A curve C is defined by the parametric equations x=cos⁡θ−1cos⁡θ,  y=cos⁡θ+1cos⁡θ,  −π2<θ<π2.x = \cos\theta - \dfrac{1}{\cos\theta},\ \ y = \cos\theta + \dfrac{1}{\cos\theta},\ \ -\dfrac{\pi}{2} < \theta < \dfrac{\pi}{2}. The line L is the normal to C at the point with parameter pp.

  1. ((i))

    Show that dydx=cos⁡2θ−1cos⁡2θ+1\dfrac{dy}{dx} = \dfrac{\cos^{2}\theta - 1}{\cos^{2}\theta + 1}.

  2. ((ii))

    Show that the equation of L is y=1+cos⁡2p1−cos⁡2p x+2(1+cos⁡2pcos⁡p)y = \dfrac{1+\cos^{2}p}{1-\cos^{2}p}\,x + 2\left(\dfrac{1+\cos^{2}p}{\cos p}\right).

  3. ((iii))

    The line L cuts the x- and y- axes at the points P and Q respectively. Find the area of triangle OPQ in terms of pp.

  4. ((iv))

    Given that pp increases at a constant rate of 0.1 units per second, find the rate of increase of the area OPQ when p=π3p = \dfrac{\pi}{3}.

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Worked solution

5((i))

1. Differentiate $x$ with respect to $\theta$.

x=cos⁡θ−(cos⁡θ)−1x = \cos\theta - (\cos\theta)^{-1}
dxdθ=−sin⁡θ−(−1)(cos⁡θ)−2(−sin⁡θ)\frac{dx}{d\theta} = -\sin\theta - (-1)(\cos\theta)^{-2}(-\sin\theta)
dxdθ=−sin⁡θ−sin⁡θcos⁡2θ\frac{dx}{d\theta} = -\sin\theta - \frac{\sin\theta}{\cos^{2}\theta}
dxdθ=−sin⁡θ(1+1cos⁡2θ)=−sin⁡θ(cos⁡2θ+1cos⁡2θ)\frac{dx}{d\theta} = -\sin\theta \left( 1 + \frac{1}{\cos^{2}\theta} \right) = -\sin\theta \left( \frac{\cos^{2}\theta + 1}{\cos^{2}\theta} \right)

2. Differentiate $y$ with respect to $\theta$.

y=cos⁡θ+(cos⁡θ)−1y = \cos\theta + (\cos\theta)^{-1}
dydθ=−sin⁡θ+(−1)(cos⁡θ)−2(−sin⁡θ)\frac{dy}{d\theta} = -\sin\theta + (-1)(\cos\theta)^{-2}(-\sin\theta)
dydθ=−sin⁡θ+sin⁡θcos⁡2θ\frac{dy}{d\theta} = -\sin\theta + \frac{\sin\theta}{\cos^{2}\theta}
dydθ=−sin⁡θ(1−1cos⁡2θ)=−sin⁡θ(cos⁡2θ−1cos⁡2θ)\frac{dy}{d\theta} = -\sin\theta \left( 1 - \frac{1}{\cos^{2}\theta} \right) = -\sin\theta \left( \frac{\cos^{2}\theta - 1}{\cos^{2}\theta} \right)

3. Apply the chain rule for parametric equations to find $\frac{dy}{dx}$.

dydx=dydθdxdθ\frac{dy}{dx} = \frac{\frac{dy}{d\theta}}{\frac{dx}{d\theta}}
dydx=−sin⁡θ(cos⁡2θ−1cos⁡2θ)−sin⁡θ(cos⁡2θ+1cos⁡2θ)\frac{dy}{dx} = \frac{-\sin\theta \left( \frac{\cos^{2}\theta - 1}{\cos^{2}\theta} \right)}{-\sin\theta \left( \frac{\cos^{2}\theta + 1}{\cos^{2}\theta} \right)}
Cancelling the common factor −sin⁡θ-\sin\theta and the common denominator cos⁡2θ\cos^{2}\theta yields:
dydx=cos⁡2θ−1cos⁡2θ+1(Shown)\frac{dy}{dx} = \frac{\cos^{2}\theta - 1}{\cos^{2}\theta + 1} \quad \text{(Shown)}

Answer

\frac{dy}{dx} = \frac{\cos^{2}\theta - 1}{\cos^{2}\theta + 1}

5((ii))

1. Determine the gradient of the normal L at parameter $p$.

From (i), the gradient of the tangent at parameter pp is mt=cos⁡2p−1cos⁡2p+1m_t = \dfrac{\cos^2 p - 1}{\cos^2 p + 1}.
The gradient of the normal L is the negative reciprocal:
mn=−1mt=−cos⁡2p+1cos⁡2p−1=1+cos⁡2p1−cos⁡2pm_n = -\dfrac{1}{m_t} = -\dfrac{\cos^2 p + 1}{\cos^2 p - 1} = \dfrac{1 + \cos^2 p}{1 - \cos^2 p}.

2. Set up the equation of the normal L using the coordinates of the point at parameter $p$.

At parameter pp, the coordinates are:
x=cos⁡p−1cos⁡p=cos⁡2p−1cos⁡px = \cos p - \dfrac{1}{\cos p} = \dfrac{\cos^2 p - 1}{\cos p}
y=cos⁡p+1cos⁡p=cos⁡2p+1cos⁡py = \cos p + \dfrac{1}{\cos p} = \dfrac{\cos^2 p + 1}{\cos p}

Using the point-gradient form y−y1=mn(x−x1)y - y_1 = m_n(x - x_1), the equation of the normal is:
y−(cos⁡2p+1cos⁡p)=1+cos⁡2p1−cos⁡2p[x−(cos⁡2p−1cos⁡p)]y - \left(\dfrac{\cos^2 p + 1}{\cos p}\right) = \dfrac{1 + \cos^2 p}{1 - \cos^2 p} \left[ x - \left(\dfrac{\cos^2 p - 1}{\cos p}\right) \right]

3. Simplify the equation to match the required form.

Expanding the right-hand side and moving the yy-coordinate term over:
y=1+cos⁡2p1−cos⁡2px−(1+cos⁡2p1−cos⁡2p)(cos⁡2p−1cos⁡p)+cos⁡2p+1cos⁡py = \dfrac{1 + \cos^2 p}{1 - \cos^2 p}x - \left(\dfrac{1 + \cos^2 p}{1 - \cos^2 p}\right) \left(\dfrac{\cos^2 p - 1}{\cos p}\right) + \dfrac{\cos^2 p + 1}{\cos p}

Notice that cos⁡2p−11−cos⁡2p=−1\dfrac{\cos^2 p - 1}{1 - \cos^2 p} = -1, so the equation simplifies to:
y=1+cos⁡2p1−cos⁡2px−(1+cos⁡2p)(−1cos⁡p)+1+cos⁡2pcos⁡py = \dfrac{1 + \cos^2 p}{1 - \cos^2 p}x - (1 + \cos^2 p)\left(-\dfrac{1}{\cos p}\right) + \dfrac{1 + \cos^2 p}{\cos p}
y=1+cos⁡2p1−cos⁡2px+1+cos⁡2pcos⁡p+1+cos⁡2pcos⁡py = \dfrac{1 + \cos^2 p}{1 - \cos^2 p}x + \dfrac{1 + \cos^2 p}{\cos p} + \dfrac{1 + \cos^2 p}{\cos p}
y=1+cos⁡2p1−cos⁡2px+2(1+cos⁡2pcos⁡p)(shown)y = \dfrac{1 + \cos^2 p}{1 - \cos^2 p}x + 2\left(\dfrac{1 + \cos^2 p}{\cos p}\right) \quad \text{(shown)}

Answer

y = \dfrac{1+\cos^{2}p}{1-\cos^{2}p},x + 2\left(\dfrac{1+\cos^{2}p}{\cos p}\right) \quad \text{(shown)}

5((iii))

1. Find the $y$-intercept $Q$ by setting $x = 0$ in the equation of line $L$.

y=1+cos⁡2p1−cos⁡2p(0)+2(1+cos⁡2pcos⁡p)y = \frac{1+\cos^{2}p}{1-\cos^{2}p}(0) + 2\left(\frac{1+\cos^{2}p}{\cos p}\right)
yQ=2(1+cos⁡2p)cos⁡py_Q = \frac{2(1+\cos^{2}p)}{\cos p}
Thus, the yy-intercept QQ is at (0,2(1+cos⁡2p)cos⁡p)\left(0, \frac{2(1+\cos^{2}p)}{\cos p}\right).

2. Find the $x$-intercept $P$ by setting $y = 0$ in the equation of line $L$.

0=1+cos⁡2p1−cos⁡2p x+2(1+cos⁡2pcos⁡p)0 = \frac{1+\cos^{2}p}{1-\cos^{2}p}\,x + 2\left(\frac{1+\cos^{2}p}{\cos p}\right)
1+cos⁡2p1−cos⁡2p x=−2(1+cos⁡2p)cos⁡p\frac{1+\cos^{2}p}{1-\cos^{2}p}\,x = - \frac{2(1+\cos^{2}p)}{\cos p}
Dividing both sides by 1+cos⁡2p1+\cos^{2}p (which is strictly positive and therefore non-zero):
x1−cos⁡2p=−2cos⁡p\frac{x}{1-\cos^{2}p} = - \frac{2}{\cos p}
xP=−2(1−cos⁡2p)cos⁡px_P = - \frac{2(1-\cos^{2}p)}{\cos p}
Thus, the xx-intercept PP is at (−2(1−cos⁡2p)cos⁡p,0)\left(- \frac{2(1-\cos^{2}p)}{\cos p}, 0\right).

3. Calculate the area of the triangle $OPQ$.

The area of right-angled triangle OPQOPQ is given by 12∣xP∣∣yQ∣\frac{1}{2} |x_P| |y_Q|.
Since −π2<p<π2-\frac{\pi}{2} < p < \frac{\pi}{2}, we have cos⁡p>0\cos p > 0.
Thus 1−cos⁡2p≥01-\cos^2 p \ge 0, meaning xP≤0x_P \le 0 and yQ≥0y_Q \ge 0.
Area=12∣−2(1−cos⁡2p)cos⁡p∣∣2(1+cos⁡2p)cos⁡p∣\text{Area} = \frac{1}{2} \left| - \frac{2(1-\cos^{2}p)}{\cos p} \right| \left| \frac{2(1+\cos^{2}p)}{\cos p} \right|
Area=12(2(1−cos⁡2p)cos⁡p)(2(1+cos⁡2p)cos⁡p)\text{Area} = \frac{1}{2} \left( \frac{2(1-\cos^{2}p)}{\cos p} \right) \left( \frac{2(1+\cos^{2}p)}{\cos p} \right)
Area=2(1−cos⁡2p)(1+cos⁡2p)cos⁡2p\text{Area} = \frac{2(1-\cos^{2}p)(1+\cos^{2}p)}{\cos^{2}p}
Area=2(1−cos⁡4p)cos⁡2p\text{Area} = \frac{2(1-\cos^{4}p)}{\cos^{2}p}
(Note: This can equivalently be written as 2sec⁡2p−2cos⁡2p2\sec^2 p - 2\cos^2 p or 2tan⁡2p(1+cos⁡2p)2\tan^2 p (1+\cos^2 p))

Answer

2(1−cos⁡4p)cos⁡2p\dfrac{2(1-\cos^{4}p)}{\cos^{2}p}

5((iv))

1. Establish the expression for the area of triangle OPQ by determining the intercepts of the normal line $L$ (from part ii).

From part (ii), the normal line LL is given by y=1+cos⁡2p1−cos⁡2px+2(1+cos⁡2pcos⁡p)y = \frac{1+\cos^{2}p}{1-\cos^{2}p}x + 2\left(\frac{1+\cos^{2}p}{\cos p}\right).
To find the area required from part (iii), we determine the xx and yy intercepts of LL.
Setting y=0y = 0, the xx-intercept is:
xP=−2(1+cos⁡2pcos⁡p)÷(1+cos⁡2p1−cos⁡2p)=−2(1−cos⁡2p)cos⁡p=−2sin⁡2pcos⁡px_P = -2\left(\frac{1+\cos^{2}p}{\cos p}\right) \div \left(\frac{1+\cos^{2}p}{1-\cos^{2}p}\right) = -\frac{2(1-\cos^2 p)}{\cos p} = -\frac{2\sin^2 p}{\cos p}
Setting x=0x = 0, the yy-intercept is:
yQ=2(1+cos⁡2p)cos⁡py_Q = \frac{2(1+\cos^{2}p)}{\cos p}
Since −π2<p<π2-\frac{\pi}{2} < p < \frac{\pi}{2}, cos⁡p>0\cos p > 0. The area AA of triangle OPQ is:
A=12∣xPyQ∣=12(2sin⁡2pcos⁡p)(2(1+cos⁡2p)cos⁡p)A = \frac{1}{2} |x_P y_Q| = \frac{1}{2} \left( \frac{2\sin^2 p}{\cos p} \right) \left( \frac{2(1+\cos^2 p)}{\cos p} \right)
A=2sin⁡2p(1+cos⁡2p)cos⁡2p=2tan⁡2p(1+cos⁡2p)A = \frac{2\sin^2 p(1+\cos^2 p)}{\cos^2 p} = 2\tan^2 p(1+\cos^2 p)
Expanding this gives a simpler form for differentiation:
A=2tan⁡2p+2sin⁡2pA = 2\tan^2 p + 2\sin^2 p

2. Differentiate the area $A$ with respect to the parameter $p$.

Differentiate the area AA with respect to pp:
dAdp=ddp(2tan⁡2p+2sin⁡2p)\frac{\mathrm{d}A}{\mathrm{d}p} = \frac{\mathrm{d}}{\mathrm{d}p}(2\tan^2 p + 2\sin^2 p)
Using the chain rule for each trigonometric term:
dAdp=2(2tan⁡psec⁡2p)+2(2sin⁡pcos⁡p)\frac{\mathrm{d}A}{\mathrm{d}p} = 2(2\tan p \sec^2 p) + 2(2\sin p \cos p)
dAdp=4tan⁡psec⁡2p+4sin⁡pcos⁡p\frac{\mathrm{d}A}{\mathrm{d}p} = 4\tan p \sec^2 p + 4\sin p \cos p

3. Evaluate the derivative $\frac{\mathrm{d}A}{\mathrm{d}p}$ at the specific value $p = \frac{\pi}{3}$.

Substitute p=π3p = \frac{\pi}{3} into the derivative. Note the exact values:
tan⁡(π3)=3,sec⁡(π3)=2,sin⁡(π3)=32,cos⁡(π3)=12\tan\left(\frac{\pi}{3}\right) = \sqrt{3}, \quad \sec\left(\frac{\pi}{3}\right) = 2, \quad \sin\left(\frac{\pi}{3}\right) = \frac{\sqrt{3}}{2}, \quad \cos\left(\frac{\pi}{3}\right) = \frac{1}{2}
Substituting these into our expression:
dAdp∣p=π3=4(3)(2)2+4(32)(12)\frac{\mathrm{d}A}{\mathrm{d}p} \bigg|_{p=\frac{\pi}{3}} = 4(\sqrt{3})(2)^2 + 4\left(\frac{\sqrt{3}}{2}\right)\left(\frac{1}{2}\right)
dAdp∣p=π3=163+3=173\frac{\mathrm{d}A}{\mathrm{d}p} \bigg|_{p=\frac{\pi}{3}} = 16\sqrt{3} + \sqrt{3} = 17\sqrt{3}

4. Apply the chain rule for connected rates of change to find the rate of increase of the area.

Using the connected rates of change formula:
dAdt=dAdp×dpdt\frac{\mathrm{d}A}{\mathrm{d}t} = \frac{\mathrm{d}A}{\mathrm{d}p} \times \frac{\mathrm{d}p}{\mathrm{d}t}
Given that pp increases at a constant rate of 0.10.1 units per second (dpdt=0.1\frac{\mathrm{d}p}{\mathrm{d}t} = 0.1):
dAdt=173×0.1=1.73\frac{\mathrm{d}A}{\mathrm{d}t} = 17\sqrt{3} \times 0.1 = 1.7\sqrt{3}

Answer

1.731.7\sqrt{3} (or approximately 2.942.94) units2/s\text{units}^2\text{/s}

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