| METHOD: |
NVT Monte Carlo |
| N: |
500 |
| TRUNCATION: |
3σ + standard long range corrections |
| EQUILIBRATION: |
5.0E7 trials |
| PRODUCTION: |
2.5E8 trials |
|
| T* |
ρ* |
U* |
+/- |
p* |
+/- |
| 8.50E-01 |
1.00E-03 |
-1.0317E-02 |
2.34E-05 |
8.4402E-04 |
4.66E-08 |
| 8.50E-01 |
3.00E-03 |
-3.1019E-02 |
5.91E-05 |
2.4965E-03 |
4.99E-07 |
| 8.50E-01 |
5.00E-03 |
-5.1901E-02 |
7.53E-05 |
4.1003E-03 |
5.05E-07 |
| 8.50E-01 |
7.00E-03 |
-7.2834E-02 |
1.34E-04 |
5.6565E-03 |
7.96E-07 |
| 8.50E-01 |
9.00E-03 |
-9.3973E-02 |
1.29E-04 |
7.1641E-03 |
2.24E-06 |
| 8.50E-01 |
7.76E-01 |
-5.5121E+00 |
4.55E-04 |
6.7714E-03 |
1.77E-03 |
| 8.50E-01 |
7.80E-01 |
-5.5386E+00 |
7.26E-04 |
4.7924E-02 |
3.18E-03 |
| 8.50E-01 |
8.20E-01 |
-5.7947E+00 |
6.03E-04 |
5.5355E-01 |
4.13E-03 |
| 8.50E-01 |
8.60E-01 |
-6.0305E+00 |
2.38E-03 |
1.2660E+00 |
1.36E-02 |
| 8.50E-01 |
9.00E-01 |
-6.2391E+00 |
5.27E-03 |
2.2314E+00 |
2.72E-02 |
| 9.00E-01 |
1.00E-03 |
-9.9165E-03 |
1.89E-05 |
8.9429E-04 |
2.48E-08 |
| 9.00E-01 |
3.00E-03 |
-2.9787E-02 |
3.21E-05 |
2.6485E-03 |
2.54E-07 |
| 9.00E-01 |
5.00E-03 |
-4.9771E-02 |
3.80E-05 |
4.3569E-03 |
2.19E-07 |
| 9.00E-01 |
7.00E-03 |
-6.9805E-02 |
7.66E-05 |
6.0193E-03 |
1.02E-06 |
| 9.00E-01 |
9.00E-03 |
-8.9936E-02 |
2.44E-05 |
7.6363E-03 |
1.44E-06 |
| 9.00E-01 |
7.76E-01 |
-5.4689E+00 |
4.20E-04 |
2.4056E-01 |
2.74E-03 |
| 9.00E-01 |
7.80E-01 |
-5.4956E+00 |
7.86E-04 |
2.7851E-01 |
2.97E-03 |
| 9.00E-01 |
8.20E-01 |
-5.7456E+00 |
7.51E-04 |
8.2386E-01 |
2.85E-03 |
| 9.00E-01 |
8.60E-01 |
-5.9753E+00 |
5.53E-04 |
1.5781E+00 |
3.29E-03 |
| 9.00E-01 |
9.00E-01 |
-6.1773E+00 |
1.57E-03 |
2.5848E+00 |
9.54E-03 |
|
Remarks:
Uncertainties were obtained from block averages of 5.0E7 trials and
correspond to 67% confidence limits (one standard deviation). The
maximum particle displacement was adjusted to maintain an acceptance
ratio of 0.40. The pressure was calculated using the virial expression.
|