Lecture 6 Flashcards

1
Q

What is interfacial energy proportional to for homogenous nucleation?

A

r^2

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2
Q

What is interfacial energy?

A

The resistance energy to forming a new phase between a new nucleus and the surrounding phase

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3
Q

Explain undercooling

A

Undercooling is when you have to cool a material past it’s “Tm” for it to ACTUALLY solidify because in reality there’s an energy barrier that it has to overcome to start forming nuclei

  • the difference between that ACTUAL temp and the Tm is the ΔT=Tm -T and ΔT is undercooling
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4
Q

What is the homogenous nucleation rate?

A

Nhom - the number of stable nuclei formed per second per m^3

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5
Q

How do you find the homogenous nucleation rate? What happens if the ΔG*hom increases?

A

**find C* - the number of nuclei per m^3 that have reached critical size, then plug that number into the Nhom equation

  • ΔG*hom increases, nucleation decreases
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6
Q

What is a good approximation for reasonable homogenous nucleation? Is nucleation easier at higher or lower temperatures?

A

Nucleation is easier at higher temperatures if there’s a small enough energy barrier -ΔGhom∗ or great enough Gv (bulk free energy change)

  • Gv in denom of formula to calculate ΔGhom*
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7
Q

What is different about the nucleation rate formula that you need to use for solidification or freezing (liquid –> solid)?

A

The A – determines how strongly the nucleation factor depends on cooling

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8
Q

When should you use this equation?

A
  1. for solidification
  2. working with supercooled liquids
  3. problem asks for effect of temp on nucleation
  4. determine how much undercooling is required for nucleation
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9
Q

For homogenous nucleation, what is ΔHm and how does it affect nucleation? Y sub SL? How does undercooling affect it?

A

ΔHm is the latent heat of fusion - high ΔHm then easier nucleation

Y sub SL is large - nucleation difficult (small easier)

since its (ΔT)^2 in the formula for Nhom, nucleation rate increases very sharply over a small undercooling temp/window (very steep graph)

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10
Q

What is ΔT sub N? What does it look like on a graph?

A

critical supercooling for detectable nucleation

  • the supercooling it needs for nucleation to happen
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11
Q

Explain ΔGv

A
  1. ΔGv<0
  2. ΔGv is ΔG per volume between S and L
  3. bulk free energy change per unit volume at phase transformation
  4. driving force of nucleation
  5. has to be negative bc nucleation happens when a system lowers its total energy – so that means that the liquid phase has higher energy than the solid
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11
Q

How is the Gibbs free energy change for het dif than a hom?

A

the negative makes it so that the presence of a solid-mould interface reduces the energy barrier

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11
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12
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