In this problem, we are given a particle moving in a plane with polar coordinates \((r, \theta)\). We need to establish the relationships between the unit vectors \(\hat{r}\) and \(\hat{\theta}\) when differentiated with respect to \(\theta\).
The unit vectors in polar coordinates are given by:
- \(\hat{r}\): the radial direction, pointing outwards from the origin to the point in consideration.
- \(\hat{\theta}\): the tangential direction, orthogonal to \(\hat{r}\), in the direction of increasing \(\theta\).
In polar coordinates, these unit vectors can be expressed in Cartesian coordinates as:
- \(\hat{r} = \cos(\theta) \hat{i} + \sin(\theta) \hat{j}\)
- \(\hat{\theta} = -\sin(\theta) \hat{i} + \cos(\theta) \hat{j}\)
Let's differentiate these unit vectors with respect to \(\theta\):
- Differentiating \(\hat{r}\) with respect to \(\theta\):
\(\frac{d\hat{r}}{d\theta} = \frac{d}{d\theta}[\cos(\theta) \hat{i} + \sin(\theta) \hat{j}] = -\sin(\theta) \hat{i} + \cos(\theta) \hat{j} = \hat{\theta}\) - Differentiating \(\hat{\theta}\) with respect to \(\theta\):
\(\frac{d\hat{\theta}}{d\theta} = \frac{d}{d\theta}[-\sin(\theta) \hat{i} + \cos(\theta) \hat{j}] = -\cos(\theta) \hat{i} - \sin(\theta) \hat{j} = -\hat{r}\)
Thus, the correct relationships are:
- \(\frac{d\hat{r}}{d\theta} = \hat{\theta}\)
- \(\frac{d\hat{\theta}}{d\theta} = -\hat{r}\)