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The position vector of a particle is r =...

The position vector of a particle is `r = a sin omega t hati +a cos omega t hatj`
The velocity of the particle is

A

parallel to position vector

B

perpendicular to position vector

C

directed towards origin

D

directed away from the origin

Text Solution

AI Generated Solution

The correct Answer is:
To find the velocity of the particle given its position vector \( \mathbf{r} = a \sin(\omega t) \hat{i} + a \cos(\omega t) \hat{j} \), we will follow these steps: ### Step 1: Differentiate the Position Vector The velocity vector \( \mathbf{v} \) is the time derivative of the position vector \( \mathbf{r} \). \[ \mathbf{v} = \frac{d\mathbf{r}}{dt} \] ### Step 2: Apply the Chain Rule Differentiate each component of \( \mathbf{r} \): 1. For the \( \hat{i} \) component: \[ \frac{d}{dt}(a \sin(\omega t)) = a \omega \cos(\omega t) \] 2. For the \( \hat{j} \) component: \[ \frac{d}{dt}(a \cos(\omega t)) = -a \omega \sin(\omega t) \] ### Step 3: Combine the Results Now, combine the derivatives to form the velocity vector: \[ \mathbf{v} = a \omega \cos(\omega t) \hat{i} - a \omega \sin(\omega t) \hat{j} \] ### Step 4: Analyze the Relationship Between Position and Velocity Vectors To find the relationship between the position vector \( \mathbf{r} \) and the velocity vector \( \mathbf{v} \), we can take the dot product \( \mathbf{r} \cdot \mathbf{v} \): \[ \mathbf{r} \cdot \mathbf{v} = (a \sin(\omega t) \hat{i} + a \cos(\omega t) \hat{j}) \cdot (a \omega \cos(\omega t) \hat{i} - a \omega \sin(\omega t) \hat{j}) \] ### Step 5: Calculate the Dot Product Calculating the dot product: \[ \mathbf{r} \cdot \mathbf{v} = a^2 \sin(\omega t) \cdot a \omega \cos(\omega t) - a^2 \cos(\omega t) \cdot a \omega \sin(\omega t) \] This simplifies to: \[ \mathbf{r} \cdot \mathbf{v} = a^2 \omega \sin(\omega t) \cos(\omega t) - a^2 \omega \cos(\omega t) \sin(\omega t) = 0 \] ### Step 6: Conclusion Since the dot product \( \mathbf{r} \cdot \mathbf{v} = 0 \), this implies that the position vector \( \mathbf{r} \) and the velocity vector \( \mathbf{v} \) are perpendicular to each other. Thus, the answer is that the velocity of the particle is **perpendicular to the position vector**. ### Final Answer The velocity of the particle is perpendicular to the position vector. ---

To find the velocity of the particle given its position vector \( \mathbf{r} = a \sin(\omega t) \hat{i} + a \cos(\omega t) \hat{j} \), we will follow these steps: ### Step 1: Differentiate the Position Vector The velocity vector \( \mathbf{v} \) is the time derivative of the position vector \( \mathbf{r} \). \[ \mathbf{v} = \frac{d\mathbf{r}}{dt} \] ...
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