Question
Question: For the unit vector \(\hat{\theta }\) , geometrically show that \(\hat{\theta }=-\sin \theta \hat{i}...
For the unit vector θ^ , geometrically show that θ^=−sinθi^+cosθj^. Essentially, converting from Cartesian to polar, how would I determine the unit vector for θ in terms of θ, i^, and j^?
Solution
With respect to the position of a point in the Cartesian plane, two vectors are defined one is the position vector r and the other is θ. The position vector is defined as r=r(cosθi^+sinθj^) and the vector θ is defined as θ=dθdr. Therefore, the vector θ can be obtained by differentiating the position vector with respect to θ. And for determining the unit vector for θ, we need to divide the obtained vector θ 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)
Now, we also know that the vector θ is defined for the same point as
⇒θ=dθdr
On substituting the equation (i) in the above vector equation, we get
⇒θ=dθd[r(cosθi^+sinθj^)]⇒θ=rdθd[(cosθi^+sinθj^)]
Separating the i^ and j^ terms, we get