How Can Tensors Be Evaluated to Scalars?

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The discussion centers on the evaluation of tensors to scalars, emphasizing that tensors are functions defined over multidimensional arrays that yield real numbers based on their arguments. It is established that a tensor cannot be represented as a single real number unless its domain is a single point or constant. The only method to derive a scalar from a tensor is through successive contractions, either with itself or with other tensors, ensuring all free indices are eliminated.

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LarryS
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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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