Scott wrote:
> My integral has several pieces  like this:
>
> int^x1_x0 int ^t0_t1 (dot(del_a(t)).T* R *b ) dt dx
>
> del_a is 3*1, b is 3*1 and R is 3*3 rotation tensor( or a non
> orthogonal velocity transformation tensor H)
>
> R,H and b are are constant over the interval of integration.
> R=H inv(H.T)
>
> My goal is to perform symbolic manipulations, plug in basis functions
> and do collections  in del_a R b form while preserving the vector
> orientations.
>
> With del_a linear (C1) in time the answer should be: (x1-x0)(del_a
> (t1).T-del_a(t0).T)* R* b =  scalar
> At this time all the pieces are added together and collected wrt the
> del terms yielding a nonlinear system.  At this point the  tensors are
> populated.
>
> On Dec 1, 3:28 pm, Scott<scotta_2...@yahoo.com>  wrote:
>    
>> Is there a sympy function for making symbolic tensors?
>> Basically I want to treat 3x3 rotation tensor symbol that is constant
>> inside of an integral while preserving the tensor algebra (A*B .ne.
>> B*A).  The 3x3 rotain tensor is multiplied by a 3x1 position tenosr
>> which is integrated.
>>
>>   Is there a built in function for converting a 3*1  tensor to a skew
>> antisymetric cross product matrix then back again?
>> V/R
>>
>> Scott
>>      
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>    
Where is the position (x) dependence in the intergrand?

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