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A particle starts from rest with a time ...

A particle starts from rest with a time varying acceleration `a=(2t-4)`. Here `t` is in second and `a` in `m//s^(2)`
The velocity time graph of the particle is

A

parabola passing through origin

B

straight line not passing through origin

C

parabola not passing through origin

D

straight line passing through origin

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The correct Answer is:
To find the velocity-time graph of a particle with a time-varying acceleration given by \( a = 2t - 4 \), we can follow these steps: ### Step 1: Understand the relationship between acceleration and velocity Acceleration \( a \) is defined as the rate of change of velocity with respect to time: \[ a = \frac{dv}{dt} \] Given that \( a = 2t - 4 \), we can write: \[ \frac{dv}{dt} = 2t - 4 \] ### Step 2: Rearrange the equation We can rearrange the equation to separate variables: \[ dv = (2t - 4) dt \] ### Step 3: Integrate both sides Next, we integrate both sides. The left side integrates to velocity \( v \), and the right side integrates with respect to time \( t \): \[ \int dv = \int (2t - 4) dt \] This gives us: \[ v = \int (2t - 4) dt \] ### Step 4: Perform the integration The integral of \( 2t \) is \( t^2 \) and the integral of \( -4 \) is \( -4t \): \[ v = t^2 - 4t + C \] where \( C \) is the constant of integration. ### Step 5: Determine the constant of integration Since the particle starts from rest, the initial velocity \( v(0) = 0 \): \[ v(0) = 0^2 - 4(0) + C = 0 \implies C = 0 \] Thus, the equation simplifies to: \[ v = t^2 - 4t \] ### Step 6: Analyze the velocity equation The equation \( v = t^2 - 4t \) is a quadratic equation in \( t \). To find the nature of the graph, we can rewrite it as: \[ v = t(t - 4) \] This indicates that the velocity is zero at \( t = 0 \) and \( t = 4 \). ### Step 7: Determine the shape of the graph Since this is a quadratic equation that opens upwards (the coefficient of \( t^2 \) is positive), the graph is a parabola. It passes through the origin (0,0) and also intersects the time axis at \( t = 4 \). ### Conclusion The velocity-time graph of the particle is a parabola that opens upwards, passing through the origin and intersecting the time axis at \( t = 4 \). ---
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