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Andrew Dougherty Franklin Stinner (‘11) Physics Department Lafayette College, Easton PA http://sites.lafayette.edu/doughera Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

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Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride. Andrew Dougherty Franklin Stinner (‘11). Physics Department Lafayette College, Easton PA http://sites.lafayette.edu/doughera. Experiments. NH 4 Cl growing in aqueous solution Growth cell: 40 x 10 x 2 mm 3 - PowerPoint PPT Presentation

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Page 1: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Andrew DoughertyFranklin Stinner (‘11)

Physics DepartmentLafayette College, Easton PA

http://sites.lafayette.edu/doughera

Sidebranching in theDendritic Crystal Growth of

Ammonium Chloride

Page 2: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Experiments• NH4Cl growing in aqueous solution

• Growth cell: 40 x 10 x 2 mm3

• Obtain an approximately spherical seed.• Lower temperature T (~1oC) to initiate slow

growth.

Page 3: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Apparatus

Page 4: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Growth from a Nearly Spherical Seed

Page 5: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 6: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Apparent tip oscillations – note the regular sidebranches close to the tip.However – such patterns are only rarely seen in this experiment, and we have not found any way to repeat them.

Page 7: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Typical sidebranches—note the long smooth tip and the slightly irregular branches.

Page 8: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 9: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Noise-induced Sidebranch Amplitude

2/1

2

3

0 *3)(

32exp)(

zzwSzA ave

202*

vDd

1/24

0 2 4

2 1 10( )

eqL

eq

C DSC v

wave(z) = average shape of the dendrite.

Page 10: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Determining Materials Constants

d0: Capillary length: Measure the very slow growth and dissolution of an initially spherical seed.

v, and : Measure the tip of steady-state growing dendrites.

Page 11: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Finding d0: Modeling the initial growth

TTdTd

Rd

RD

dtdR

eq

where2 0

Assume quasi-static, diffusion-limited, spherically-symmetric growth:

•Increasing supersaturation increases growth rate.•Growth rate proportional to local concentration gradient.•Surface tension limits sharpness•Unstable equilibrium at Rc, the critical radius for nucleation.

•2d0//R term is very small; need to optimize the experimentalprotocol to determine d0

02dRc

Page 12: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Slow Growth of a Spherical Crystal

Page 13: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Modeling the initial growth

Page 14: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Fitting the Dendrite Tip

• First, model the tip, then look for sidebranches as deviations from the initially smooth tip.

• Approximate model for tip shape: (A4 -0.002)

• Measure tip position to determine v.

3

4

4

2)4cos(2

xAxz

Page 15: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Preliminary Results for Materials Constants

d0 (2.2 + 0.1)x10-4 m

d/dT 0.0043 + 0.0001/oC

v2 12.1 + 0.1 m2/s

* 0.093 + 0.008

Page 16: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Noise-induced Sidebranch Amplitude

2/1

2

3

0 *3)(

32exp)(

zzwSzA ave

202*

vDd

1/24

0 2 4

2 1 10( )

eqL

eq

C DSC v

wave(z) = average shape of the dendrite.

Page 17: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Average Shape: No single simple shape –Different Scaling Regimes:

• Near tip, w ~ z1/2

• Very far back, w ~ z1

• Intermediate region: w ~ z3/5 ? Actual scaling varies more continuously.

Page 18: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Average shape for 3 growth velocities. w ~ z0.6~0.8

Page 19: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 20: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 21: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Modeling Initial Sidebranches

Approximate model for initial sidebranches (all distances are scaled by :

zzAzmzmw

zzwzwdev2sin)()(

2)()(

2210

5/2)/(0)( szeSzA

Page 22: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 23: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 24: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride
Page 25: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Aggregated Fits for RMS Sidebranch Amplitude

Page 26: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Aggregated Fits for RMS Sidebranch Amplitude

Page 27: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Preliminary Fit Results forNoise Amplitude

S0 (expt) ~5 x 10-4

S0 (theory) ~1 x 10-4

Page 28: Sidebranching in the Dendritic Crystal Growth of Ammonium Chloride

Conclusions:• No velocity oscillations were observed during

normal steady-state growth.• The functional form of the sidebranch amplitude

is reasonably-well described by the noise-driven scenario.

• The amplitude of the sidebranches is slightly larger, but of the same order of magnitude as predicted by the noise-driven scenario.

Limitations: The most important limitations are precise characterizations of both wave and actual sidebranch amplitudes.