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Mentor's note: These posts were split off from a thread in the textbooks forum. Most of them are about calculus, even though they start off with a non-calculus question. I was too lazy to split them further into two threads
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The calculation of the magnitude of that vector is pretty straightforward if you know these definitions and the identity ##\sin^2x+\cos^2x=1##, which is just a special case of the pythagorean theorem.
\begin{align}
&\mathbf r(t)=r(\mathbf i\cos\omega t+\mathbf j\sin\omega t) =r(\cos\omega t\, (1,0)+\sin\omega t\, (0,1)) = r((\cos\omega t,0)+(0,\sin\omega t))\\
&\phantom{\mathbf r(t)}=r(\cos\omega t+0,0+\sin\omega t)=(r\cos\omega t,r\sin\omega t),\\
&|\mathbf r(t)|^2=(r\cos\omega t)^2+(r\sin\omega t)^2= r^2\cos^2\omega t+r^2\sin^2\omega t=r^2(\cos^2\omega t+\sin^2\omega t)=r^2.
\end{align} As you can see, the magnitude is r, not 1. Perhaps that's what you meant to say. Or maybe the professor was referring to the vector between the parentheses, which is just ##(\cos\omega t,\sin\omega t)##.
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I don't know what books to recommend, but I can answer the specific question. Feel free to post more of them. In this case, the vectors are ordered pairs of real numbers. In particular, we have i=(1,0) and j=(0,1). Addition of ordered pairs is defined by (a,b)+(c,d)=(a+c,b+d) and the product of a real number and an ordered pair is defined by k(a,b)=(ka,kb).christian0710 said:And example would be the motion of a particle where r(t) is a vector and i,j are unit vectors.
r(t) = r(i*coswt + j*sinwt)
The professor says "we can see from this that the length of the vector is one" But for me this does not make sense, how can we see this, and how do we apply the length formyla |r|=sqrt(a^2 + b^2) on the r(t) equation?
The calculation of the magnitude of that vector is pretty straightforward if you know these definitions and the identity ##\sin^2x+\cos^2x=1##, which is just a special case of the pythagorean theorem.
\begin{align}
&\mathbf r(t)=r(\mathbf i\cos\omega t+\mathbf j\sin\omega t) =r(\cos\omega t\, (1,0)+\sin\omega t\, (0,1)) = r((\cos\omega t,0)+(0,\sin\omega t))\\
&\phantom{\mathbf r(t)}=r(\cos\omega t+0,0+\sin\omega t)=(r\cos\omega t,r\sin\omega t),\\
&|\mathbf r(t)|^2=(r\cos\omega t)^2+(r\sin\omega t)^2= r^2\cos^2\omega t+r^2\sin^2\omega t=r^2(\cos^2\omega t+\sin^2\omega t)=r^2.
\end{align} As you can see, the magnitude is r, not 1. Perhaps that's what you meant to say. Or maybe the professor was referring to the vector between the parentheses, which is just ##(\cos\omega t,\sin\omega t)##.
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