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Acceleration of a particle moving along x-axis at time t, given by `f = f_(0) (2 - t/T)`, where `f_0` and T are constants. Initial velocity is zero. In the time interval between t = 0, and the instant when f = 0, the particle's velocity was found to be `N/M f_(0)T`. The value of `N/M` is ______

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To solve the problem, we will follow these steps: ### Step 1: Understand the given acceleration function The acceleration of the particle is given by: \[ f = f_0 \left(2 - \frac{t}{T}\right) \] where \( f_0 \) and \( T \) are constants. ### Step 2: Determine when the acceleration becomes zero To find the time when the acceleration \( f \) becomes zero, we set: \[ f = 0 \] This gives us: \[ 0 = f_0 \left(2 - \frac{t}{T}\right) \] Solving for \( t \): \[ 2 - \frac{t}{T} = 0 \] \[ \frac{t}{T} = 2 \] \[ t = 2T \] ### Step 3: Set up the equation for velocity The velocity \( v \) of the particle can be found by integrating the acceleration function. We know that: \[ a = \frac{dv}{dt} \] Thus, \[ dv = f \, dt \] Substituting the expression for \( f \): \[ dv = f_0 \left(2 - \frac{t}{T}\right) dt \] ### Step 4: Integrate to find the velocity We will integrate from \( t = 0 \) to \( t = 2T \): \[ v = \int_0^{2T} f_0 \left(2 - \frac{t}{T}\right) dt \] ### Step 5: Perform the integration Breaking the integral into two parts: \[ v = f_0 \left( \int_0^{2T} 2 \, dt - \int_0^{2T} \frac{t}{T} \, dt \right) \] Calculating the first integral: \[ \int_0^{2T} 2 \, dt = 2 \times (2T - 0) = 4T \] Calculating the second integral: \[ \int_0^{2T} \frac{t}{T} \, dt = \frac{1}{T} \cdot \left[\frac{t^2}{2}\right]_0^{2T} = \frac{1}{T} \cdot \left(\frac{(2T)^2}{2} - 0\right) = \frac{1}{T} \cdot \frac{4T^2}{2} = \frac{2T^2}{T} = 2T \] ### Step 6: Combine the results Now substituting back into the equation for \( v \): \[ v = f_0 \left(4T - 2T\right) = f_0 \cdot 2T \] ### Step 7: Relate the velocity to the given expression We are given that the velocity is also expressed as: \[ v = \frac{N}{M} f_0 T \] Setting the two expressions for \( v \) equal: \[ f_0 \cdot 2T = \frac{N}{M} f_0 T \] ### Step 8: Solve for \( \frac{N}{M} \) Dividing both sides by \( f_0 T \) (assuming \( f_0 \) and \( T \) are not zero): \[ 2 = \frac{N}{M} \] ### Final Answer Thus, the value of \( \frac{N}{M} \) is: \[ \frac{N}{M} = 2 \] ---

To solve the problem, we will follow these steps: ### Step 1: Understand the given acceleration function The acceleration of the particle is given by: \[ f = f_0 \left(2 - \frac{t}{T}\right) \] where \( f_0 \) and \( T \) are constants. ### Step 2: Determine when the acceleration becomes zero ...
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