T= 0.75 Quenches

We present the results of the systems quenched to a reduced temperature of 0.75. Each set of results have been averaged over two different initial configurations. You may view the overall results for each initial configuration: set 1, set 2.



F3-2 Run: phi0=0.68 T=0.75 N=150

Initially unstable with respect to PS only.


PS significant by t=6. PO significant by t=14. See separate analysis on this quench.

Resulting intermediate/late-time structure: Elongated LC-rich domains (minor phase) in a polymer-rich matrix (major phase). View phi and S profiles.

F3-2-pk2b-avr1sc.pl2bsh.GIF


#1: "new" k1 -- from phi-based S(k).





H21-2 Run: phi0=0.75 T=0.75 N=150

Initially unstable with respect to PS only.


PS significant by t=. PO significant by t=. See separate analysis on this quench.

Resulting intermediate/late-time structure: Elongated polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

H21-2-pk2b_r1sc.pl2sh.GIF


#1: new" k1 -- from phi-based S(k).





H41-2 Run: phi0=0.80 T=0.75 N=150

Initially unstable with respect to PS only.


PS significant by t=. PO significant by t=. See separate analysis on this quench.

Resulting intermediate/late-time structure: Elongated polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

.GIF


#1: new" k1 -- from phi-based S(k).





F6-2 Run: phi0=0.83 T=0.75 N=150

Initially unstable with respect to PS only.


PS significant by t=6. PO significant by t=8. See separate analysis on this quench.

Resulting intermediate/late-time structure: Elongated polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

F6-2-pk2b-avr1sc.pl2sh.GIF


#2: new" k1 -- from phi-based S(k).





F2-2 Run: phi0=0.84 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PS.


PS significant by t=6. PO significant by t=8. See separate analysis on this quench.

Resulting intermediate/late-time structure: Elongated and noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

F2-2-pk2b-avr1sc.pl2bsh.GIF


#3: new" k1 -- from phi-based S(k).





C2-1 Run: phi0=0.85 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PS.


Both PS and PO well-established by t=5. See separate analysis on this quench.

Resulting intermediate/late-time structure: Noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

C2-1all-kone_2a+2b-p.pl1sh.GIF


#1: "old" k1 vs. "new" k1: using phi-based S(k).
"old" k1: R ~ t1/2 --> t1/3; "new" k1: R ~ t1/3 --> slower than t1/3.
We focus on our "new" k1 results. Initially, domain growth appears to have a t1/3 growth law (Model B). Growth slows down around t=20, but PS and PO both well-established by t=5. What causes the slowing down? Should we even get t1/3 behavior? Perhaps the initial behavior is transient and the only significant result is the eventual slowing down of domain growth due to the coupling of PS and PO. But why don't we see this "intermediate" behavior for quenches that are unstable wrt PS and PO, but more unstable wrt PO? Maybe the rate at which ordering occurs becomes faster than the rate at which PS occurs at t~20, causing domain growth to slow down. This would not be observed in quenches like E7-2 (unstable wrt PS and PO, but more unstable wrt PO), since for such a quench, the rate at which ordering happens already exceeds the rate at which PS happens. How can we check this?
Note: Initial growth behavior is actually slightly faster than t1/3. (See below.)




F5-2all Run: phi0=0.86 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PO.


PS significant by t=3. PO significant by t=2. See separate analysis on this quench.

Resulting intermediate/late-time structure: Noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

F5-2all-pk2b-avr1sc.pl1bsh.GIF


#4: new" k1 -- from phi-based S(k).




F1-2 Run: phi0=0.87 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PO.


PS significant by t=1.4. PO significant by t=1.4. See separate analysis on this quench.

Resulting intermediate/late-time structure: Noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

F1-2-pk2b-avr1sc.pl1csh.GIF


#5: new" k1 -- from phi-based S(k).





F4-2 Run: phi0=0.88 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PO.


PS significant by t=0.30. PO significant by t=0.27. See separate analysis on this quench.

Resulting intermediate/late-time structure: Noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase). View phi and S profiles.

F4-2-pk2b-avr1sc.pl1csh.GIF


#6: new" k1 -- from phi-based S(k).




E7-2 Run: phi0=0.89 T=0.75 N=150

Initially unstable with respect to PS and PO, but more unstable with respect to PO.


Both PS and PO well-established by t~0.02. See separate analysis on this quench.

Resulting intermediate/late-time structure: Noncircular polymer-rich domains (minor phase) in a LC-rich matrix (major phase).View phi and S profiles.

E7-2all-p_k2b-r1sc.pl1csh.GIF


#1: "new" k1 -- from phi-based S(k): R ~ t0.18 (~ t1/5.6)
Domain growth slower than t1/3 immediately; no "intermediate" t1/3 behavior. Significant ordering from the start causes domain growth to slow down from the start.
Although our calculated power law produces a good fit to our data, this system does not exhibit true scaling behavior, except maybe towards the end of this time frame.




Jump to the individual results of the quench with (phi0, T, N) of:

A2: 0.76, 0.95, 100 A21-2: 0.76, 0.95, 150 A4: 0.68, 0.95, 100 A4-1: 0.68, 0.95, 150 A41-250-2: 0.68, 0.95, 250
F31-2: 0.68, 0.75, 150 H21-2: 0.75, 0.75, 150 H41-2: 0.80, 0.75, 150 F61-2: 0.83, 0.75, 150 F21-2: 0.84, 0.75, 150
C2-1: 0.85, 0.75, 150 C21-250-2: 0.85, 0.75, 250 F5-2: 0.86, 0.75, 150 F11-2: 0.87, 0.75, 150 F4a-2: 0.88, 0.75, 150
E7-2: 0.89, 0.75, 150 E71-250-2: 0.89, 0.75, 250 G11-2: 0.68, 0.85, 150 H11-2: 0.75, 0.85, 150 H31-2: 0.80, 0.85, 150
G21-2: 0.83, 0.85, 150 G31-2: 0.84, 0.85, 150 G41-2: 0.85, 0.85, 150 G51-2: 0.86, 0.85, 150 G61-2: 0.87, 0.85, 150

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Last updated August 1, 1999.