I have the following code generated in Mathematica 7. When I DSolve it in Mathematica 7, the imaginary parts of the solution are really low-valued. As a result, I can easily chop them and plot the results. However, the same operation does not give low values for the imaginary parts in Mathematica 10.4 and the results cannot be plotted.
Here is the code.
Ef = 220000; bf = 1; tf = 0.167; Af = bf*tf;
EA = Ef*Af; EI = 100; kt = 10; kr = 0.1; r = 25; GA =
100000*Af; \[Chi] = 1.2;
ut[s_];
ur[s_];
pt[s_] = kt*ut[s];
pr[s_] = kr*ur[s];
equ1 = n'[s] - T[s]/r + pt[s];
equ2 = T'[s] + n[s]/r + pr[s];
equ3 = M'[s] - T[s];
eps[s_] = ut'[s] - ur[s]/r;
\[Gamma]s[s_] = ur'[s] + ut[s]/r + \[Phi][s];
k[s_] = \[Phi]'[s];
equ4 = eps[s] - n[s]/EA;
equ5 = k[s] + M[s]/EI;
equ6 = \[Gamma]s[s] - (\[Chi]*T[s])/GA;
an = DSolve[{equ1 == 0, equ2 == 0, equ3 == 0, equ4 == 0, equ5 == 0,
equ6 == 0,
n[0] - F == 0, n[\[Pi]/2*r] - F == 0,
ut[0] == 0, ur[0] == 0, ut[\[Pi]/2*r] == 0,
ur[\[Pi]/2*r] == 0}, {n[s], T[s], M[s], ut[s], ur[s], \[Phi][s]},
s];
n[s_] = Chop[n[s] /. an[[1, 2]]];
Plot[n[s], {s, 0, \[Pi]/2*r}]
The results of different versions of Mathematica for the solution of the differential equation is:
Mathematica 7:
{{n[s] ->
E^(-0.345376 s) ((1.19981 - 1.91926*10^-16 I) E^(0.128248 s)
F + (0.000237717 + 9.04032*10^-19 I) E^(0.562504 s)
F + (0.00798872 + 2.12516*10^-17 I) E^(0.473623 s)
F Cos[0.204351 s] - (0.208036 - 1.6977*10^-16 I) E^(
0.217128 s)
F Cos[0.204351 s] + (6.72924*10^-6 - 2.64133*10^-17 I) E^(
0.473623 s)
F Sin[0.204351 s] + (1.21171 - 1.21342*10^-16 I) E^(
0.217128 s) F Sin[0.204351 s]),
T[s] -> E^(-0.345376 s) ((0.153989 - 2.46326*10^-17 I) E^(
0.128248 s) F - (0.0000305097 + 1.16027*10^-19 I) E^(
0.562504 s) F - (0.000441035 + 9.1325*10^-18 I) E^(0.473623 s)
F Cos[0.204351 s] + (0.217962 - 2.29161*10^-17 I) E^(
0.217128 s)
F Cos[0.204351 s] - (0.00151332 + 1.9483*10^-17 I) E^(
0.473623 s)
F Sin[0.204351 s] + (0.106487 - 2.85166*10^-17 I) E^(
0.217128 s) F Sin[0.204351 s]),
M[s] -> E^(-0.345376 s) ((-0.709208 + 1.13448*10^-16 I) E^(
0.128248 s) F - (0.000140515 + 5.34374*10^-19 I) E^(0.562504 s)
F + (0.0043412 + 2.14946*10^-17 I) E^(0.473623 s)
F Cos[0.204351 s] - (0.85409 - 2.14849*10^-16 I) E^(
0.217128 s)
F Cos[0.204351 s] - (0.00488269 + 7.14507*10^-17 I) E^(
0.473623 s)
F Sin[0.204351 s] + (0.53059 + 1.99297*10^-17 I) E^(
0.217128 s) F Sin[0.204351 s]),
ut[s] -> E^(-0.345376 s) ((0.0266672 - 4.26578*10^-18 I) E^(
0.128248 s) F - (5.28354*10^-6 + 2.00932*10^-20 I) E^(
0.562504 s) F - (0.000104355 + 1.08889*10^-18 I) E^(0.473623 s)
F Cos[0.204351 s] - (0.0265575 - 5.37477*10^-18 I) E^(
0.217128 s)
F Cos[0.204351 s] + (0.000157111 + 4.80885*10^-19 I) E^(
0.473623 s)
F Sin[0.204351 s] + (0.0117146 - 3.91483*10^-19 I) E^(
0.217128 s) F Sin[0.204351 s]), \[Phi][s] ->
E^(-0.345376 s) ((-0.0326632 + 5.22492*10^-18 I) E^(0.128248 s)
F + (6.47152*10^-6 + 2.4611*10^-20 I) E^(0.562504 s)
F - (0.00026707 + 2.52378*10^-18 I) E^(0.473623 s)
F Cos[0.204351 s] - (0.000190439 - 3.34787*10^-18 I) E^(
0.217128 s)
F Cos[0.204351 s] - (0.0000448289 - 1.24984*10^-18 I) E^(
0.473623 s)
F Sin[0.204351 s] + (0.0416757 - 5.1102*10^-18 I) E^(
0.217128 s) F Sin[0.204351 s]),
ur[s] -> E^(-0.345376 s) ((-0.145571 + 2.32861*10^-17 I) E^(
0.128248 s) F - (0.0000288419 + 1.09685*10^-19 I) E^(
0.562504 s) F + (0.000462626 - 6.46096*10^-18 I) E^(0.473623 s)
F Cos[0.204351 s] + (0.145137 - 1.67154*10^-17 I) E^(
0.217128 s)
F Cos[0.204351 s] + (0.00103685 + 2.53644*10^-18 I) E^(
0.473623 s)
F Sin[0.204351 s] + (0.097293 - 2.50601*10^-17 I) E^(
0.217128 s) F Sin[0.204351 s])}}
Mathematica 10.4:
{{M[s] -> (3.52596 +
3.28357 I) E^(-0.345376 s) ((0. - 1. I) E^(0.128248 s)
F + (0.00444174 + 0.0871541 I) E^(0.562504 s)
F - (0.392686 + 0.29177 I) E^(0.473623 s)
F Cos[0.204351 s] + (0.252446 - 1.54495 I) E^(0.217128 s)
F Cos[0.204351 s] + (1.60583 + 0.145085 I) E^(0.473623 s)
F Sin[0.204351 s] + (1.90461 - 0.0680882 I) E^(0.217128 s)
F Sin[0.204351 s]),
n[s] -> (5.96507 +
5.55501 I) E^(-0.345376 s) ((0. + 1. I) E^(0.128248 s)
F - (0.00444174 + 0.0871541 I) E^(0.562504 s)
F - (1.05642 + 0.218411 I) E^(0.473623 s)
F Cos[0.204351 s] + (1.15065 - 0.778044 I) E^(0.217128 s)
F Cos[0.204351 s] + (0.558183 - 0.0881049 I) E^(0.473623 s)
F Sin[0.204351 s] + (0.777341 + 0.802445 I) E^(0.217128 s)
F Sin[0.204351 s]),
T[s] -> (0.765583 +
0.712954 I) E^(-0.345376 s) ((0. + 1. I) E^(0.128248 s)
F + (0.00444174 + 0.0871541 I) E^(0.562504 s)
F + (1.27939 - 0.0357876 I) E^(0.473623 s)
F Cos[0.204351 s] + (1.64343 + 0.848452 I) E^(0.217128 s)
F Cos[0.204351 s] + (1.31807 + 0.360296 I) E^(0.473623 s)
F Sin[0.204351 s] - (1.36256 - 1.49426 I) E^(0.217128 s)
F Sin[0.204351 s]),
ur[s] -> (0.723733 +
0.673981 I) E^(-0.345376 s) ((0. - 1. I) E^(0.128248 s)
F + (0.00444174 + 0.0871541 I) E^(0.562504 s)
F - (1.10206 + 0.0102304 I) E^(0.473623 s)
F Cos[0.204351 s] + (1.38147 + 0.486021 I) E^(0.217128 s)
F Cos[0.204351 s] - (0.862745 + 0.275686 I) E^(0.473623 s)
F Sin[0.204351 s] - (0.858699 - 1.21572 I) E^(0.217128 s)
F Sin[0.204351 s]),
ut[s] -> (0.132581 +
0.123467 I) E^(-0.345376 s) ((0. + 1. I) E^(0.128248 s)
F + (0.00444174 + 0.0871541 I) E^(0.562504 s)
F + (0.125917 + 0.206204 I) E^(0.473623 s)
F Cos[0.204351 s] - (0.0128045 + 1.16713 I) E^(0.217128 s)
F Cos[0.204351 s] - (1.26293 + 0.141651 I) E^(0.473623 s)
F Sin[0.204351 s] + (1.47499 - 0.217812 I) E^(0.217128 s)
F Sin[0.204351 s]), \[Phi][
s] -> (0.162391 +
0.151227 I) E^(-0.345376 s) ((0. - 1. I) E^(0.128248 s)
F - (0.00444174 + 0.0871541 I) E^(0.562504 s)
F + (1.41196 + 0.250179 I) E^(0.473623 s)
F Cos[0.204351 s] + (1.57263 - 0.791006 I) E^(0.217128 s)
F Cos[0.204351 s] - (0.468887 - 0.153003 I) E^(0.473623 s)
F Sin[0.204351 s] + (0.71873 + 1.14512 I) E^(0.217128 s)
F Sin[0.204351 s])}}
As it is obvious the imaginary parts for the result of Mathematica 7 are negligible. While in the case of Mathematica 10.4 Chop does not do anything and the imaginary parts are significant.
F
so your code cannot be evaluated.Rationalize
all of the inexact numbers prior toDSolve
, UsingF=1;
theChop
is not necessary and the plot evaluates successfully with version 10.4.1. $\endgroup$