How to prove that something transforms like a tensor?

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To prove that a quantity transforms like a tensor, one must apply the tensor transformation property to the given relationships. In the example, the relationship B_mu(x) = T_mu_nu(x) A^nu(x) indicates that if B_mu transforms like a covariant vector, then T_mu_nu must transform according to the tensor transformation law. The discussion emphasizes the need to perform a coordinate transformation on both sides of the equation to isolate T_mu_nu and demonstrate its compliance with the transformation property. It is noted that the components of the tensor may already be defined in a specific coordinate system, which aids in the proof. Understanding these transformations is essential for confirming that T_mu_nu behaves as a tensor of type (0,2).
Chris B
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Homework Statement


I have several problems that ask me to prove that some quantity "transforms like a tensor"

For example:

"Suppose that for each choice of contravariant vector (a vector) A^nu(x), the quantities B_mu(x) are defined at teach point through a linear relationship of the form
B_mu(x) =T_mu_nu(x) A^nu(x)
transform like a covariant vector (1-form). Prove that the quantities T_mu_nu(x) transform like a tensor of type (0,2) at each point."

(Here an underscore followed by a letter is a lower index and a caret followed by a letter is an upper index).

Homework Equations



Transformation property of a tensor:
T'_mu_nu = dx^mu/dx'^mu dx^nu/dx'^nu T_mu_nu

(dx is a partial derivative and)

The Attempt at a Solution



My first guess is that I need to apply a coordinate transformation to both sides of the equation given in the problem, but I'm kind of stuck there. I don't know how to manipulate things to get T_mu_nu by itself and show it obeys the tensor transformation property.
 
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Chris B said:

Homework Statement


I have several problems that ask me to prove that some quantity "transforms like a tensor"

For example:

"Suppose that for each choice of contravariant vector (a vector) A^nu(x), the quantities B_mu(x) are defined at teach point through a linear relationship of the form
B_mu(x) =T_mu_nu(x) A^nu(x)
transform like a covariant vector (1-form). Prove that the quantities T_mu_nu(x) transform like a tensor of type (0,2) at each point."

(Here an underscore followed by a letter is a lower index and a caret followed by a letter is an upper index).

Homework Equations



Transformation property of a tensor:
T'_mu_nu = dx^mu/dx'^mu dx^nu/dx'^nu T_mu_nu

(dx is a partial derivative and)

The Attempt at a Solution



My first guess is that I need to apply a coordinate transformation to both sides of the equation given in the problem, but I'm kind of stuck there. I don't know how to manipulate things to get T_mu_nu by itself and show it obeys the tensor transformation property.
I think you are correct. To get the partial derivative of x with respect to x prime you need x as a function x prime. And that is the coordinate transformation you mentioned. Probably in you problem or examples the tensor component is already given in one coordinaye system.
 
Question: A clock's minute hand has length 4 and its hour hand has length 3. What is the distance between the tips at the moment when it is increasing most rapidly?(Putnam Exam Question) Answer: Making assumption that both the hands moves at constant angular velocities, the answer is ## \sqrt{7} .## But don't you think this assumption is somewhat doubtful and wrong?

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