The figure shows two rods PA and PB which are hinged at P. The rods slide such that P, A and B are on the same vertical plane. When P moves down, A and B will move in opposite directions on the horizontal ground. The horizontal distance between A and B is x metres and P is y metres from the ground.

  1. ((a))

    Express x in terms of y.

  2. ((b))

    Given that P is falling at the rate of 2 m s^-1, find the rate of change of x when P is 3 metres from the ground.

  3. ((iii))

    The rod PA makes an acute angle θ\theta with the horizontal ground.

    (iii) Using your answer to part (ii), find the rate of change of θ\theta when P is 3 metres from the ground.

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Worked solution

8((a))

1. Form an equation using Pythagoras' theorem.

Since P is vertically above the midpoint of ABAB, the horizontal distance from the midpoint of ABAB to AA is x2\frac{x}{2}.

Using Pythagoras' theorem on the right-angled triangle,
(x2)2+y2=52\left(\frac{x}{2}\right)^2+y^2=5^2
(x2)2+y2=25\left(\frac{x}{2}\right)^2+y^2=25

2. Rearrange the equation to express $x$ in terms of $y$.

(x2)2=25−y2\left(\frac{x}{2}\right)^2=25-y^2
x2=25−y2\frac{x}{2}=\sqrt{25-y^2}
Since xx is a distance, take the positive square root.
x=225−y2x=2\sqrt{25-y^2}

Answer

x=225−y2x=2\sqrt{25-y^2}

8((b))

1. Write the geometric relation between $x$ and $y$.

From the right triangle,
(x2)2+y2=25\left(\frac{x}{2}\right)^2+y^2=25
so
x24+y2=25.\frac{x^2}{4}+y^2=25.

2. Differentiate implicitly with respect to time.

Differentiate both sides with respect to tt:
12xdxdt+2ydydt=0.\frac{1}{2}x\frac{dx}{dt}+2y\frac{dy}{dt}=0.

3. Substitute $y=3$ and the falling rate of $P$ to find $\dfrac{dx}{dt}$.

Since PP is falling at 2 m s−12\text{ m s}^{-1},
dydt=−2.\frac{dy}{dt}=-2.
When y=3y=3,
(x2)2+32=25\left(\frac{x}{2}\right)^2+3^2=25
(x2)2=16\left(\frac{x}{2}\right)^2=16
x=8.x=8.
Substitute into
12xdxdt+2ydydt=0:\frac{1}{2}x\frac{dx}{dt}+2y\frac{dy}{dt}=0:
12(8)dxdt+2(3)(−2)=0\frac{1}{2}(8)\frac{dx}{dt}+2(3)(-2)=0
4dxdt−12=04\frac{dx}{dt}-12=0
dxdt=3.\frac{dx}{dt}=3.

Answer

dxdt=32 m s−1\frac{dx}{dt}=\frac{3}{2}\text{ m s}^{-1}
So xx is increasing at 1.5 m s−11.5\text{ m s}^{-1}.

8((iii))

1. Write a trigonometric relation connecting $x$ and $\theta$.

From the right triangle with hypotenuse PA=5PA=5 and adjacent side x2\dfrac{x}{2},
cos⁡θ=x/25=x10.\cos\theta=\frac{x/2}{5}=\frac{x}{10}.

2. Differentiate the relation with respect to time.

Differentiate
cos⁡θ=x10\cos\theta=\frac{x}{10}
with respect to tt:
−sin⁡θdθdt=110dxdt.-\sin\theta\frac{d\theta}{dt}=\frac{1}{10}\frac{dx}{dt}.

3. Find $\sin\theta$ when $P$ is $3$ metres from the ground.

When y=3y=3, from the earlier geometry,
(x2)2+32=25\left(\frac{x}{2}\right)^2+3^2=25
(x2)2=16\left(\frac{x}{2}\right)^2=16
so x2=4\dfrac{x}{2}=4 and x=8x=8.

Thus
cos⁡θ=810=45.\cos\theta=\frac{8}{10}=\frac45.
Since θ\theta is acute,
sin⁡θ=35.\sin\theta=\frac35.

4. Substitute $\dfrac{dx}{dt}=\dfrac32$ and solve for $\dfrac{d\theta}{dt}$.

Using the answer to part (ii),
dxdt=32.\frac{dx}{dt}=\frac32.
Substitute into
−sin⁡θdθdt=110dxdt:-\sin\theta\frac{d\theta}{dt}=\frac{1}{10}\frac{dx}{dt}:
−35dθdt=110(32)-\frac35\frac{d\theta}{dt}=\frac{1}{10}\left(\frac32\right)
−35dθdt=320-\frac35\frac{d\theta}{dt}=\frac{3}{20}
dθdt=−320×53=−14.\frac{d\theta}{dt}=-\frac{3}{20}\times\frac{5}{3}=-\frac14.

Answer

dθdt=−14 rad s−1\frac{d\theta}{dt}=-\frac14\text{ rad s}^{-1}
So θ\theta is decreasing at 0.25 rad s−10.25\text{ rad s}^{-1}.

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