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For a body moving with uniform accelerat...

For a body moving with uniform acceleration along straight line, the variation of its velocity (v) with position (x) is best represented by

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To solve the problem of how the velocity (v) of a body moving with uniform acceleration varies with its position (x), we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Problem**: We are dealing with a body moving with uniform acceleration along a straight line. This means that the acceleration (a) is constant. 2. **Using the Relationship Between Acceleration, Velocity, and Position**: We know that acceleration can be expressed in two ways: - \( a = \frac{dv}{dt} \) (acceleration as the rate of change of velocity with respect to time) - \( a = v \frac{dv}{dx} \) (acceleration as the product of velocity and the rate of change of velocity with respect to position) 3. **Setting Up the Equation**: Since the acceleration is constant, we can set: \[ a = v \frac{dv}{dx} = c \] where \( c \) is a constant representing the uniform acceleration. 4. **Rearranging the Equation**: Rearranging gives us: \[ v \, dv = c \, dx \] 5. **Integrating Both Sides**: We integrate both sides: \[ \int v \, dv = \int c \, dx \] This results in: \[ \frac{v^2}{2} = cx + C \] where \( C \) is the integration constant. 6. **Determining the Constant**: To find the constant \( C \), we can use initial conditions. If at \( x = 0 \), \( v = 0 \): \[ \frac{0^2}{2} = c(0) + C \implies C = 0 \] Thus, the equation simplifies to: \[ \frac{v^2}{2} = cx \] or \[ v^2 = 2cx \] 7. **Final Form of the Equation**: Rearranging gives us: \[ v^2 = 2cx \] This equation shows that the relationship between \( v^2 \) and \( x \) is linear, which is characteristic of a parabolic graph. 8. **Identifying the Graph**: The equation \( v^2 = 2cx \) resembles the standard form of a parabola \( y = kx \) where \( y \) is \( v^2 \) and \( x \) is the position \( x \). Therefore, the graph of \( v \) versus \( x \) is a parabola opening to the right. ### Conclusion: The variation of velocity (v) with position (x) for a body moving with uniform acceleration is best represented by a parabolic curve.
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