The curve C is defined by the parametric equations x=a(1+1t)x = a\left(1 + \dfrac{1}{t}\right) and y=a(t−1t2)y = a\left(t - \dfrac{1}{t^2}\right) where aa is a positive constant and t≠0t \ne 0.

  1. (a)

    Show that dydx=−(2+t3t).\dfrac{dy}{dx} = -\left(\dfrac{2 + t^3}{t}\right).

  2. (b)

    Find, in terms of aa, the coordinates of the turning point on C, and explain why it is a maximum.

  3. (c)

    Sketch C.

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Worked solution

4(a)

1. Differentiate $x$ with respect to $t$.

x=a(1+t−1)x = a(1 + t^{-1})
dxdt=a(−t−2)=−at2\frac{dx}{dt} = a(-t^{-2}) = -\frac{a}{t^2}

2. Differentiate $y$ with respect to $t$.

y=a(t−t−2)y = a(t - t^{-2})
dydt=a(1−(−2)t−3)=a(1+2t−3)=a(t3+2t3)\frac{dy}{dt} = a(1 - (-2)t^{-3}) = a(1 + 2t^{-3}) = a\left(\frac{t^3 + 2}{t^3}\right)

3. Use the chain rule for parametric equations to find $\frac{dy}{dx}$ and simplify to the required form.

dydx=dydtdxdt\frac{dy}{dx} = \frac{\frac{dy}{dt}}{\frac{dx}{dt}}
dydx=a(t3+2t3)−at2\frac{dy}{dx} = \frac{a\left(\frac{t^3+2}{t^3}\right)}{-\frac{a}{t^2}}
dydx=(t3+2t3)×(−t2)\frac{dy}{dx} = \left(\frac{t^3+2}{t^3}\right) \times \left(-t^2\right)
dydx=−t3+2t\frac{dy}{dx} = -\frac{t^3+2}{t}
dydx=−(2+t3t)\frac{dy}{dx} = -\left(\frac{2+t^3}{t}\right)

Answer

−(2+t3t)-\left(\frac{2 + t^3}{t}\right) (Shown)

4(b)

1. Set the first derivative to zero to find the parameter $t$ at the turning point.

For a turning point, dydx=0\frac{dy}{dx} = 0.
−(2+t3t)=0-\left(\frac{2 + t^3}{t}\right) = 0
2+t3=0  ⟹  t3=−2  ⟹  t=−2132 + t^3 = 0 \implies t^3 = -2 \implies t = -2^{\frac{1}{3}}

2. Find the $x$ and $y$ coordinates of the turning point.

Substitute t=−213t = -2^{\frac{1}{3}} into the parametric equations:
x=a(1+1−21/3)=a(1−2−13)x = a\left(1 + \frac{1}{-2^{1/3}}\right) = a\left(1 - 2^{-\frac{1}{3}}\right)
For yy, we can rewrite the equation as y=a(t3−1t2)y = a\left(\frac{t^3 - 1}{t^2}\right).
Substituting t3=−2t^3 = -2 and t2=(−21/3)2=22/3t^2 = (-2^{1/3})^2 = 2^{2/3}:
y=a(−2−122/3)=−3a22/3=−3a(2−23)y = a\left(\frac{-2 - 1}{2^{2/3}}\right) = -\frac{3a}{2^{2/3}} = -3a(2^{-\frac{2}{3}})
The coordinates are (a(1−2−13),−3a(2−23))\left(a(1 - 2^{-\frac{1}{3}}), -3a(2^{-\frac{2}{3}})\right).

3. Find the second derivative parametrically to test the nature of the turning point.

Using the chain rule for parametric equations, d2ydx2=ddt(dydx)dxdt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}.
First, differentiate xx with respect to tt:
dxdt=−at−2=−at2\frac{dx}{dt} = -at^{-2} = -\frac{a}{t^2}
Next, differentiate dydx\frac{dy}{dx} with respect to tt:
ddt(dydx)=ddt(−2t−1−t2)=2t−2−2t=2−2t3t2\frac{d}{dt}\left(\frac{dy}{dx}\right) = \frac{d}{dt}\left(-2t^{-1} - t^2\right) = 2t^{-2} - 2t = \frac{2 - 2t^3}{t^2}
Now, divide the two to find d2ydx2\frac{d^2y}{dx^2}:
d2ydx2=2−2t3t2−at2=2t3−2a\frac{d^2y}{dx^2} = \frac{\frac{2 - 2t^3}{t^2}}{-\frac{a}{t^2}} = \frac{2t^3 - 2}{a}

4. Evaluate the second derivative at the turning point to conclude it is a maximum.

Substitute t3=−2t^3 = -2 into the second derivative:
d2ydx2=2(−2)−2a=−6a\frac{d^2y}{dx^2} = \frac{2(-2) - 2}{a} = -\frac{6}{a}
Since aa is a positive constant (a>0a > 0), we have d2ydx2<0\frac{d^2y}{dx^2} < 0.
Because the second derivative is negative at the turning point, it is a maximum.

Answer

Coordinates: (a(1−2−13),−3a(2−23))\left(a(1 - 2^{-\frac{1}{3}}), -3a(2^{-\frac{2}{3}})\right); it is a maximum because d2ydx2=−6a<0\frac{d^2y}{dx^2} = -\frac{6}{a} < 0.

4(c)

1. Find the $x$ and $y$-intercepts of the curve.

To find the yy-intercept, set x=0x = 0:
a(1+1t)=0  ⟹  t=−1a\left(1 + \frac{1}{t}\right) = 0 \implies t = -1
Substitute t=−1t = -1 into yy:
y=a(−1−1(−1)2)=−2ay = a\left(-1 - \frac{1}{(-1)^2}\right) = -2a
The yy-intercept is (0,−2a)(0, -2a).

To find the xx-intercept, set y=0y = 0:
a(t−1t2)=0  ⟹  t3=1  ⟹  t=1a\left(t - \frac{1}{t^2}\right) = 0 \implies t^3 = 1 \implies t = 1
Substitute t=1t = 1 into xx:
x=a(1+11)=2ax = a\left(1 + \frac{1}{1}\right) = 2a
The xx-intercept is (2a,0)(2a, 0).

2. Determine the equations of any asymptotes.

Consider the behavior of xx and yy as t→±∞t \to \pm\infty:
As t→±∞t \to \pm\infty, 1t→0\frac{1}{t} \to 0 and 1t2→0\frac{1}{t^2} \to 0.
x=a(1+1t)→ax = a\left(1 + \frac{1}{t}\right) \to a
y=a(t−1t2)→±∞y = a\left(t - \frac{1}{t^2}\right) \to \pm\infty
Because y→±∞y \to \pm\infty as x→ax \to a, the line x=ax = a is a vertical asymptote.

3. Deduce the overall shape of the curve to complete the sketch.

From part (b), there is a maximum turning point at (a(1−2−1/3),−a(21/3+2−2/3))\left(a(1 - 2^{-1/3}), -a(2^{1/3} + 2^{-2/3})\right) when t=−21/3t = -2^{1/3}.
The domain t≠0t \neq 0 divides the curve into two continuous branches separated by the vertical asymptote x=ax = a (which corresponds to t→±∞t \to \pm\infty).

  • Left branch (t<0  ⟹  x<at < 0 \implies x < a): Comes from the third quadrant (as t→0−t \to 0^-, x→−∞x \to -\infty and y→−∞y \to -\infty), crosses the yy-axis at (0,−2a)(0, -2a), rises to the maximum turning point, and then falls towards −∞-\infty approaching the asymptote x=ax=a.
  • Right branch (t>0  ⟹  x>at > 0 \implies x > a): Falls from +∞+\infty alongside the right of x=ax=a, crosses the xx-axis at (2a,0)(2a, 0), and continues strictly decreasing towards the fourth quadrant as x→∞x \to \infty.
Answer

A valid sketch of CC must include the following features plotted on a set of axes:

  • A dashed vertical line indicating the asymptote at x=ax = a.
  • The left branch (x<ax < a): a curve starting from the bottom-left (third quadrant), crossing the yy-axis at (0,−2a)(0, -2a), rising to a local maximum point at (a(1−2−1/3),−a(21/3+2−2/3))\left(a(1 - 2^{-1/3}), -a(2^{1/3} + 2^{-2/3})\right), and then curving downwards to approach x=ax = a asymptotically from the left as y→−∞y \to -\infty.
  • The right branch (x>ax > a): a curve approaching x=ax = a asymptotically from the right as y→∞y \to \infty, passing downwards through the xx-intercept (2a,0)(2a, 0), and continuing decreasing into the fourth quadrant as x→∞x \to \infty.

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