File: README.md

package info (click to toggle)
apbs 3.4.1-7
  • links: PTS, VCS
  • area: main
  • in suites: forky, sid
  • size: 199,188 kB
  • sloc: ansic: 284,988; cpp: 60,416; fortran: 44,896; xml: 13,895; sh: 13,838; python: 8,105; yacc: 2,922; makefile: 1,428; f90: 989; objc: 448; lex: 294; awk: 266; sed: 205; java: 134; csh: 79
file content (103 lines) | stat: -rw-r--r-- 4,410 bytes parent folder | download | duplicates (3)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
README for Born APBS examples
=============================

This is the canonical electrostatics test case: Born ion. A non-polarizable ion with a single embedded point charge; has an analytical solution for the potential. We examine the solvation free energy as a function of ionic radius.

Please see apbs.in for details on the particular solvation energy calculations. Analytical results are given in pmf.dat.

This example was contributed by Nathan Baker.

Input File|Description|APBS Version|Results (kJ/mol)|Analytical (kJ/mol)
---|---|---|---|---
[apbs-mol-auto.in](apbs-mol-auto.in)|Sequential, 3 A sphere, 3-level focusing to 0.188 A, srfm mol|**1.5**|**-229.7740**|-230.62
|||1.4.2|-229.774
|||1.4.1|-229.7736|
|||1.4|-229.7736<sup>[3](#3)</sup>
|||1.3|-229.7735
|||1.2.1|-229.7735
|||1.2|-229.7735
|||1.1.0|-229.7735
|||1.0.0|-229.7735
|||0.5.1|-229.7735
|||0.5.0|-229.7735
|||0.4.0|-229.7735<sup>[1](#1)</sup>
|||0.3.2|-229.7248
|||0.3.1|-229.7248
|||0.3.0|-229.7248
|||0.2.6|-229.7248
|||0.2.5|-229.7248
|||0.2.4|-227.1859
|||0.2.3|-227.1589
|||0.2.2|-227.186
|||0.2.1|-227.19
|||0.2.0|-227.19
|||0.1.8|-227.19
[apbs-smol-auto.in](apbs-smol-auto.in)|Sequential, 3 A sphere, 3-level focusing to 0.188 A, srfm smol|**1.5**|**-229.012**|-230.62
|||1.4.2|-229.0124
|||1.4.1|-229.0124
|||1.4|-229.0124
|||1.3|-229.0124
|||1.2.1|-229.0124
|||1.2|-229.0124<sup>[2](#2)</sup>
|||1.1.0|-229.0123
|||1.0.0|-229.0123
|||0.5.1|-229.0123
|||0.5.0|-229.0123
|||0.4.0|-229.0123
[apbs-mol-parallel.in](apbs-mol-parallel.in)|Parallel with 4 processors, 3 A sphere, focusing to 0.103 A, srfm mol|**1.5**|**-230.492**|-230.62
|||1.4.2|-230.492
|||1.4.1|-230.4918<sup>[4](#4)</sup>|
|||1.4|-230.4919<sup>[3](#3)</sup>
|||1.3|-230.4918
|||1.2.1|-230.4918
|||1.2|-230.4918<sup>[2](#2)</sup>
|||1.1.0|-230.4916
|||1.0.0|-230.4916
|||0.5.1|-230.4916
|||0.5.0|-230.4916
|||0.4.0|-230.4916
|||0.2.1|-230.77
[apbs-smol-parallel.in](apbs-smol-parallel.in)|Parallel with 4 processors, 3 A sphere, focusing to 0.103 A, srfm smol|**1.5**|**-229.387**|-230.62
|||1.4.2|-229.387
|||1.4.1|-229.3871
|||1.4|-229.3871
|||1.3|-229.3871
|||1.2.1|-229.3871
|||1.2|-229.3871<sup>[2](#2)</sup>
|||1.1.0|-229.3872
|||1.0.0|-229.3872
|||0.5.1|-229.3872
|||0.5.0|-229.3872
|||0.4.0|-229.3872<sup>[1](#1)</sup>
|||0.3.2|-226.3529
|||0.3.1|-226.3529
|||0.3.0|-229.5849
|||0.2.6|-229.5849
|||0.2.5|-229.5849
|||0.2.4|-226.2276
|||0.2.3|-226.2276
|||0.2.2|-226.2276
|||0.2.0|-226.228
|||0.1.8|-226.23
[apbs-smol-parallel.in](apbs-mol-fem.in)|Finite Element Method, 3 A sphere, 3-level focusing to 0.188 A, srfm mol|**1.4.1-binary**|**-231.9550**|-230.62
[apbs-smol-parallel.in](apbs-smol-fem.in)|Finite Element Method, 3 A sphere, 3-level focusing to 0.188 A, srfm smol|**1.4.1-binary**|**-230.9760**|-230.62

<a name=1></a><sup>1</sup> The discrepancy in values between versions 0.4.0 and 0.3.2 is most likely due to three factors:

-   A bug fix in Vacc_molAcc which removed spurious regions of high internal dielectric values
-   A switch in the algorithm used to compute the dielectric smoothing for srfm smol.
-   The addition of the Vacc sphere density (sdens keyword) as a variable and a change in the default sdens value from 3.0 to 10.0

<a name=2></a><sup>2</sup> APBS 1.2 has switched the multigrid smoothing algorithm from standard Gauss-Seidel to Gauss-Seidel red/black in order to facilitate parallelization. This switch has caused small differences in individual calculation energies which, when combined to the final answer, create larger errors (up to 0.04%). These errors can be reduced by resetting the APBS error tolerance to 1e-9 or smaller values. For a more detailed explanation, please see the APBS FAQ, [here](http://www.poissonboltzmann.org/docs/apbs-faq/#sources error calculation).

<a name=3></a><sup>3</sup> The discrepancy in values between versions 1.3 and 1.4 is most likely due to the following factor(s):

-   Translation of contrib/pmgZ library from FORTRAN to C
-   Differences in numerical implementations between FORTRAN and C compilers result in small round-off discrepencies
-   Small margins due to these round-off discrepencies acumulate in the computations

<a name=4></a><sup>4</sup> The discrepancy in the result between versions 1.4 and 1.4.1-binary is most likely due to a reporting error.

Please see the ChangeLog or the [APBS website](http://www.poissonboltzmann.org/) for more information.