I am a Classics major trying to teach myself physics. I am on summer vacation at the moment, and I am going through a book called Classical Mechanics by J. Taylor. I am on the first chapter, and I need help with a question from the end of chapter 1.
Thank you, in advance. Please let me know if I should make any edits to the question.
Here is the question at hand.
I am having difficulty even showing that it is true for 2-D vectors. I would ask you to not provide an answer, but maybe some direction.
When trying to show for 2-D: $r \cdot s = (r_1^2 + r_2^2)^{1/2} \times (s_1^2 + s_2^2)^{1/2} \times \cos(\theta_{rs}) = r_1 \cdot s_1 + r_2\cdot s_2$
I tried squaring both sides. Which seems like it may be the right step forward. However, I had difficulty with trying to understand what to do with "$\cos(\theta_{rs})$." There is the suggestion to make our coordinate system such that vector-$r$ is aligned with the $x$-axis. Does that make $\cos(\theta_{rs})= {|s|\over s_1}$? It would seem like this would only be the case if $|s| > |r|$. Moreover, would this not make the component $r_2 = 0$, since the only component necessary to define vector-r in our coordinate system be $r_1$?
I feel like I may be overlooking something – maybe not so large. Some direction would be nice, but please, again, do not give me the answer!
Thank you very much for your patience and consideration.
