple bonds, carbon dioxide (CO₂) illustrates the octet rule through double bonds: the central carbon atom shares two electron pairs (a double bond) with each of two oxygen atoms, enabling carbon to reach eight electrons, while each oxygen also achieves an octet via the shared pairs and its own lone pairs. The in these molecules—single (one shared pair), double (two shared pairs), or triple (three shared pairs)—directly relates to the number of electrons contributed to each atom's octet, with higher bond orders generally indicating stronger bonds. In , the four equivalent C-H bonds arise from the carbon atom's sp³ ization, where its 2s and three 2p orbitals mix to form four sp³ hybrid orbitals arranged in a tetrahedral , facilitating the symmetric sharing of electrons. This adherence to the octet rule in covalent compounds results in lower for the compared to isolated atoms, as the filled shells mimic the electron configuration of , enhancing overall molecular stability./Electronic_Structure_of_Atoms_and_Molecules/Electronic_Configurations/The_Octet_Rule)

Theoretical Foundations

Valence Bond Theory

describes chemical bonds as the result of overlapping atomic orbitals from adjacent atoms, where a pair of s is shared to form a localized , enabling atoms to achieve a stable configuration. This sharing aligns with the octet rule, as the central atom in a typically forms four such electron pairs in its valence shell, resulting in eight electrons surrounding it. For instance, in diatomic molecules like , the overlap of p orbitals creates a with shared electrons satisfying the octet for each atom. To explain molecular geometries that conform to the octet rule, incorporates , where atomic s and p orbitals mix to form equivalent hybrid orbitals suitable for bonding. In (CH₄), the carbon atom hybridizes its 2s and three 2p orbitals into four sp³ hybrid orbitals, each overlapping with a 1s orbital to form four equivalent C-H bonds arranged tetrahedrally, thus fulfilling the octet around carbon while matching the observed 109.5° bond angles. This hybridization concept, developed by , provides a framework for understanding how the octet rule dictates both bonding and shape in simple molecules. In cases where a single Lewis structure cannot fully represent the bonding while adhering to the octet rule, employs , superimposing multiple contributing structures to describe the actual distribution. For (O₃), two resonance forms, in each of which the central oxygen has one to one terminal oxygen, one to the other, and one , satisfy the octet around all atoms, but the hybrid structure delocalizes the pi electrons, averaging bond orders to 1.5 while maintaining an effective octet configuration around all atoms. The stability from this resonance arises from the between atomic orbitals in the contributing forms, which enhances without requiring mathematical derivation here.

Molecular Orbital Theory

Molecular orbital (MO) theory provides a quantum mechanical framework for understanding chemical bonding, where atomic orbitals from constituent atoms combine linearly to form molecular orbitals that extend over the entire molecule. These molecular orbitals are classified as bonding (lower energy, stabilizing the molecule), antibonding (higher energy, destabilizing), or non-bonding, and electrons occupy them according to the , , and Hund's rule. In this delocalized electron picture, the octet rule emerges as the tendency for main-group elements, particularly those in the second period, to achieve stability by filling their valence molecular orbitals with eight electrons, corresponding to a closed-shell configuration analogous to . The stability associated with the octet in MO theory arises from a large energy gap between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO), which minimizes reactivity in closed-shell species. For example, in the nitrogen molecule (N₂), the ten valence electrons (five from each nitrogen atom) fill the bonding molecular orbitals—specifically, the σ_{2s}, π_{2p}, and σ_{2p} orbitals—resulting in a triple bond and a HOMO-LUMO gap that reflects the molecule's high stability, consistent with each nitrogen effectively sharing eight valence electrons in a delocalized manner. This configuration underscores how MO theory rationalizes the octet as a filled valence shell without invoking localized pairs, contrasting with the complementary localized perspective of valence bond theory. For elements in the second period, the strict adherence to the octet rule stems from the limited availability of valence orbitals: only the 2s and three 2p orbitals are involved, accommodating a maximum of eight electrons due to poor overlap with higher-energy 3d orbitals, which are energetically inaccessible for bonding. This orbital constraint prevents expansion beyond eight electrons, enforcing the octet for compounds like water (H₂O), where the total of eight valence electrons (six from oxygen, one from each hydrogen) occupy four molecular orbitals—two bonding σ orbitals for the O-H bonds and two non-bonding lone-pair orbitals on oxygen—yielding a bent structure with the octet satisfied around the central atom.

Exceptions and Limitations

Sub-Octet Compounds

Sub-octet compounds, also known as electron-deficient compounds, feature a central atom with fewer than eight valence electrons in its , representing a key exception to the octet rule. These structures arise primarily in compounds of second-period elements, where the limited availability of electrons and the inability to utilize d orbitals prevent the central atom from achieving a full octet./Chemical_Bonding/Lewis_Theory_of_Bonding/Violations_of_the_Octet_Rule) A prominent example is (BF₃), in which the boron atom forms three single bonds with atoms, resulting in only six valence electrons around . Similarly, (BeCl₂) in the gas phase adopts a linear monomeric structure, with surrounded by just four valence electrons from two Be–Cl bonds. These configurations highlight the at the central atom, which stems from the small atomic size and high of the surrounding atoms, such as or , that draw away./Chemical_Bonding/Lewis_Theory_of_Bonding/Violations_of_the_Octet_Rule) The electron deficiency in these compounds confers strong Lewis acidity, as the central atom readily accepts an electron pair from a Lewis base to form stable adducts, such as BF₃·NH₃. This behavior is particularly pronounced in period 2 elements like and , which cannot expand their valence shells beyond the s and p orbitals, and where the high bond dissociation energies of the resulting bonds outweigh the energetic cost of an incomplete octet./08:_Ionic_versus_Covalent_Bonding/8.06:_Exceptions_to_the_Octet_Rule) To compensate for the electron shortage, sub-octet compounds often engage in dimerization or coordination with multidentate ligands, effectively sharing electrons across multiple centers. For example, BeCl₂ in the gas phase can dimerize to (BeCl₂)₂, allowing bridging chlorines to donate electron density and increase coordination around beryllium. Despite violating the octet rule, these compounds exhibit remarkable stability, as evidenced by formal charge calculations that yield zero formal charges for all atoms; in BF₃, boron's formal charge is calculated as $3 - 0 - \frac{1}{2}(6) = 0, and each fluorine's as $7 - 6 - \frac{1}{2}(2) = 0./Chemical_Bonding/Lewis_Theory_of_Bonding/Violations_of_the_Octet_Rule)

Hypervalent Compounds

Hypervalent compounds are molecules in which the central atom, typically from the third period or below, appears to possess more than eight valence electrons, challenging the strict application of the octet rule.00102-9) Classic examples include sulfur hexafluoride (SF6), where the sulfur atom is surrounded by 12 valence electrons from six S–F bonds, and phosphorus pentachloride (PCl5), with phosphorus exhibiting 10 valence electrons from five P–Cl bonds. These structures adopt geometries predicted by valence shell electron pair repulsion (VSEPR) theory: octahedral for SF6 (AX6 notation) and trigonal bipyramidal for PCl5 (AX5 notation), reflecting the repulsion among the electron domains around the central atom. Traditionally, hypervalency was attributed to the participation of d-orbitals in , allowing of the octet for elements like and , which have available 3d orbitals. However, this view has been widely debated and largely discredited by quantum chemical studies, as d-orbitals are energetically mismatched and contribute negligibly to the bonding wavefunctions in these molecules. For instance, high-level calculations on SF6 show minimal d-orbital involvement, with the bonding better described without invoking octet . Modern explanations reject the notion of true hypervalency as a violation of the octet rule, instead favoring models that maintain octet configurations through multicenter bonding or charge delocalization. In the three-center four-electron (3c–4e) bond model, originally proposed by Pimentel and Rundle, axial ligands in molecules like PCl5 share electrons in delocalized bonds that avoid exceeding eight electrons on the central atom. Similarly, the recoupled (RPB) model, developed through generalized , describes SF6 as involving recoupling of s2 lone pairs on to form additional bonds without d-orbital reliance, aligning with quantum calculations that emphasize ionic character and effects. Post-2010 studies, including breathing orbital bond analyses, further support charge-shift bonding in like SF4, PF5, and ClF3, where between covalent and ionic structures stabilizes the electron-rich environments, confirming that hypervalent appearances stem from and multicenter interactions rather than d-orbital usage. localization function (ELF) analyses reinforce this by revealing valence shell populations that often align with or fall below eight electrons when accounting for ligand , as in SF6.00102-9)

Extensions

Duet Rule

The duet rule is a chemical principle that describes the stable achieved by and atoms through the acquisition of two electrons, fully occupying their 1s orbital in a manner analogous to the atom's . This rule applies exclusively to these period 1 elements, which lack the higher-energy orbitals necessary for accommodating eight electrons, making an octet configuration impossible due to the spatial and energetic constraints of the 1s shell. Unlike heavier elements, and thus seek a "" of electrons to attain nobility-like stability, serving as a foundational in electron dot structures. A classic example of the duet rule is the hydrogen molecule (H₂), where two hydrogen atoms each contribute one to form a single , resulting in each atom possessing two electrons in its valence shell. In (HF), the hydrogen atom shares its single valence electron with , achieving a duet while the fluorine atom completes its octet through this bonding pair and its own lone pairs. These structures illustrate how the duet rule governs bonding in simple diatomic species involving hydrogen, ensuring minimal electron sharing limited by the atom's capacity. As a specialized case of the broader octet rule, the duet rule pertains specifically to period 1 elements and elucidates why forms no more than one per atom, as additional bonds would exceed the 1s orbital's capacity. This distinction is evident in polyatomic molecules like (CH₄), where each of the four atoms adheres to the duet rule via a to the central carbon atom, while the carbon satisfies the octet rule with eight shared electrons. Such examples highlight the duet rule's role in predicting stable configurations for -containing compounds without violating electronic shell limits.

18-Electron Rule

The 18-electron rule describes the tendency of complexes to achieve stability by attaining 18 electrons around the central metal atom, filling the nine available valence orbitals (one s, three p, and five d) to achieve an electronic configuration analogous to that of (ns² (n-1)d¹⁰ np⁶). This rule extends the octet principle from main-group elements to the d-block by accounting for the additional d-orbitals, where the total electron count is determined by adding the metal's valence electrons (group number) to those donated by ligands, often using neutral or ionic counting methods. Complexes adhering to this rule are typically coordinatively saturated and kinetically inert, promoting thermodynamic stability. In practice, ligands such as phosphines or carbonyls donate electrons to the metal's empty orbitals via sigma bonds, while back-donation from the metal's filled d-orbitals to the ligands' empty pi* orbitals further stabilizes the complex by relieving electron density on the metal and strengthening metal-ligand interactions. This synergistic bonding is particularly evident in organometallic compounds. For instance, in (\ce{Ni(CO)4}), (group 10, 10 valence electrons) receives 2 electrons from each of the four CO ligands, yielding 18 electrons total and a tetrahedral geometry. Similarly, (\ce{Fe(C5H5)2}) follows the rule using the neutral counting method, where iron contributes 8 valence electrons and each cyclopentadienyl ligand acts as a 5-electron donor, resulting in 18 electrons and exceptional stability for this sandwich compound. The primarily applies to , guiding the design of stable complexes in low-oxidation states with pi-acceptor ligands. However, in research during the 2020s, deviations from this rule—such as 16-electron unsaturated or even 20-electron configurations—have been increasingly emphasized to enable reactive intermediates for processes like cross-coupling and , as demonstrated by stable 20-electron derivatives that challenge traditional stability paradigms.

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