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--- documentation:ref:reduce [2015/11/21 12:33]
+++ documentation:ref:reduce [2015/11/21 12:33] (current)
@@ Line 1: / Line 1: @@
+====== Reduce ======
+----
+====Description====
+  * ''Reduce(equations, vars)'' reduces a system of tensorial equations to a system of symbolic equations.
+  * ''Reduce(equations, vars, options)'' allows to pass additional [[#Options|options]] .
+  * ''Reduce'' allows to completely solve a system of equations using external system (Maple or Mathematica).
+====Examples====
+Reduce a system of tensorial equations:
+<sxh groovy; gutter: false>
+def eq1 = 'F_mn + F_nm + A_mn + A_nm = 0'.t
+def eq2 = 'F_mn/2 + A_nm/2 = F_nm + A_mn '.t
+def reduced = Reduce([eq1, eq2], ['F_mn'])
+println reduced
+</sxh>
+<sxh plain; gutter: false>
+   > [F_{mn} = C[0]*g_{mn}+C[1]*A_{mn}+C[2]*A_{nm}, 1+C[1]+C[2] = 0,
++C[1]+C[2] = 0, 2*C[0] = 0, -1-C[2]+(1/2)*C[1] = 0,
+/2-C[1]+(1/2)*C[2] = 0, -(1/2)*C[0] = 0]
+</sxh>
+Solve it using Wolfram Mathematica:
+<sxh groovy; gutter: false>
+def options = [ExternalSolver: [Solver: 'Mathematica', Path: '/usr/local/bin']]
+println Reduce([eq1, eq2], ['F_mn'], options)
+</sxh>
+<sxh plain; gutter: false>
+   > [[F_{mn} = -A_{nm}]]
+</sxh>
+----
+Solve a system of equations with special symmetries of unknown tensor:
+\[
+\left\{
+\begin{array}{l}
+T^{abe}{}_{rba}-x\,T^{bea}{}_{rba} = 8\,d_{r}^{e}\\
+T^{pqr}{}_{klm} T^{abc}{}_{pqr} = d^{a}_{m}\,g^{bc}\,g_{lk}
+\end{array}
+\right.
+\]
+where \(x\) and \(T^{abe}{}_{rba}\) are unknown variables and the last one has [[documentation:guide:symmetries_of_tensors|symmetry]] [1, 5, 0, 4, 3, 2] (in one-line notation).
+Redberry code:
+<sxh groovy; gutter: true>
+//setting up symmetries
+addSymmetry 'T^abc_pqr', [1, 5, 0, 4, 3, 2].p
+def eq1 = 'T^{abe}_{rba}-x*T^{bea}_{rba} = 8*d_{r}^{e}'.t
+def eq2 = 'T^{pqr}_{klm}*T^{abc}_{pqr} = d^{a}_{m}*g^{bc}*g_{lk}'
+def options = [Transformations: 'd_n^n = 4'.t, ExternalSolver:
+                  [Solver: 'Mathematica',
+                   Path: '/usr/local/bin']]
+def s = Reduce([eq1, eq2], ['T^abc_pqr', 'x'], options)
+println s
+</sxh>
+<sxh plain; gutter: false>
+   > [[T^{abc}_{pqr} = -d^{a}_{r}*g^{cb}*g_{qp}, x = 12],
+      [T^{abc}_{pqr} = d^{a}_{r}*g^{cb}*g_{qp}, x = -4]]
+</sxh>
+----
+[[documentation:ref:generatetensor|Generate]] and find projection operator:
+\[
+\left\{
+\begin{array}{l}
+J_{ab cd}\,J^{ab pq} = J_{ab}{}^{pq}\\
+J_{abcd}\,J^{acbd} = \frac{1}{2}\,J^a{}_{ba}{}^b\\
+J_a{}^{abc} = 0
+\end{array}
+\right.
+\]
+with [[documentation:guide:symmetries_of_tensors|symmetries]]
+\[J_{abcd} = J_{cd ab} \quad \mbox{and} \quad J_{ab cd} = J_{ba cd}\]
+Redberry code:
+<sxh groovy; gutter: true>
+//setting up symmetries of tensors
+addSymmetry 'J_abcd', 1, 0, 2, 3
+addSymmetry 'J_abcd', 2, 3, 0, 1
+//generate solution of the most general tensorial form
+// and store the coefficients
+def coefs = []
+def genTensor =
+    GenerateTensor('_{ab cd}'.si, ['g_mn', 'k_m'],
+     [GeneratedParameters: { i -> coefs << "C$i".t; "C$i".t }])
+def equations = [
+   'J_{ab cd}*J^{ab pq} = J_{cd}^{pq}',
+   'J_abcd*J^acbd = J^a_ba^b/2',
+   'J_a^acd = 0',
+   'J_abcd'.eq(genTensor)]
+def options = [
+    Transformations: 'd_m^m = 4'.t & 'k_m*k^m = M**2'.t, //additional simplifications
+    ExternalSolver: [
+        Solver: 'Maple',
+        Path: '/home/stas/maple13/bin']]
+def s = Reduce(equations, ['J_abcd'.t, * coefs], options)
+def result = s.collect { it[0] }
+println result
+</sxh>
+<sxh plain; gutter: false>
+   > [J_{abcd} = 0,
+          J_{abcd} = -2*M**(-4)*k_{a}*k_{b}*k_{c}*k_{d}
+           +(1/2)*M**(-2)*g_{bc}*k_{a}*k_{d}
+           +(1/2)*M**(-2)*g_{ac}*k_{b}*k_{d}
+           +(1/2)*M**(-2)*g_{ad}*k_{b}*k_{c}
+           +(1/2)*M**(-2)*g_{bd}*k_{a}*k_{c}]
+</sxh>
+====Options====
+  * ''Transformations'': specify transformation rules that will be used in Reduce to simplify the resulting system. \\ Consider system:\[
+\left\{
+\begin{array}{l}
+J_{ac} J^{ab} + 3\,J_c{}^b = -2\,d^{b}_{c}\\
+k^a J_{ab} = -k_b \\
+J_{ab} J^{ab} = 9
+\end{array}
+\right.
+\]This system have solutions only for particular space dimensions. \\ Redberry code:<sxh groovy; gutter: false>
+def eq1 = 'J_ac*J^ab + 3*J_c^b = -2*d^{b}_{c}'.t
+def eq2 = 'k^a*J_ab = -k_b'.t
+def eq3 = 'J_ab*J^ab = 9'.t
+def options = [Transformations: 'd_n^n = dim'.t, //here we specify dimension
+               ExternalSolver: [
+                    Solver: 'Mathematica',
+                    Path: '/usr/local/bin']]
+def s = Reduce([eq1, eq2, eq3], ['dim', 'J_ab'], options)
+println s
+</sxh>
+<sxh plain; gutter: false>
+   > [[dim = 9, J_{ab} = -g_{ab}],
+           [dim = 3, J_{ab} = -2*g_{ab}+(k^{c}*k_{c})**(-1)*k_{a}*k_{b}]]
+</sxh>
+  * ''SymmetricForm'':\\ by default, there is no assumptions on the symmetries of the solution. If SymmetricForm is true, then each unique term in the general solution will be putted into a symmetrized form.\\Consider equation:\[
+\frac{2}{3} \left( g_{cd} J_{b}{}^{bpq}+J_{dc}{}^{pq}+J_{cd}{}^{pq} \right)= \frac{1}{2} \left(d_{c}{}^{q} d_{d}{}^{p}+ d_{c}{}^{p} d_{d}{}^{q}\right) + 2\,g_{cd} g^{pq}
+\]By default its general solution contains a free parameter (''C[0]'' in the following example):<sxh groovy; gutter: false>
+def eq = '''(2/3)*(J_{b}^{bpq}*g_{cd}+J_{dc}^{pq}+J_{cd}^{pq}) =
+          (1/2)*(d_{c}^{q}*d_{d}^{p}+d_{c}^{p}*d_{d}^{q})
+                                      +2*g_{cd}*g^{pq}'''.t
+def options = [Transformations: 'd^m_m = 4'.t,
+               ExternalSolver: [
+                    Solver: 'Mathematica',
+                    Path: '/usr/local/bin']]
+def s = Reduce([eq], ['J_abcd'], options)
+println s
+</sxh><sxh plain; gutter: false>
+   > [[J_{abcd} =
+           (-C[0]+3/4)*g_{ac}*g_{bd}+C[0]*g_{ad}*g_{bc}+(3/8)*g_{ab}*g_{cd}]]
+</sxh>If ''SymmetricForm'' is true then a unique symmetric solution will be found:<sxh groovy; gutter: false>
+def options = [Transformations: 'd^m_m = 4'.t,
+               SymmetricForm: [true],
+               ExternalSolver: [
+                    Solver: 'Mathematica',
+                    Path: '/usr/local/bin']]
+def s = Reduce([eq], ['J_abcd'], options)
+println s
+</sxh>
+<sxh plain; gutter: false>
+   > [[J_{abcd} =
+            (3/8)*(g_{ad}*g_{bc}+g_{ab}*g_{cd}+g_{ac}*g_{bd})]]
+</sxh>
+  * ''GeneratedParameters'': \\ ''Reduce'' introduces new parameters to represent the solution:<sxh groovy; gutter: false>
+println Reduce(['F_mn + F_nm + A_mn + A_nm= 0'], ['F_mn'])
+</sxh><sxh plain; gutter: false>
+   > [F_{mn} = C[0]*g_{mn}+C[1]*A_{mn}+C[2]*A_{nm},
+*C[0] = 0, C[2]+C[1]+1 = 0, C[2]+C[1]+1 = 0]
+</sxh>Use ''GeneratedParameters'' to control how the parameters are generated:
+<sxh groovy; gutter: false>
+println Reduce(['F_mn + F_nm + A_mn + A_nm= 0'],
+            ['F_mn'], [GeneratedParameters: { i -> "X$i" }])
+</sxh> <sxh plain; gutter: false>
+   > [F_{mn} = X0*g_{mn}+X1*A_{mn}+X2*A_{nm},
+*X0 = 0, X2+X1+1 = 0, X2+X1+1 = 0]
+</sxh>
+  * ''ExternalSolver'':\\ should be specified to solve the symbolic system produced by ''Reduce''. External sover have several options:
+     * ''Solver'' :(required) At the moment there are two supported external systems: Maple and Mathematica.
+     * ''Path'' :(required) Path to directory that contains external solver executables.
+     * ''KeepFreeParams'' : By default the most general solution will be returned, which can contain some free parameters. If ''KeepFreeParams'' set to false, then only one representative from each family of solutions will be taken.
+     * ''TmpDir'' : Path to temporary directory where generated Maple (or Mathematica) files wil be putted.
+====See also====
+  * Related guides: [[documentation:guide:tensors_and_indices]], [[documentation:guide:symmetries_of_tensors]]
+  * Related reference material: [[documentation:ref:generatetensor]], [[documentation:ref:simpleindices]]
+  * JavaDocs: [[http://api.redberry.cc/redberry/1.1.9/java-api/cc/redberry/core/solver/ReduceEngine.html|ReduceEngine]]
+  * Source code: [[https://bitbucket.org/redberry/redberry/src/tip/core/src/main/java/cc/redberry/core/solver/ReduceEngine.java|ReduceEngine.java]]