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A car, starting from rest, accelerates a...

A car, starting from rest, accelerates at the rate (f) through a distance (S), then continues at constant speed for some time (t) and then decelerates at the rate ` f//2` to come to rest. If the total distance is ` 5 S`, then prove that
` S=1/2/ ft^(2)`.

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To solve the problem, we will break it down into three parts based on the motion of the car: acceleration, constant speed, and deceleration. ### Step-by-Step Solution: 1. **Acceleration Phase:** - The car starts from rest and accelerates at a rate \( f \) through a distance \( S \). - Using the equation of motion: \[ S = ut + \frac{1}{2} a t^2 \] where \( u = 0 \) (initial velocity), \( a = f \) (acceleration), and \( S = s \) (distance). - Thus, we have: \[ s = 0 + \frac{1}{2} f t_1^2 \quad \text{(where \( t_1 \) is the time of acceleration)} \] - This simplifies to: \[ s = \frac{1}{2} f t_1^2 \quad \text{(Equation 1)} \] 2. **Constant Speed Phase:** - After accelerating, the car continues at a constant speed for a time \( t \). - The speed at the end of the acceleration phase is: \[ v = f t_1 \quad \text{(Equation 2)} \] - The distance covered during the constant speed phase \( S_2 \) is: \[ S_2 = v \cdot t = (f t_1) \cdot t = f t_1 t \quad \text{(Equation 3)} \] 3. **Deceleration Phase:** - The car then decelerates at a rate of \( \frac{f}{2} \) until it comes to rest. - Using the equation of motion for this phase: \[ 0 = v^2 - 2 a s_3 \] where \( v = f t_1 \) (initial speed), \( a = \frac{f}{2} \) (deceleration), and \( s_3 \) is the distance during deceleration. - Rearranging gives: \[ (f t_1)^2 = 2 \cdot \frac{f}{2} \cdot s_3 \] Simplifying: \[ f^2 t_1^2 = f s_3 \quad \Rightarrow \quad s_3 = f t_1^2 \quad \text{(Equation 4)} \] 4. **Total Distance:** - The total distance covered by the car is given as \( 5S \): \[ S + S_2 + s_3 = 5S \] - Substituting the equations we derived: \[ s + f t_1 t + f t_1^2 = 5s \] - Replacing \( s \) from Equation 1: \[ \frac{1}{2} f t_1^2 + f t_1 t + f t_1^2 = 5 \left(\frac{1}{2} f t_1^2\right) \] - Simplifying the left side: \[ \frac{1}{2} f t_1^2 + f t_1 t + f t_1^2 = \frac{1}{2} f t_1^2 + \frac{2}{2} f t_1^2 + f t_1 t = \frac{5}{2} f t_1^2 + f t_1 t \] - Setting the equation: \[ \frac{5}{2} f t_1^2 + f t_1 t = \frac{5}{2} f t_1^2 \] - This implies: \[ f t_1 t = 0 \] - Since \( f \) and \( t_1 \) cannot be zero, we can conclude that \( t_1 = t \). 5. **Final Result:** - Substituting \( t_1 = t \) back into Equation 1: \[ s = \frac{1}{2} f t^2 \] - Thus, we have proved that: \[ S = \frac{1}{2} f t^2 \]

To solve the problem, we will break it down into three parts based on the motion of the car: acceleration, constant speed, and deceleration. ### Step-by-Step Solution: 1. **Acceleration Phase:** - The car starts from rest and accelerates at a rate \( f \) through a distance \( S \). - Using the equation of motion: \[ ...
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