I How Can Tensors Be Evaluated to Scalars?

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Tensors are defined as multidimensional arrays that transform in specific ways, functioning mathematically as mappings from multidimensional arrays to real numbers. To evaluate a tensor to a scalar, one must perform successive contractions until all free indices are eliminated, resulting in a scalar value. It is emphasized that a tensor itself does not have a single real number assigned to it without specific arguments. The components of a tensor can be interpreted as contractions with particular basis vectors and covectors in a chosen reference frame. Understanding these concepts requires further study of tensor mathematics.
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Many descriptions of tensors define them to be these kind of multidimensional arrays of numbers, as generalizations of vectors and matrices, that transform in a certain way. But, mathematically, tensors are functions whose domains are these multidimensional arrays and whose codomains/ranges are the real numbers.

My question: Is there a general rule to evaluate any tensor, to determine the real number that is assigned to it? Perhaps by successive contractions, until it becomes a scalar?

Thanks in advance.
 
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No. You cannot represent any function as a single real number (unless the domain is a single point or the function is a constant). The number depends on the arguments.
 
LarryS said:
the real number that is assigned to it?
I am not sure what you mean by this. There is a real number assigned to ##T^{\mu\nu…}a_\mu b_\nu …## but there is no number assigned to ##T^{\mu\nu…}##
 
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Dale said:
I am not sure what you mean by this. There is a real number assigned to ##T^{\mu\nu…}a_\mu b_\nu …## but there is no number assigned to ##T^{\mu\nu…}##
I think I see where you are going. I probably need to read/study this subject a little further.
 
LarryS said:
Perhaps by successive contractions, until it becomes a scalar?
That is the only way to get a scalar from a tensor, yes: by contracting it, either with itself or with appropriate other tensors, so that there are no free indexes left and you have a scalar.

What are usually called the "components" of a tensor can be viewed as contractions of that tensor with appropriate combinations of basis vectors and covectors of a particular reference frame.
 
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