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Question: For the unit vector \(\hat{\theta }\) , geometrically show that \(\hat{\theta }=-\sin \theta \hat{i}...

For the unit vector θ^\hat{\theta } , geometrically show that θ^=sinθi^+cosθj^\hat{\theta }=-\sin \theta \hat{i}+\cos \theta \hat{j}. Essentially, converting from Cartesian to polar, how would I determine the unit vector for θ\vec{\theta } in terms of θ\theta , i^\hat{i}, and j^\hat{j}?

Explanation

Solution

With respect to the position of a point in the Cartesian plane, two vectors are defined one is the position vector r\vec{r} and the other is θ\vec{\theta }. The position vector is defined as r=r(cosθi^+sinθj^)\vec{r}=r\left( \cos \theta \hat{i}+\sin \theta \hat{j} \right) and the vector θ\vec{\theta } is defined as θ=drdθ\vec{\theta }=\dfrac{d\vec{r}}{d\theta }. Therefore, the vector θ\vec{\theta } can be obtained by differentiating the position vector with respect to θ\theta . And for determining the unit vector for θ\vec{\theta }, we need to divide the obtained vector θ\vec{\theta } by its magnitude, which is equal to r.

Complete step by step solution:
We know that the position vector of a point in the Cartesian plane is defined as
r=r(cosθi^+sinθj^)........(i)\Rightarrow \vec{r}=r\left( \cos \theta \hat{i}+\sin \theta \hat{j} \right)........\left( i \right)
Now, we also know that the vector θ\vec{\theta } is defined for the same point as
θ=drdθ\Rightarrow \vec{\theta }=\dfrac{d\vec{r}}{d\theta }
On substituting the equation (i) in the above vector equation, we get
θ=d[r(cosθi^+sinθj^)]dθ θ=rd[(cosθi^+sinθj^)]dθ \begin{aligned} & \Rightarrow \vec{\theta }=\dfrac{d\left[ r\left( \cos \theta \hat{i}+\sin \theta \hat{j} \right) \right]}{d\theta } \\\ & \Rightarrow \vec{\theta }=r\dfrac{d\left[ \left( \cos \theta \hat{i}+\sin \theta \hat{j} \right) \right]}{d\theta } \\\ \end{aligned}
Separating the i^\hat{i} and j^\hat{j} terms, we get

& \Rightarrow \vec{\theta }=r\left\\{ \dfrac{d\left[ \left( \cos \theta \hat{i} \right) \right]}{d\theta }+\dfrac{d\left[ \left( \sin \theta \hat{j} \right) \right]}{d\theta } \right\\} \\\ & \Rightarrow \vec{\theta }=r\left( \dfrac{d\left( \cos \theta \right)}{d\theta }\hat{i}+\dfrac{d\left( \sin \theta \right)}{d\theta }\hat{j} \right) \\\ & \Rightarrow \vec{\theta }=r\left( -\sin \theta \hat{i}+\cos \theta \hat{j} \right) \\\ \end{aligned}$$ Clearly, the magnitude of the vector $\vec{\theta }$ is equal to $r$. Therefore, for getting the unit vector $\hat{\theta }$, we divide the above equation by $r$. $$\Rightarrow \hat{\theta }=-\sin \theta \hat{i}+\cos \theta \hat{j}$$ **Hence, we have determined the unit vector for $\vec{\theta }$ in terms of $\theta $, $\hat{i}$, and $\hat{j}$ as $$\hat{\theta }=-\sin \theta \hat{i}+\cos \theta \hat{j}$$** **Note:** For solving these types of questions, we must remember the important relation between the position vector $\vec{r}$ and the vector $\vec{\theta }$ which is given by $\vec{\theta }=\dfrac{d\vec{r}}{d\theta }$. Also, we must be careful regarding the signs of the derivatives of the trigonometric functions.