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A point moves in the plane so that its t...

A point moves in the plane so that its tangential acceleration `w_tau=a`, and its normal acceleration `w_n=bt^4`, where a and b are positive constants, and t is time. At the moment `t=0` the point was at rest. Find how the curvature radius R of the point's trajectory and the total acceleration w depend on the distance covered s.

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To solve the problem step by step, we will analyze the given information about the motion of the point and derive the required expressions for the curvature radius \( R \) and the total acceleration \( w \). ### Step 1: Understand the given information We have: - Tangential acceleration \( w_{\tau} = a \) - Normal acceleration \( w_n = bt^4 \) - Initial conditions: At \( t = 0 \), the point is at rest. ### Step 2: Find the velocity as a function of time Since the tangential acceleration is constant, we can use the formula for velocity: \[ v(t) = v_0 + w_{\tau} t \] Given that \( v_0 = 0 \) (the point is at rest), we have: \[ v(t) = at \] ### Step 3: Find the distance covered as a function of time Using the equation of motion for distance: \[ s(t) = v_0 t + \frac{1}{2} w_{\tau} t^2 \] Substituting \( v_0 = 0 \): \[ s(t) = \frac{1}{2} a t^2 \] ### Step 4: Express time \( t \) in terms of distance \( s \) From the equation \( s(t) = \frac{1}{2} a t^2 \), we can solve for \( t \): \[ t^2 = \frac{2s}{a} \quad \Rightarrow \quad t = \sqrt{\frac{2s}{a}} \] ### Step 5: Find the normal acceleration in terms of distance \( s \) We know that the normal acceleration is given by: \[ w_n = \frac{v^2}{R} \] Substituting \( v(t) = at \): \[ w_n = \frac{(at)^2}{R} = \frac{a^2 t^2}{R} \] Now substituting \( t^2 = \frac{2s}{a} \): \[ w_n = \frac{a^2 \left(\frac{2s}{a}\right)}{R} = \frac{2as}{R} \] We also know from the problem statement that: \[ w_n = bt^4 \] Substituting \( t^4 = \left(\sqrt{\frac{2s}{a}}\right)^4 = \frac{4s^2}{a^2} \): \[ w_n = b \cdot \frac{4s^2}{a^2} \] ### Step 6: Equate the two expressions for normal acceleration Setting the two expressions for \( w_n \) equal to each other: \[ \frac{2as}{R} = b \cdot \frac{4s^2}{a^2} \] Rearranging gives: \[ R = \frac{2as^2}{b \cdot 4s} = \frac{as}{2b} \] ### Step 7: Find the total acceleration \( w \) The total acceleration \( w \) is given by: \[ w = \sqrt{w_{\tau}^2 + w_n^2} \] Substituting the known values: \[ w = \sqrt{a^2 + \left(bt^4\right)^2} \] Substituting \( t^4 = \frac{4s^2}{a^2} \): \[ w = \sqrt{a^2 + b^2 \left(\frac{4s^2}{a^2}\right)^2} = \sqrt{a^2 + \frac{16b^2s^4}{a^4}} \] ### Final Results 1. The curvature radius \( R \) of the point's trajectory is: \[ R = \frac{as}{2b} \] 2. The total acceleration \( w \) depends on the distance \( s \) as: \[ w = \sqrt{a^2 + \frac{16b^2s^4}{a^4}} \]
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