Module 2.2: How Differences in Atomic-Scale Bonding Create Macroscopic Property Differences in Materials

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Vocabulary flashcards covering the relationships between atomic bonding potential curves and macroscopic mechanical and thermal properties such as elastic modulus, activation energy, melting temperature, and coefficient of thermal expansion.

13 Terms

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<p>Spring Model of Atomic Bonding</p>

Spring Model of Atomic Bonding

A physical model that treats bonds between atoms as springs, enabling the connection between atomic-scale bonding models and macroscopic stiffness (elastic modulus).

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Elastic Modulus (EE) from Force-Distance Curve

The measure of material stiffness modeled by the slope near the equilibrium point on an interatomic force versus separation curve: dFdx∼dσdϵ=E\frac{dF}{dx} \sim \frac{d\sigma}{d\epsilon} = E.

<p>The measure of material stiffness modeled by the slope near the equilibrium point on an interatomic force versus separation curve: $$\frac{dF}{dx} \sim \frac{d\sigma}{d\epsilon} = E$$.</p>
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Curvature of the Bond-Energy Curve

The second derivative of potential energy with respect to distance (d2Udx2∼dFdx∼E\frac{d^2U}{dx^2} \sim \frac{dF}{dx} \sim E), where a tighter bend indicates higher curvature (1radius of curvature\frac{1}{\text{radius of curvature}}) and a higher elastic modulus (EE).

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Potential Energy Function (U(x)U(x))

The potential energy of an interatomic bond as a function of atomic separation distance xx, determined by integrating force: U(x)=∫x∞F dxU(x) = \int_x^{\infty} F\,dx.

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Thermal Vibration in Solids

The atomic oscillations within a potential well that increase in frequency and amplitude as temperature rises, broadening the range of interatomic distances (xx) between the most compressed and most stretched states.

<p>The atomic oscillations within a potential well that increase in frequency and amplitude as temperature rises, broadening the range of interatomic distances ($$x$$) between the most compressed and most stretched states.</p>
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Activation Energy (EaE_a)

The barrier energy that an atom must overcome to accomplish a kinetic process, such as melting, evaporating, or diffusing.

<p>The barrier energy that an atom must overcome to accomplish a kinetic process, such as melting, evaporating, or diffusing.</p>
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Boltzmann's Constant (kBk_B)

A fundamental constant used to calculate thermal energy per atom, having values of 1.38×10−23 J/(atom⋅K)1.38 \times 10^{-23}\,\text{J}/(\text{atom}\cdot\text{K}) or 8.62×10−5 eV/(atom⋅K)8.62 \times 10^{-5}\,\text{eV}/(\text{atom}\cdot\text{K}).

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Ideal Gas Constant (RR)

The molar gas constant equal to 8.314 J/(mol⋅K)8.314\,\text{J}/(\text{mol}\cdot\text{K}), defined on a per-mole basis and related to Boltzmann's constant by R=kB×NAR = k_B \times N_A.

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Thermal Energy of Atoms

The energy associated with temperature for atoms in a system, expressed quantitatively as kBTk_B T (with temperature TT in Kelvin, K\text{K}).

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Thermal Criterion for Atomic Tasks

The kinetic condition stating that an atomic process (such as melting or diffusion) is likely to occur when the thermal energy exceeds the barrier energy (thermal energy>Ea\text{thermal energy} > E_a).

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Coefficient of Thermal Expansion (CTE)

A macroscopic thermal property arising from the asymmetry of the interatomic potential energy well, which causes the average bond distance xx to increase as temperature increases.

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Potential Well Depth Rule of Thumb

The general principle that deeper potential energy wells are typically more symmetric, which causes materials with deeper wells to exhibit lower coefficients of thermal expansion (CTEs).

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Row 3 Elemental Bonding Trends

The trend across Sodium, Magnesium, Aluminum, and Silicon demonstrating that an increasing well depth (EaE_a) corresponds to higher enthalpy of fusion (3 kJ/mol3\,\text{kJ/mol} to 51 kJ/mol51\,\text{kJ/mol}), higher melting temperature (98 ∘C98\,^\circ\text{C} to 1412 ∘C1412\,^\circ\text{C}), higher elastic modulus (10 GPa10\,\text{GPa} to ∼150 GPa\sim 150\,\text{GPa}), and lower CTE (70 ppm/∘C70\,\text{ppm/}^\circ\text{C} to 3 ppm/∘C3\,\text{ppm/}^\circ\text{C}).