(Vector Calculus) A student asked me the following: \[\frac{d}{dt}\left[\vec{R}\cdot\vec{R}\right]=\frac{d\vec{R}}{dt}\cdot\vec{R}+\vec{R}\cdot\frac{d\vec{R}}{dt}=2\vec{R}\cdot\frac{d\vec{R}}{dt}=2\vec{R}\cdot\vec{V}.\]However (from dot-product properties), \[\frac{d}{dt}\left[\vec{R}\cdot\vec{R}\right]=\frac{d}{dt}\left[\left|\vec{R}\right|^2\right]=2\left|\vec{R}\right|\cdot\frac{d\vec{R}}{dt}=2\left|\vec{R}\right|\cdot\vec{V}.\]What's the catch here?
its prolly in the 2(R.R')
or not :)
Note that in the second method it is \[2 |R| \frac{d |R|}{dt}\] Note also this isn't a dot product, just regular multiplication of real numbers or real-valued functions.
I was thinking perhaps I'm performing the chain rule incorrectly, as there's an absolute value, if I may, given these are vectors, in the expression.
On the second line you can't have a scalar (|R|) dotted with a vector (V).
I know.
Apparently, \[2\vec{R}\cdot\vec{V}=2\left | \vec{R} \right |\frac{d\left | \vec{R} \right |}{dt}?\]
Let's do an example: uniform circular motion, R = (cos t, sin t) Then 2R.R' = 2(cos t, sin t).(-sin t, cos t) = 0 and 2|R| d|R|/dt = 2 times 1 times 0 = 0, as |R| = 1 for all t So the two formulae are consistent.
Yes.
It makes sense physical this way. Write R is polar coordinates (or spherical polars if you're in R^3) Then the dot product tells you how much the velocity is in the direction of the radial displacement, as the spherical terms dot product to zero
I'm thinking R and V are orthogonal?
and then the other expression is exactly the radial displacement times the rate of change of the radial displacement. So the two interpretations are the same thing.
In the example above, of course there is no change in radial displacement, so both terms are zero.
In the second equation, once you do R dot R don't you get a scalar, and the derivative is zero.
no, because it's a function of t
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