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Question: Find ⅰ) acd", when v = 30ms$^{-1}$ ⅱ) acd" at x = 15 m...

Find ⅰ) acd", when v = 30ms1^{-1}

ⅱ) acd" at x = 15 m

Answer

-1 ms2^{-2} for i) and -1 ms2^{-2} for ii)

Explanation

Solution

The graph shows the relationship between v2v^2 and xx. The graph is a straight line passing through the points (x1,v12)=(0,40)(x_1, v_1^2) = (0, 40) and (x2,v22)=(20,0)(x_2, v_2^2) = (20, 0).

The equation of the straight line is given by v2v12=v22v12x2x1(xx1)v^2 - v_1^2 = \frac{v_2^2 - v_1^2}{x_2 - x_1} (x - x_1). Substituting the given points, we get: v240=040200(x0)v^2 - 40 = \frac{0 - 40}{20 - 0} (x - 0) v240=4020xv^2 - 40 = \frac{-40}{20} x v240=2xv^2 - 40 = -2x v2=2x+40v^2 = -2x + 40

The acceleration aa is related to velocity vv and position xx by the formula a=vdvdxa = v \frac{dv}{dx}. We can find dvdx\frac{dv}{dx} by differentiating the equation v2=2x+40v^2 = -2x + 40 with respect to to xx. Differentiating both sides with respect to xx: ddx(v2)=ddx(2x+40)\frac{d}{dx}(v^2) = \frac{d}{dx}(-2x + 40) Using the chain rule on the left side, ddx(v2)=d(v2)dvdvdx=2vdvdx\frac{d}{dx}(v^2) = \frac{d(v^2)}{dv} \frac{dv}{dx} = 2v \frac{dv}{dx}. So, 2vdvdx=22v \frac{dv}{dx} = -2. Dividing by 2, we get vdvdx=1v \frac{dv}{dx} = -1. Since a=vdvdxa = v \frac{dv}{dx}, the acceleration is a=1ms2a = -1 \, \text{ms}^{-2}.

The acceleration is constant and equal to 1ms2-1 \, \text{ms}^{-2} for the motion described by the equation v2=2x+40v^2 = -2x + 40.

ⅰ) Find acceleration when v=30ms1v = 30 \, \text{ms}^{-1}. Since the acceleration is constant, its value is 1ms2-1 \, \text{ms}^{-2} at any velocity for which the relationship v2=2x+40v^2 = -2x + 40 holds. While the graph shows the velocity decreasing from 406.32ms1\sqrt{40} \approx 6.32 \, \text{ms}^{-1} to 0ms10 \, \text{ms}^{-1}, if we assume the relationship holds even for v=30ms1v=30 \, \text{ms}^{-1}, the acceleration is still the constant value we calculated. Acceleration when v=30ms1v = 30 \, \text{ms}^{-1} is 1ms2-1 \, \text{ms}^{-2}.

ⅱ) Find acceleration at x=15mx = 15 \, \text{m}. Since the acceleration is constant, its value at x=15mx = 15 \, \text{m} is 1ms2-1 \, \text{ms}^{-2}. We can also find the velocity at x=15mx = 15 \, \text{m}: v2=2(15)+40=30+40=10v^2 = -2(15) + 40 = -30 + 40 = 10. v=10ms1v = \sqrt{10} \, \text{ms}^{-1}. The acceleration at this position is 1ms2-1 \, \text{ms}^{-2}.

Explanation of the solution: The given graph is of v2v^2 versus xx. The graph is a straight line, indicating a linear relationship between v2v^2 and xx. The equation of the line is found to be v2=2x+40v^2 = -2x + 40. The acceleration aa is related to vv and xx by a=vdvdxa = v \frac{dv}{dx}. Differentiating the equation v2=2x+40v^2 = -2x + 40 with respect to xx, we get 2vdvdx=22v \frac{dv}{dx} = -2, which simplifies to vdvdx=1v \frac{dv}{dx} = -1. Thus, the acceleration a=1ms2a = -1 \, \text{ms}^{-2}. Since the acceleration is a constant value, it is the same at any given velocity or position within the motion described by the relationship.