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I'm having trouble with this question. It's from Rindler's Introduction to Special Relativity which I'm going through myself. I'm just starting to learn about tensors.
<<<<i) A vector A^i has components \dot{x}, \dot{y} in rectangular Cartesian coordinates; what are its components in polar coordinates?>>>>
This part I believe I know. The components are \dot{r}, r\dot{\theta}. The first component is the a_r component and the second is the a_{\theta} component.
<<<<ii) A vector B^i has components \ddot{x}, \ddot{y} in rectangular Cartesian coordinates; prove, directly from A.3 that its components in polar coordinates are \ddot{r}-r{(\ddot{\theta})}^2, \ddot{\theta}+2\dot{r}\dot{\theta}/r>>>>
This is what A.3 says:
<<<<An object having components A^{ij...n} in the x^i system of coordinates and A^{i'j'...n'} in the x^{i'} system is said to behave as a contravariant tensor under the transformation \{x^i\}->\{x^{i'}\} if A^{i'j'...n'}=A^{ij...n}{p_i}^{i'}{p_j}^{j'}...{p_n}^{n'}>>>>
I'm not sure how this is to be done. The a_{\theta} coordinate in part ii) seems to be divided by r. I don't know if this is a mistake in the book or there is some reason for it.
How do I use the definition of contravariant tensors to derive the formula for acceleration in polar coordinates? I really have no clue. I can derive the formula just using derivatives, but I don't see how to use tensors to derive it.
Thanks a bunch for your help!
<<<<i) A vector A^i has components \dot{x}, \dot{y} in rectangular Cartesian coordinates; what are its components in polar coordinates?>>>>
This part I believe I know. The components are \dot{r}, r\dot{\theta}. The first component is the a_r component and the second is the a_{\theta} component.
<<<<ii) A vector B^i has components \ddot{x}, \ddot{y} in rectangular Cartesian coordinates; prove, directly from A.3 that its components in polar coordinates are \ddot{r}-r{(\ddot{\theta})}^2, \ddot{\theta}+2\dot{r}\dot{\theta}/r>>>>
This is what A.3 says:
<<<<An object having components A^{ij...n} in the x^i system of coordinates and A^{i'j'...n'} in the x^{i'} system is said to behave as a contravariant tensor under the transformation \{x^i\}->\{x^{i'}\} if A^{i'j'...n'}=A^{ij...n}{p_i}^{i'}{p_j}^{j'}...{p_n}^{n'}>>>>
I'm not sure how this is to be done. The a_{\theta} coordinate in part ii) seems to be divided by r. I don't know if this is a mistake in the book or there is some reason for it.
How do I use the definition of contravariant tensors to derive the formula for acceleration in polar coordinates? I really have no clue. I can derive the formula just using derivatives, but I don't see how to use tensors to derive it.
Thanks a bunch for your help!