Parametric Equations

A2 · P3 · 14 min

A curve can be described by giving xx and yy separately as functions of a third variable, the parameter, usually tt or θ\theta. Think of tt as time and the point (x(t),y(t))\big(x(t), y(t)\big) as a particle moving across the page: each value of tt gives one position, and as tt runs through its values the particle traces the curve. In P3 you must find the gradient of such a curve using the chain rule, and use it for tangents, normals, and points where the tangent is horizontal or vertical. A parametric differentiation question appears on most papers, typically worth five to seven marks.

Parametric curves

Definition

A curve is given parametrically when its coordinates are written as x=f(t)x = f(t), y=g(t)y = g(t) for a parameter tt taking values in some interval. Each value of tt gives exactly one point.

Example: x=3cos⁡θx = 3\cos\theta, y=2sin⁡θy = 2\sin\theta for 0≤θ<2π0 \le \theta < 2\pi. At θ=0\theta = 0 the point is (3,0)(3, 0); at θ=π2\theta = \tfrac{\pi}{2}, (0,2)(0, 2); at θ=π\theta = \pi, (−3,0)(-3, 0); at θ=3π2\theta = \tfrac{3\pi}{2}, (0,−2)(0, -2). The curve is an ellipse, traced anticlockwise.

(3 cos(t), 2 sin(t))

The ellipse x=3cos⁡θx = 3\cos\theta, y=2sin⁡θy = 2\sin\theta. Its Cartesian equation is x29+y24=1\dfrac{x^2}{9} + \dfrac{y^2}{4} = 1.

Parametric form is powerful because it describes curves that are hard or impossible to write as y=f(x)y = f(x): closed loops, curves that cross themselves, curves with vertical tangents. It also keeps the algebra simple: two easy equations instead of one awkward one.

Differentiating parametric equations

The question is: as tt changes, how fast does yy change compared with xx? Over a small change δt\delta t in the parameter, xx changes by about dxdt δt\dfrac{dx}{dt}\,\delta t and yy by about dydt δt\dfrac{dy}{dt}\,\delta t. The gradient of the chord is the ratio of those changes:

δyδx≈dydt δtdxdt δt=dy/dtdx/dt\frac{\delta y}{\delta x} \approx \frac{\frac{dy}{dt}\,\delta t}{\frac{dx}{dt}\,\delta t} = \frac{dy/dt}{dx/dt}

Formally it is the chain rule, dydx=dydt×dtdx\dfrac{dy}{dx} = \dfrac{dy}{dt}\times\dfrac{dt}{dx}, together with dtdx=1/dxdt\dfrac{dt}{dx} = 1\Big/\dfrac{dx}{dt}.

Gradient of a parametric curve
dydx=dy/dtdx/dt=dydt÷dxdt,provided dxdt≠0\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{dy}{dt} \div \frac{dx}{dt}, \qquad \text{provided } \frac{dx}{dt} \ne 0

The answer is in terms of the parameter tt.

A sanity check: x=2tx = 2t, y=6ty = 6t is the straight line y=3xy = 3x. The formula gives 62=3\dfrac{6}{2} = 3. Correct.

Tangent or normal to a parametric curve
  1. Differentiate: find dxdt\dfrac{dx}{dt} and dydt\dfrac{dy}{dt}.
  2. Divide: dydx=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt}, simplified, in terms of tt.
  3. Substitute the given parameter value into dydx\dfrac{dy}{dx} to get the gradient mm (or −1m-\dfrac{1}{m} for the normal).
  4. Substitute the same parameter value into x=f(t)x = f(t) and y=g(t)y = g(t) to get the point.
  5. Write the line: y−y1=m(x−x1)y - y_1 = m(x - x_1).

If the question gives a point (x,y)(x, y) instead of a value of tt, first find the value of tt that gives that point, checking it satisfies both equations.

Horizontal and vertical tangents

From dydx=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt}:

  • Tangent parallel to the xx-axis (a stationary point): dydt=0\dfrac{dy}{dt} = 0 with dxdt≠0\dfrac{dx}{dt} \ne 0.
  • Tangent parallel to the yy-axis: dxdt=0\dfrac{dx}{dt} = 0 with dydt≠0\dfrac{dy}{dt} \ne 0.

Solve for tt, then find the coordinates. If both derivatives are zero at the same tt, the curve may have a cusp there and the formula gives no information.

Nature of a stationary point

The sign of dydx\dfrac{dy}{dx} tells you whether yy increases with xx. To test the nature of a stationary point at t=t0t = t_0, look at the sign of dydx\dfrac{dy}{dx} for tt just below and just above t0t_0, and check which way xx is moving. If xx increases with tt (that is, dxdt>0\dfrac{dx}{dt} > 0), then "before" in tt is also "to the left" in xx, and the usual sign test works. Second derivatives in parametric form are not required in P3.

Converting to a Cartesian equation

Although the syllabus focuses on differentiation, questions sometimes ask for the Cartesian equation, and it helps you recognise the curve. Eliminate the parameter:

  • Make tt the subject of one equation and substitute into the other: x=2t+1x = 2t + 1, y=t2y = t^2 gives t=x−12t = \dfrac{x - 1}{2} and y=(x−1)24y = \dfrac{(x - 1)^2}{4}.
  • For trigonometric parameters, isolate cos⁡θ\cos\theta and sin⁡θ\sin\theta and use cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1: x=3cos⁡θx = 3\cos\theta, y=2sin⁡θy = 2\sin\theta gives x29+y24=1\dfrac{x^2}{9} + \dfrac{y^2}{4} = 1.
  • Use other identities as needed: x=sec⁡θx = \sec\theta, y=tan⁡θy = \tan\theta gives x2−y2=1x^2 - y^2 = 1 from sec⁡2θ−tan⁡2θ=1\sec^2\theta - \tan^2\theta = 1; x=cos⁡2θx = \cos 2\theta, y=sin⁡θy = \sin\theta gives x=1−2y2x = 1 - 2y^2 from cos⁡2θ=1−2sin⁡2θ\cos 2\theta = 1 - 2\sin^2\theta.

Worked examples

The syllabus curve

A curve has parametric equations x=t−e2tx = t - e^{2t}, y=t+e2ty = t + e^{2t}. Find the equation of the tangent at the point where t=0t = 0.

Solution

dxdt=1−2e2t\dfrac{dx}{dt} = 1 - 2e^{2t}, dydt=1+2e2t\dfrac{dy}{dt} = 1 + 2e^{2t}, so

dydx=1+2e2t1−2e2t\frac{dy}{dx} = \frac{1 + 2e^{2t}}{1 - 2e^{2t}}

At t=0t = 0: dydx=3−1=−3\dfrac{dy}{dx} = \dfrac{3}{-1} = -3. The point is x=0−1=−1x = 0 - 1 = -1, y=0+1=1y = 0 + 1 = 1.

Tangent: y−1=−3(x+1)y - 1 = -3(x + 1), i.e. y=−3x−2y = -3x - 2.

Tangent to an ellipse

The ellipse x=3cos⁡θx = 3\cos\theta, y=2sin⁡θy = 2\sin\theta. Find the equation of the tangent at the point where θ=π4\theta = \tfrac{\pi}{4}, in the form ax+by=cax + by = c.

Solution

dxdθ=−3sin⁡θ\dfrac{dx}{d\theta} = -3\sin\theta, dydθ=2cos⁡θ\dfrac{dy}{d\theta} = 2\cos\theta, so dydx=−2cos⁡θ3sin⁡θ=−23cot⁡θ\dfrac{dy}{dx} = -\dfrac{2\cos\theta}{3\sin\theta} = -\dfrac{2}{3}\cot\theta.

At θ=π4\theta = \tfrac{\pi}{4}: gradient −23-\tfrac{2}{3}; point (32,22)=(322,2)\left(\dfrac{3}{\sqrt{2}}, \dfrac{2}{\sqrt{2}}\right) = \left(\dfrac{3\sqrt{2}}{2}, \sqrt{2}\right).

y−2=−23(x−322)⇒3y−32=−2x+32⇒2x+3y=62y - \sqrt{2} = -\frac{2}{3}\left(x - \frac{3\sqrt{2}}{2}\right) \quad\Rightarrow\quad 3y - 3\sqrt{2} = -2x + 3\sqrt{2} \quad\Rightarrow\quad 2x + 3y = 6\sqrt{2}
Horizontal and vertical tangents

A curve has parametric equations x=t2+2tx = t^2 + 2t, y=t3−12ty = t^3 - 12t. Find the coordinates of the points where the tangent is (a) parallel to the xx-axis, (b) parallel to the yy-axis.

Solution

dxdt=2t+2\dfrac{dx}{dt} = 2t + 2, dydt=3t2−12\dfrac{dy}{dt} = 3t^2 - 12.

(a) dydt=0\dfrac{dy}{dt} = 0: t2=4t^2 = 4, t=±2t = \pm 2. Neither makes dxdt\dfrac{dx}{dt} zero.

  • t=2t = 2: (4+4, 8−24)=(8,−16)(4 + 4,\ 8 - 24) = (8, -16).
  • t=−2t = -2: (4−4, −8+24)=(0,16)(4 - 4,\ -8 + 24) = (0, 16).

(b) dxdt=0\dfrac{dx}{dt} = 0: t=−1t = -1, where dydt=−9≠0\dfrac{dy}{dt} = -9 \ne 0. Point: (1−2, −1+12)=(−1,11)(1 - 2,\ -1 + 12) = (-1, 11).

A stationary point and its nature

A curve has parametric equations x=1+ln⁡tx = 1 + \ln t, y=t2−4ln⁡ty = t^2 - 4\ln t, for t>0t > 0. Find the exact coordinates of the stationary point and determine its nature.

Solution

dxdt=1t\dfrac{dx}{dt} = \dfrac{1}{t}, dydt=2t−4t\dfrac{dy}{dt} = 2t - \dfrac{4}{t}, so

dydx=(2t−4t)÷1t=2t2−4\frac{dy}{dx} = \left(2t - \frac{4}{t}\right) \div \frac{1}{t} = 2t^2 - 4

Zero when t2=2t^2 = 2, so t=2t = \sqrt{2} (as t>0t > 0). Coordinates: x=1+ln⁡2=1+12ln⁡2x = 1 + \ln\sqrt{2} = 1 + \tfrac{1}{2}\ln 2, y=2−4ln⁡2=2−2ln⁡2y = 2 - 4\ln\sqrt{2} = 2 - 2\ln 2.

Nature: dxdt=1t>0\dfrac{dx}{dt} = \tfrac{1}{t} > 0, so xx increases with tt. For tt slightly less than 2\sqrt{2}, dydx=2t2−4<0\dfrac{dy}{dx} = 2t^2 - 4 < 0; slightly more, dydx>0\dfrac{dy}{dx} > 0. The gradient goes from negative to positive as xx increases: a minimum at (1+12ln⁡2, 2−2ln⁡2)\left(1 + \tfrac{1}{2}\ln 2,\ 2 - 2\ln 2\right).

Exam-hard: where the normal meets the curve again

The curve CC has parametric equations x=t2x = t^2, y=2ty = 2t.

(a) Find the equation of the normal to CC at the point PP where t=2t = 2.

(b) The normal meets CC again at QQ. Find the coordinates of QQ.

Solution

(a) dxdt=2t\dfrac{dx}{dt} = 2t, dydt=2\dfrac{dy}{dt} = 2, so dydx=1t\dfrac{dy}{dx} = \dfrac{1}{t}. At t=2t = 2: gradient 12\tfrac{1}{2}, point P(4,4)P(4, 4). The normal has gradient −2-2:

y−4=−2(x−4)⇒y=12−2xy - 4 = -2(x - 4) \quad\Rightarrow\quad y = 12 - 2x

(b) Substitute the parametric equations into the normal:

2t=12−2t2⇒t2+t−6=0⇒(t+3)(t−2)=02t = 12 - 2t^2 \quad\Rightarrow\quad t^2 + t - 6 = 0 \quad\Rightarrow\quad (t + 3)(t - 2) = 0

t=2t = 2 is PP itself, so QQ has t=−3t = -3: Q=(9,−6)Q = (9, -6).

y^2 = 4x y = 12 - 2x

The curve x=t2x = t^2, y=2ty = 2t (the parabola y2=4xy^2 = 4x) and its normal at P(4,4)P(4, 4), which meets the curve again at Q(9,−6)Q(9, -6).

The technique in (b) is the key idea: substituting x(t)x(t) and y(t)y(t) into the equation of a line gives an equation in tt whose roots are the parameters of the intersection points. You already know one root (the point PP), which makes factorising easy.

Exam-hard: a cardioid

The curve with parametric equations x=2cos⁡θ−cos⁡2θx = 2\cos\theta - \cos 2\theta, y=2sin⁡θ−sin⁡2θy = 2\sin\theta - \sin 2\theta, for 0<θ<π0 < \theta < \pi, is part of a cardioid.

(a) Show that dydx=cos⁡θ−cos⁡2θsin⁡2θ−sin⁡θ\dfrac{dy}{dx} = \dfrac{\cos\theta - \cos 2\theta}{\sin 2\theta - \sin\theta}.

(b) Find the exact coordinates of the point where the tangent is parallel to the xx-axis.

Solution

(a) dxdθ=−2sin⁡θ+2sin⁡2θ\dfrac{dx}{d\theta} = -2\sin\theta + 2\sin 2\theta and dydθ=2cos⁡θ−2cos⁡2θ\dfrac{dy}{d\theta} = 2\cos\theta - 2\cos 2\theta. Dividing and cancelling the 22:

dydx=2(cos⁡θ−cos⁡2θ)2(sin⁡2θ−sin⁡θ)=cos⁡θ−cos⁡2θsin⁡2θ−sin⁡θ\frac{dy}{dx} = \frac{2(\cos\theta - \cos 2\theta)}{2(\sin 2\theta - \sin\theta)} = \frac{\cos\theta - \cos 2\theta}{\sin 2\theta - \sin\theta}

(b) Need cos⁡2θ=cos⁡θ\cos 2\theta = \cos\theta. Using cos⁡2θ=2cos⁡2θ−1\cos 2\theta = 2\cos^2\theta - 1:

2cos⁡2θ−cos⁡θ−1=0⇒(2cos⁡θ+1)(cos⁡θ−1)=02\cos^2\theta - \cos\theta - 1 = 0 \quad\Rightarrow\quad (2\cos\theta + 1)(\cos\theta - 1) = 0

cos⁡θ=1\cos\theta = 1 gives θ=0\theta = 0, outside the interval. So cos⁡θ=−12\cos\theta = -\tfrac{1}{2}, θ=2π3\theta = \tfrac{2\pi}{3}.

Check the denominator: sin⁡4π3−sin⁡2π3=−32−32=−3≠0\sin\tfrac{4\pi}{3} - \sin\tfrac{2\pi}{3} = -\tfrac{\sqrt{3}}{2} - \tfrac{\sqrt{3}}{2} = -\sqrt{3} \ne 0.

x=2(−12)−cos⁡4π3=−1+12=−12x = 2\left(-\tfrac{1}{2}\right) - \cos\tfrac{4\pi}{3} = -1 + \tfrac{1}{2} = -\tfrac{1}{2}, and y=2⋅32−sin⁡4π3=3+32=332y = 2\cdot\tfrac{\sqrt{3}}{2} - \sin\tfrac{4\pi}{3} = \sqrt{3} + \tfrac{\sqrt{3}}{2} = \tfrac{3\sqrt{3}}{2}.

The point is (−12,332)\left(-\tfrac{1}{2}, \tfrac{3\sqrt{3}}{2}\right).

(2 cos(t) - cos(2t), 2 sin(t) - sin(2t)) y = 3 sqrt(3) / 2

The full cardioid. The horizontal tangent y=332y = \tfrac{3\sqrt{3}}{2} touches the top of the curve at θ=2π3\theta = \tfrac{2\pi}{3}.

Common mistakes
  • Multiplying instead of dividing. dydx=dydt÷dxdt\dfrac{dy}{dx} = \dfrac{dy}{dt} \div \dfrac{dx}{dt}, not dydt×dxdt\dfrac{dy}{dt} \times \dfrac{dx}{dt}. Check with a straight line.
  • Dividing the wrong way up. dx/dtdy/dt\dfrac{dx/dt}{dy/dt} is dxdy\dfrac{dx}{dy}, the reciprocal of what you want.
  • Giving the answer as a value of tt. "Find the point" means give (x,y)(x, y).
  • Substituting tt into the wrong place. The point comes from x(t)x(t) and y(t)y(t), the gradient from dydx\dfrac{dy}{dx}. Do not put the xx-coordinate into an expression in tt.
  • Forgetting the chain rule in ddte2t=2e2t\dfrac{d}{dt}e^{2t} = 2e^{2t} or ddθsin⁡2θ=2cos⁡2θ\dfrac{d}{d\theta}\sin 2\theta = 2\cos 2\theta.
  • Missing the restriction. If t>0t > 0 or 0<θ<π0 < \theta < \pi is given, reject parameter values outside it.
Exam tip
  • Typical marks: one for each of dxdt\dfrac{dx}{dt} and dydt\dfrac{dy}{dt}, one for dividing correctly, then marks for the gradient, the point and the line.
  • "Show that dydx=…\dfrac{dy}{dx} = \ldots": simplify with identities as needed until you match the printed form exactly. In trigonometric questions, the identity step usually earns its own mark.
  • Leave equations of tangents and normals exact, in the form requested. If no form is specified, y−y1=m(x−x1)y - y_1 = m(x - x_1) with exact values is acceptable, but simplifying is safer.
  • In "meets the curve again" questions, always substitute the parametric equations into the line. Do not try to find the Cartesian equation first unless asked.
Summary
  • Parametric curve: x=f(t)x = f(t), y=g(t)y = g(t); each tt gives one point.
  • dydx=dy/dtdx/dt\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt}, in terms of tt.
  • Tangent and normal: gradient and point both come from the same value of tt.
  • Horizontal tangent: dydt=0\dfrac{dy}{dt} = 0. Vertical tangent: dxdt=0\dfrac{dx}{dt} = 0.
  • Nature of a stationary point: sign test on dydx\dfrac{dy}{dx}, checking the direction in which xx moves.
  • Cartesian equation: eliminate tt by substitution or an identity such as cos⁡2θ+sin⁡2θ=1\cos^2\theta + \sin^2\theta = 1.
  • Intersections with a line: substitute x(t)x(t), y(t)y(t) into the line and solve for tt.

Practice

Question
  1. A curve has x=3t2x = 3t^2, y=6ty = 6t. Find dydx\dfrac{dy}{dx} in terms of tt and the equation of the tangent at t=1t = 1.
  2. A curve has x=ln⁡tx = \ln t, y=t2−1y = t^2 - 1 for t>0t > 0. Find dydx\dfrac{dy}{dx} in terms of tt, and the exact coordinates of the point where the gradient is 88.
  3. A curve has x=cos⁡2θx = \cos 2\theta, y=sin⁡θy = \sin\theta. Show that dydx=−14sin⁡θ\dfrac{dy}{dx} = -\dfrac{1}{4\sin\theta}, and find the Cartesian equation of the curve.
  4. A curve has x=etx = e^t, y=te−ty = te^{-t}. Find dydx\dfrac{dy}{dx} and the exact coordinates of the stationary point.
  5. A curve has x=t+1tx = t + \dfrac{1}{t}, y=t−1ty = t - \dfrac{1}{t} for t>0t > 0. Find the point where the tangent is parallel to the yy-axis, and show that the Cartesian equation is x2−y2=4x^2 - y^2 = 4.
  6. A curve has x=2θ−sin⁡2θx = 2\theta - \sin 2\theta, y=1−cos⁡2θy = 1 - \cos 2\theta, for 0<θ<π0 < \theta < \pi. Show that dydx=cot⁡θ\dfrac{dy}{dx} = \cot\theta, and find the equation of the tangent at θ=π4\theta = \tfrac{\pi}{4}.
  7. The curve x=t3x = t^3, y=t2y = t^2. Find the equation of the normal at the point where t=1t = 1, and show that this normal does not meet the curve again.
  8. A curve has x=e2t−2tx = e^{2t} - 2t, y=4ety = 4e^t. Show that dydx=2ete2t−1\dfrac{dy}{dx} = \dfrac{2e^t}{e^{2t} - 1}, and find the exact value of tt at the point where the gradient is 11.
  9. A curve has x=2sin⁡2θx = 2\sin^2\theta, y=3tan⁡θy = 3\tan\theta, for 0<θ<π20 < \theta < \tfrac{\pi}{2}. Show that dydx=34sin⁡θcos⁡3θ\dfrac{dy}{dx} = \dfrac{3}{4\sin\theta\cos^3\theta}. Find the equation of the tangent at the point where θ=π4\theta = \tfrac{\pi}{4}, and the coordinates of the point where it meets the xx-axis.
Answers
  1. dydx=66t=1t\dfrac{dy}{dx} = \dfrac{6}{6t} = \dfrac{1}{t}. At t=1t = 1: gradient 11, point (3,6)(3, 6). Tangent: y=x+3y = x + 3.

  2. dydx=2t1/t=2t2\dfrac{dy}{dx} = \dfrac{2t}{1/t} = 2t^2. 2t2=8⇒t=22t^2 = 8 \Rightarrow t = 2 (as t>0t > 0). Point: (ln⁡2,3)(\ln 2, 3).

  3. dxdθ=−2sin⁡2θ=−4sin⁡θcos⁡θ\dfrac{dx}{d\theta} = -2\sin 2\theta = -4\sin\theta\cos\theta, dydθ=cos⁡θ\dfrac{dy}{d\theta} = \cos\theta. So dydx=cos⁡θ−4sin⁡θcos⁡θ=−14sin⁡θ\dfrac{dy}{dx} = \dfrac{\cos\theta}{-4\sin\theta\cos\theta} = -\dfrac{1}{4\sin\theta}. Cartesian: x=1−2sin⁡2θ=1−2y2x = 1 - 2\sin^2\theta = 1 - 2y^2.

  4. dxdt=et\dfrac{dx}{dt} = e^t, dydt=e−t−te−t=e−t(1−t)\dfrac{dy}{dt} = e^{-t} - te^{-t} = e^{-t}(1 - t). So dydx=(1−t)e−2t\dfrac{dy}{dx} = (1 - t)e^{-2t}. Zero at t=1t = 1: the point (e,e−1)\left(e, e^{-1}\right).

  5. dxdt=1−1t2\dfrac{dx}{dt} = 1 - \dfrac{1}{t^2}, dydt=1+1t2\dfrac{dy}{dt} = 1 + \dfrac{1}{t^2}. Vertical tangent: dxdt=0⇒t=1\dfrac{dx}{dt} = 0 \Rightarrow t = 1 (as t>0t > 0), where dydt=2≠0\dfrac{dy}{dt} = 2 \ne 0. Point: (2,0)(2, 0). Cartesian: x2−y2=(t+1t)2−(t−1t)2=4x^2 - y^2 = \left(t + \tfrac{1}{t}\right)^2 - \left(t - \tfrac{1}{t}\right)^2 = 4.

  6. dxdθ=2−2cos⁡2θ=4sin⁡2θ\dfrac{dx}{d\theta} = 2 - 2\cos 2\theta = 4\sin^2\theta, dydθ=2sin⁡2θ=4sin⁡θcos⁡θ\dfrac{dy}{d\theta} = 2\sin 2\theta = 4\sin\theta\cos\theta. So dydx=4sin⁡θcos⁡θ4sin⁡2θ=cot⁡θ\dfrac{dy}{dx} = \dfrac{4\sin\theta\cos\theta}{4\sin^2\theta} = \cot\theta. At θ=π4\theta = \tfrac{\pi}{4}: gradient 11, point (π2−1,1)\left(\tfrac{\pi}{2} - 1, 1\right). Tangent: y−1=x−π2+1y - 1 = x - \tfrac{\pi}{2} + 1, i.e. y=x+2−π2y = x + 2 - \tfrac{\pi}{2}.

  7. dydx=2t3t2=23t\dfrac{dy}{dx} = \dfrac{2t}{3t^2} = \dfrac{2}{3t}. At t=1t = 1: gradient 23\tfrac{2}{3}, point (1,1)(1, 1); normal gradient −32-\tfrac{3}{2}. Normal: y−1=−32(x−1)y - 1 = -\tfrac{3}{2}(x - 1), i.e. 3x+2y=53x + 2y = 5. Substituting: 3t3+2t2−5=03t^3 + 2t^2 - 5 = 0, which factorises as (t−1)(3t2+5t+5)=0(t - 1)(3t^2 + 5t + 5) = 0. The quadratic has discriminant 25−60<025 - 60 < 0, so t=1t = 1 is the only intersection.

  8. dxdt=2e2t−2\dfrac{dx}{dt} = 2e^{2t} - 2, dydt=4et\dfrac{dy}{dt} = 4e^t, so dydx=4et2e2t−2=2ete2t−1\dfrac{dy}{dx} = \dfrac{4e^t}{2e^{2t} - 2} = \dfrac{2e^t}{e^{2t} - 1}. Gradient 11: with u=etu = e^t, u2−2u−1=0u^2 - 2u - 1 = 0, u=1±2u = 1 \pm \sqrt{2}. Since u>0u > 0, u=1+2u = 1 + \sqrt{2} and t=ln⁡(1+2)t = \ln(1 + \sqrt{2}).

  9. dxdθ=4sin⁡θcos⁡θ\dfrac{dx}{d\theta} = 4\sin\theta\cos\theta, dydθ=3sec⁡2θ\dfrac{dy}{d\theta} = 3\sec^2\theta, so dydx=3cos⁡2θ⋅14sin⁡θcos⁡θ=34sin⁡θcos⁡3θ\dfrac{dy}{dx} = \dfrac{3}{\cos^2\theta}\cdot\dfrac{1}{4\sin\theta\cos\theta} = \dfrac{3}{4\sin\theta\cos^3\theta}. At θ=π4\theta = \tfrac{\pi}{4}: sin⁡θcos⁡3θ=12⋅122=14\sin\theta\cos^3\theta = \tfrac{1}{\sqrt{2}}\cdot\tfrac{1}{2\sqrt{2}} = \tfrac{1}{4}, so the gradient is 33. Point: x=2⋅12=1x = 2\cdot\tfrac{1}{2} = 1, y=3y = 3. Tangent: y−3=3(x−1)y - 3 = 3(x - 1), i.e. y=3xy = 3x. It meets the xx-axis at the origin (0,0)(0, 0).

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