What students learn
vector differential in both cartesian and polar coordinates, particularly the arc length factor in the \(\boldsymbol{\hat\theta}\) component
The diagonal of the rectangle on the left below shows (a blown-up picture of)
an infinitesimal displacement from the point (\(x\), \(y\)) to the nearby point
(\(x+dx\), \(y+dy\)).
- The diagonal of the “rectangle” on the right above shows (a blown-up
picture of) the same infinitesimal displacement, now expressed in
polar coordinates, from the point (\(r\), \(\phi\)) to the nearby point
(\(r+dr\), \(\phi+d\phi\)).
- Label the rectangle with the lengths of the sides.
Careful!
- Express the sides of the rectangle indicated by arrows as vectors.
Use the natural orthonormal basis defined by the picture, that is, let
\(\hat{r}\) be the unit vector which points in the direction of increasing \(\vec{r}\),
and let \(\hat{\phi}\) be the unit vector which points in the direction of increasing
\(\phi\). Do not attempt to express these vectors in terms of \(\boldsymbol{\hat{x}}\) and
\(\boldsymbol{\hat{y}}\)! You do not need to worry about the fact that some sides of the
rectangle aren't straight; the rectangle is so small that this error is
negligible.
- The diagonal of this rectangle is again the vector differential \(d\boldsymbol{\vec{r}}\).
Express \(d\boldsymbol{\vec{r}}\) in terms of \(\hat{r}\) and \(\hat{\phi}\)
- Find the length \(ds=|d\vec{r}|\) of the diagonal.
- Keywords
- Learning Outcomes
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