atoms Flashcards

1
Q

what’s the LJ 6-12 potential

A

the Lennard Jones 6-12 potential.

V = 4ε [ (σ/r^)12 - (σ/r)^6]

(σ/r^)12 represents the strong force
(σ/r^)6 represents the van der waals force

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2
Q

potential energy per atom

A

n/2 * ε
n: number of nearest neighbours
ε: binding energy
1/2 : the ε is shared between both atoms in the bond

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3
Q

how does the LJ 6-12 potential change for an ionic bond

A

the 4ε changes

the (σ/r)^6 loses its power of 6. (not actually lost just replaced as the van der Waals force is tiny compared to the Coulomb force)

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4
Q

whats the unit cell

A

smallest unit that can form the whole structure by tessalation

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5
Q

draw a diagram to show Bragg scattering

A

2 rows of parallel particles

2 parallel light rays incident at the centre (one at the top row and one at the bottom row)

θ is the angle between the light ray and the line of particles

draw 2 lines. each is from the top row’s centre particle and is perpendicular to the incident and reflected rays.

θ is also the angle between those lines and the normal to the row of particles.

this makes the distance between the bottom centre particle and the point where those lines intercept the light ray equal to d*sin(θ)

hence the path difference is 2d*sin(θ)

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6
Q

Bragg’s law equation

A

2dsin(θ) = nλ
d: the particle separation
λ: wavelength
n: an integer (for constructive interference)
θ: angle between light ray and row of particles

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7
Q

whats the scattering angle for Bragg scattering

A

2θ. (twice the angle between the light ray and the row of particles)

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8
Q

define quasistatic.

A

a process that happens so slowly that the system is always in instantaneous thermal equilibrium.

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9
Q

show how to relate the fractional volume change to the fractional d-spacing change for Bragg-scattering

A

nλ = 2d*sin(θ)
d= λ/2sin(θ) (use n= 1 for the scatter angle)
∂d/∂θ = -λcos(θ)/2sin²(θ) = -d/tan(θ)
∂d/d = -∂θ/tan(θ)

V∝d³
V = Ad³ (A is a constant of proportionality)
∂V/∂d = 3Ad²
∂V/V = 3* ∂d/d = -3 *∂θ/tan(θ)

this can be subbed into the Bulk modulus equation

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