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A particle moves clockwise in a circle o...

A particle moves clockwise in a circle of radius `1 m` with centre at `(x, y) = (1m, 0)`. It starts from rest at the origin at time `t = 0`. Its speed increase at the constant rate of `((pi)/(2)) m//s^(2)`. If the net acceleration at `t = 2 sec` is `(pi)/(2) sqrt((1 + Npi^(2))` then what is the value of `N` ?

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To solve the problem, we need to find the value of \( N \) given the conditions of the particle's motion. Here's a step-by-step breakdown of the solution: ### Step 1: Identify the Given Information - Radius of the circle, \( R = 1 \, \text{m} \) - Center of the circle at \( (1, 0) \) - Initial position of the particle at the origin \( (0, 0) \) - The particle starts from rest, so initial velocity \( u = 0 \) - Tangential acceleration \( a_T = \frac{\pi}{2} \, \text{m/s}^2 \) - Time \( t = 2 \, \text{s} \) ### Step 2: Calculate the Final Velocity at \( t = 2 \, \text{s} \) Using the first equation of motion: \[ v = u + a_T t \] Substituting the values: \[ v = 0 + \left(\frac{\pi}{2}\right) \cdot 2 = \pi \, \text{m/s} \] ### Step 3: Calculate the Radial Acceleration The radial acceleration \( a_R \) is given by: \[ a_R = \frac{v^2}{R} \] Substituting \( v = \pi \) and \( R = 1 \): \[ a_R = \frac{\pi^2}{1} = \pi^2 \, \text{m/s}^2 \] ### Step 4: Calculate the Net Acceleration The net acceleration \( a \) is the vector sum of tangential acceleration \( a_T \) and radial acceleration \( a_R \): \[ a = \sqrt{a_T^2 + a_R^2} \] Substituting the values: \[ a = \sqrt{\left(\frac{\pi}{2}\right)^2 + (\pi^2)^2} \] Calculating \( a_T^2 \): \[ a_T^2 = \left(\frac{\pi}{2}\right)^2 = \frac{\pi^2}{4} \] Calculating \( a_R^2 \): \[ a_R^2 = (\pi^2)^2 = \pi^4 \] Now substituting these into the equation for \( a \): \[ a = \sqrt{\frac{\pi^2}{4} + \pi^4} \] Factoring out \( \pi^2 \): \[ a = \sqrt{\pi^2 \left(\frac{1}{4} + \pi^2\right)} = \pi \sqrt{\frac{1}{4} + \pi^2} \] ### Step 5: Set the Net Acceleration Equal to the Given Expression According to the problem, the net acceleration at \( t = 2 \, \text{s} \) is given as: \[ a = \frac{\pi}{2} \sqrt{1 + N\pi^2} \] Setting the two expressions for \( a \) equal: \[ \pi \sqrt{\frac{1}{4} + \pi^2} = \frac{\pi}{2} \sqrt{1 + N\pi^2} \] ### Step 6: Simplify and Solve for \( N \) Dividing both sides by \( \pi \) (assuming \( \pi \neq 0 \)): \[ \sqrt{\frac{1}{4} + \pi^2} = \frac{1}{2} \sqrt{1 + N\pi^2} \] Squaring both sides: \[ \frac{1}{4} + \pi^2 = \frac{1}{4} (1 + N\pi^2) \] Multiplying through by 4: \[ 1 + 4\pi^2 = 1 + N\pi^2 \] Subtracting 1 from both sides: \[ 4\pi^2 = N\pi^2 \] Dividing by \( \pi^2 \) (assuming \( \pi \neq 0 \)): \[ N = 4 \] ### Final Answer The value of \( N \) is \( 4 \). ---

To solve the problem, we need to find the value of \( N \) given the conditions of the particle's motion. Here's a step-by-step breakdown of the solution: ### Step 1: Identify the Given Information - Radius of the circle, \( R = 1 \, \text{m} \) - Center of the circle at \( (1, 0) \) - Initial position of the particle at the origin \( (0, 0) \) - The particle starts from rest, so initial velocity \( u = 0 \) - Tangential acceleration \( a_T = \frac{\pi}{2} \, \text{m/s}^2 \) ...
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