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Derivatives of functions defined parametrically: dy/dx = (dy/dt) / (dx/dt) by the chain rule, horizontal and vertical tangents, tangents and normals to parametric curves (new in the 2024 Extension 1 syllabus)

Syllabus dot point

“Find the derivative of a function defined parametrically using the chain rule”

HSCMaths Extension 1Calculus (ME-C1, C2, C3)12 min read

Quick answer

For x=f(t)x = f(t) and y=g(t)y = g(t), the chain rule gives dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt} (where dxdt≠0\frac{dx}{dt} \neq 0). Leave it in terms of tt, substitute the parameter for a gradient, and use the same tt for the point when finding tangents and normals. Horizontal tangents: dydt=0\frac{dy}{dt} = 0; vertical tangents: dxdt=0\frac{dx}{dt} = 0. New in the 2024 Extension 1 syllabus.

Jump to a section
  1. What this dot point is asking
  2. The answer
  3. Exam-style questions
  4. Practice questions

What this dot point is asking

This is new content in the Mathematics Extension 1 11-12 Syllabus (2024), first examined in the 2027 HSC. In Year 11 (Further work with functions) you learned to write lines, parabolas and circles in parametric form, with xx and yy both given as functions of a parameter tt. The Year 12 Further calculus skills focus area now asks you to:

  • find the derivative of a function defined parametrically using the chain rule, and
  • solve problems involving derivatives of functions defined parametrically.

The 2017 course taught parametric form but had no content point on differentiating it. The skill also connects directly to projectile motion, where xx and yy are both functions of time.

Note

Think of a car on a winding road. A GPS records where it is east-west and north-south every second. You want to know how steep the road is at some point. You know how fast the car is moving north each second and how fast it is moving east each second. Divide one by the other and you get the slope of the road itself: "up this much for every one across". Time has cancelled out. That is all a parametric derivative is.

The answer

Key fact

If x=f(t)x = f(t) and y=g(t)y = g(t), the chain rule gives dydt=dydx×dxdt\frac{dy}{dt} = \frac{dy}{dx} \times \frac{dx}{dt}, so

dydx=dy/dtdx/dt,provided dxdt≠0.\frac{dy}{dx} = \frac{dy/dt}{dx/dt}, \qquad \text{provided } \frac{dx}{dt} \neq 0.

The tangent is horizontal where dydt=0\frac{dy}{dt} = 0 and dxdt≠0\frac{dx}{dt} \neq 0, and vertical where dxdt=0\frac{dx}{dt} = 0 and dydt≠0\frac{dy}{dt} \neq 0.

Why dividing the rates works

Along the curve, yy depends on xx, and both depend on tt. The chain rule links the three rates: dydt=dydx⋅dxdt\frac{dy}{dt} = \frac{dy}{dx} \cdot \frac{dx}{dt}. Rearranging gives the formula. You never need the Cartesian equation, which is the point: many parametric curves (projectile paths with the angle unknown, curves involving sin⁡t\sin t and cos⁡2t\cos 2t) are awkward or impossible to write as y=f(x)y = f(x), but their tt-derivatives are easy.

The answer is usually left in terms of tt. To get a numerical gradient at a point, substitute that point's parameter value.

A worked picture: the circle

For the circle x=3cos⁡tx = 3\cos t, y=3sin⁡ty = 3\sin t,

dydx=3cos⁡t−3sin⁡t=−cot⁡t.\frac{dy}{dx} = \frac{3\cos t}{-3\sin t} = -\cot t.

At t=π3t = \frac{\pi}{3} the point is (32,332)\left( \frac{3}{2}, \frac{3\sqrt{3}}{2} \right) and the gradient is −13-\frac{1}{\sqrt{3}}, giving the tangent x+3 y=6x + \sqrt{3}\,y = 6. The radius to that point has gradient 3\sqrt{3}, and 3×(−13)=−1\sqrt{3} \times \left( -\frac{1}{\sqrt{3}} \right) = -1: the parametric derivative agrees with the geometry fact that a tangent to a circle is perpendicular to the radius.

Tangent to a parametric circleThe circle x equals 3 cos t, y equals 3 sin t, centred at the origin with radius 3. At the parameter value t equals pi on 3 the point is (3 on 2, 3 root 3 on 2). The radius to that point makes an angle t with the positive x-axis, and the tangent line there, x plus root 3 y equals 6, is perpendicular to the radius and has gradient dy/dx equals minus cot t, which is minus 1 on root 3. xy t t = π/3: (3/2, 3√3/2) tangent x + √3y = 6 gradient −1/√3 x = 3cos t, y = 3sin t dy/dx = (dy/dt) ÷ (dx/dt) = 3cos t ÷ (−3sin t) = −cot t

Tangents and normals

The recipe is the usual one, with the parameter doing the bookkeeping:

  1. Find dydx\frac{dy}{dx} in terms of tt.
  2. Substitute the parameter value to get the gradient mm (use −1m-\frac{1}{m} for a normal).
  3. Substitute the same parameter value into xx and yy to get the point.
  4. Use y−y1=m(x−x1)y - y_1 = m(x - x_1).

For a general point (parameter pp), keep pp as a letter; this is how "show that the tangent at t=pt = p is ..." questions work.

Projectiles

A projectile launched with speed VV at angle α\alpha has x=Vtcos⁡αx = Vt\cos\alpha and y=Vtsin⁡α−12gt2y = Vt\sin\alpha - \frac{1}{2}gt^2. Then

dydx=Vsin⁡α−gtVcos⁡α,\frac{dy}{dx} = \frac{V\sin\alpha - gt}{V\cos\alpha},

which is tan⁡\tan of the angle the path makes with the horizontal at time tt. It is zero at the maximum height, positive on the way up and negative on the way down. See our page on projectile motion for the full model.

How exam questions ask about it

  • "Find dydx\frac{dy}{dx} in terms of tt." Two derivatives and a quotient; simplify.
  • "Find the gradient / tangent / normal at the point where t=…t = \dots" Substitute the parameter into both the gradient and the coordinates.
  • "Show that the tangent at t=pt = p has equation ..." Keep the working in pp and rearrange to the given form.
  • "Find where the tangent is horizontal (or vertical)." Solve dydt=0\frac{dy}{dt} = 0 (or dxdt=0\frac{dx}{dt} = 0) and check the other derivative is non-zero.
  • "Find the angle of the path / the maximum height." Use tan⁡θ=dydx\tan\theta = \frac{dy}{dx} and dydx=0\frac{dy}{dx} = 0.
Worked examples

Gradient in terms of the parameter

Find dydx\frac{dy}{dx} for x=etx = e^t, y=e2t+1y = e^{2t} + 1, and check it against the Cartesian equation.

Parametric. dxdt=et\frac{dx}{dt} = e^t and dydt=2e2t\frac{dy}{dt} = 2e^{2t}, so dydx=2e2tet=2et\frac{dy}{dx} = \frac{2e^{2t}}{e^t} = 2e^t.

Check. y=(et)2+1=x2+1y = (e^t)^2 + 1 = x^2 + 1, so dydx=2x=2et\frac{dy}{dx} = 2x = 2e^t. The two agree.

Marker's note: the check is optional in an exam, but it is a quick way to catch a slip.

Horizontal and vertical tangents

For x=t2−4x = t^2 - 4, y=t3−3ty = t^3 - 3t: dydt=3t2−3=0\frac{dy}{dt} = 3t^2 - 3 = 0 at t=±1t = \pm 1 (where dxdt=±2≠0\frac{dx}{dt} = \pm 2 \neq 0), giving horizontal tangents at (−3,−2)(-3, -2) and (−3,2)(-3, 2). dxdt=2t=0\frac{dx}{dt} = 2t = 0 at t=0t = 0 (where dydt=−3≠0\frac{dy}{dt} = -3 \neq 0), giving a vertical tangent at (−4,0)(-4, 0).

Marker's note: two different parameter values give the same xx-coordinate here; always compute both coordinates from the parameter.

Normal to a parabola at a general point

For x=2atx = 2at, y=at2y = at^2, the gradient is 2at2a=t\frac{2at}{2a} = t, so at t=pt = p the normal has gradient −1p-\frac{1}{p} and passes through (2ap,ap2)(2ap, ap^2):

y−ap2=−1p(x−2ap)⇒x+py=2ap+ap3.y - ap^2 = -\frac{1}{p}(x - 2ap) \quad\Rightarrow\quad x + py = 2ap + ap^3.

Marker's note: multiplying through by pp before rearranging keeps the algebra clean.

Common traps
Dividing the wrong way
It is dy/dtdx/dt\frac{dy/dt}{dx/dt}, not dx/dtdy/dt\frac{dx/dt}{dy/dt}.
Stopping at dydt\frac{dy}{dt}
That is how fast yy changes with the parameter, not the gradient of the curve.
Substituting the parameter into only one place
A tangent needs the point as well as the gradient, both from the same tt.
Cancelling a factor that could be zero
3t22t=3t2\frac{3t^2}{2t} = \frac{3t}{2} only for t≠0t \neq 0; at t=0t = 0 look at the curve separately.
Missing the conditions for horizontal and vertical tangents
If dxdt\frac{dx}{dt} and dydt\frac{dy}{dt} are both zero at the same tt, neither conclusion follows automatically.
Exam technique

Write dxdt\frac{dx}{dt} and dydt\frac{dy}{dt} on separate lines before dividing, so a marker can award the method even if a later step slips. Simplify dydx\frac{dy}{dx} fully (cancel common factors, use identities such as sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t), then substitute the parameter value. In "show that" questions, keep the parameter as a letter and rearrange to exactly the stated form.

Exam-style questions

Questions in the style of NESA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

HSC-style3 marks
A curve is defined by x=3t2x = 3t^2, y=2t3y = 2t^3. Find dydx\frac{dy}{dx} in terms of tt, and hence find the equation of the tangent at the point where t=1t = 1.
Show worked answer →

dxdt=6t\frac{dx}{dt} = 6t and dydt=6t2\frac{dy}{dt} = 6t^2, so dydx=6t26t=t\frac{dy}{dx} = \frac{6t^2}{6t} = t for t≠0t \neq 0.

At t=1t = 1 the point is (3,2)(3, 2) and the gradient is 11, so the tangent is y−2=x−3y - 2 = x - 3, that is y=x−1y = x - 1.

Markers expect the two tt-derivatives, the quotient, the point from the parameter value, and the tangent in any correct form.

HSC-style4 marks
A curve has parametric equations x=2cos⁡θx = 2\cos\theta, y=sin⁡θy = \sin\theta for 0≤θ<2π0 \leq \theta < 2\pi. (a) Find dydx\frac{dy}{dx} in terms of θ\theta. (b) Find the points where the tangent is horizontal. (c) Find the gradient at θ=π4\theta = \frac{\pi}{4}.
Show worked answer →

(a) dxdθ=−2sin⁡θ\frac{dx}{d\theta} = -2\sin\theta and dydθ=cos⁡θ\frac{dy}{d\theta} = \cos\theta, so dydx=−cos⁡θ2sin⁡θ=−12cot⁡θ\frac{dy}{dx} = -\frac{\cos\theta}{2\sin\theta} = -\frac{1}{2}\cot\theta.

(b) Horizontal tangents need cos⁡θ=0\cos\theta = 0 with sin⁡θ≠0\sin\theta \neq 0: θ=π2\theta = \frac{\pi}{2} and 3π2\frac{3\pi}{2}, giving the points (0,1)(0, 1) and (0,−1)(0, -1).

(c) At θ=π4\theta = \frac{\pi}{4}, dydx=−12cot⁡π4=−12\frac{dy}{dx} = -\frac{1}{2} \cot \frac{\pi}{4} = -\frac{1}{2}.

Markers award one mark for (a), two for (b) (both parameter values and both points), and one for (c).

Practice questions

Original practice questions graded from foundation to exam level, each with a full worked solution. Try them before revealing the solution.

foundation2 marks
A curve is given by x=t2x = t^2, y=t3y = t^3. Find dydx\frac{dy}{dx} in terms of tt, for t≠0t \neq 0.
Show worked solution →

Differentiate each coordinate with respect to tt. dxdt=2t\frac{dx}{dt} = 2t and dydt=3t2\frac{dy}{dt} = 3t^2.

Divide.

dydx=dy/dtdx/dt=3t22t=3t2,t≠0.\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{3t^2}{2t} = \frac{3t}{2}, \quad t \neq 0.

Marker's note: one mark for both tt-derivatives, one for 3t2\frac{3t}{2}. Cancelling tt is only valid because t≠0t \neq 0.

foundation2 marks
For x=2t+1x = 2t + 1, y=t2−4y = t^2 - 4, find the gradient of the curve at the point where t=3t = 3.
Show worked solution →

Find dydx\frac{dy}{dx}. dxdt=2\frac{dx}{dt} = 2 and dydt=2t\frac{dy}{dt} = 2t, so dydx=2t2=t\frac{dy}{dx} = \frac{2t}{2} = t.

Substitute t=3t = 3. The gradient is 33.

Marker's note: one mark for dydx=t\frac{dy}{dx} = t, one for the value. Substituting t=3t = 3 into xx or yy is not needed for a gradient.

core3 marks
A circle is given by x=3cos⁡tx = 3\cos t, y=3sin⁡ty = 3\sin t. Find the equation of the tangent at the point where t=π3t = \frac{\pi}{3}.
Show worked solution →
Gradient
dxdt=−3sin⁡t\frac{dx}{dt} = -3\sin t and dydt=3cos⁡t\frac{dy}{dt} = 3\cos t, so dydx=3cos⁡t−3sin⁡t=−cot⁡t\frac{dy}{dx} = \frac{3\cos t}{-3\sin t} = -\cot t. At t=π3t = \frac{\pi}{3}, dydx=−13\frac{dy}{dx} = -\frac{1}{\sqrt{3}}.
Point
x=3cos⁡π3=32x = 3 \cos \frac{\pi}{3} = \frac{3}{2} and y=3sin⁡π3=332y = 3 \sin \frac{\pi}{3} = \frac{3\sqrt{3}}{2}.
Tangent
y−332=−13(x−32)y - \frac{3\sqrt{3}}{2} = -\frac{1}{\sqrt{3}} \left( x - \frac{3}{2} \right). Multiplying by 3\sqrt{3}: 3 y−92=−x+32\sqrt{3}\,y - \frac{9}{2} = -x + \frac{3}{2}, so

x+3 y=6.x + \sqrt{3}\,y = 6.

Marker's note: one mark for −cot⁡t-\cot t, one for the point, one for the equation. As a check, the tangent to a circle is perpendicular to the radius: the radius has gradient 3\sqrt{3} and 3×(−13)=−1\sqrt{3} \times \left( -\frac{1}{\sqrt{3}} \right) = -1.

core3 marks
The parabola x=4tx = 4t, y=2t2y = 2t^2 has parameter tt. Show that the tangent at the point where t=pt = p has equation y=px−2p2y = px - 2p^2.
Show worked solution →
Gradient
dxdt=4\frac{dx}{dt} = 4 and dydt=4t\frac{dy}{dt} = 4t, so dydx=t\frac{dy}{dx} = t, which is pp at t=pt = p.
Point
(4p,2p2)(4p, 2p^2).
Tangent
y−2p2=p(x−4p)=px−4p2y - 2p^2 = p(x - 4p) = px - 4p^2, so y=px−2p2y = px - 2p^2.

Marker's note: one mark each for the gradient, the point and the simplified equation.

core3 marks
A curve is defined by x=t2−4x = t^2 - 4, y=t3−3ty = t^3 - 3t. Find the points on the curve where the tangent is horizontal and where it is vertical.
Show worked solution →

Derivatives. dxdt=2t\frac{dx}{dt} = 2t and dydt=3t2−3=3(t−1)(t+1)\frac{dy}{dt} = 3t^2 - 3 = 3(t - 1)(t + 1).

Horizontal tangents need dydt=0\frac{dy}{dt} = 0 with dxdt≠0\frac{dx}{dt} \neq 0: t=±1t = \pm 1. At t=1t = 1 the point is (−3,−2)(-3, -2); at t=−1t = -1 it is (−3,2)(-3, 2).

Vertical tangents need dxdt=0\frac{dx}{dt} = 0 with dydt≠0\frac{dy}{dt} \neq 0: t=0t = 0, giving (−4,0)(-4, 0).

Marker's note: one mark for the horizontal points, one for the vertical point, one for stating the conditions (in particular that the other derivative is non-zero).

exam5 marks
A projectile moves so that x=20tx = 20t and y=203 t−5t2y = 20\sqrt{3}\,t - 5t^2, where tt is in seconds and distances are in metres. (a) Show that dydx=3−t2\frac{dy}{dx} = \sqrt{3} - \frac{t}{2}. (b) Find the time at which the path is inclined at 30∘30^\circ above the horizontal. (c) Use dydx\frac{dy}{dx} to find the maximum height.
Show worked solution →

(a) dxdt=20\frac{dx}{dt} = 20 and dydt=203−10t\frac{dy}{dt} = 20\sqrt{3} - 10t, so

dydx=203−10t20=3−t2.\frac{dy}{dx} = \frac{20\sqrt{3} - 10t}{20} = \sqrt{3} - \frac{t}{2}.

(b) The gradient of the path is tan⁡30∘=13\tan 30^\circ = \frac{1}{\sqrt{3}}:

3−t2=13⇒t2=3−13=23⇒t=43=433≈2.31 s.\sqrt{3} - \frac{t}{2} = \frac{1}{\sqrt{3}} \quad\Rightarrow\quad \frac{t}{2} = \sqrt{3} - \frac{1}{\sqrt{3}} = \frac{2}{\sqrt{3}} \quad\Rightarrow\quad t = \frac{4}{\sqrt{3}} = \frac{4\sqrt{3}}{3} \approx 2.31 \text{ s}.

(c) At the maximum height the path is horizontal, so dydx=0\frac{dy}{dx} = 0: t=23t = 2\sqrt{3}. Then

y=203(23)−5(23)2=120−60=60 m.y = 20\sqrt{3}(2\sqrt{3}) - 5(2\sqrt{3})^2 = 120 - 60 = 60 \text{ m}.

Marker's note: one mark for (a); two for (b) (the tan⁡30∘\tan 30^\circ condition, then tt); two for (c) (t=23t = 2\sqrt{3}, then 6060 m).

exam4 marks
Show that the normal to the parabola x=2atx = 2at, y=at2y = at^2 at the point where t=pt = p has equation x+py=2ap+ap3x + py = 2ap + ap^3.
Show worked solution →
Tangent gradient
dxdt=2a\frac{dx}{dt} = 2a and dydt=2at\frac{dy}{dt} = 2at, so dydx=t\frac{dy}{dx} = t, which is pp at the point (2ap,ap2)(2ap, ap^2).
Normal gradient
−1p-\frac{1}{p} (for p≠0p \neq 0).
Equation
y−ap2=−1p(x−2ap)y - ap^2 = -\frac{1}{p}(x - 2ap). Multiply by pp: py−ap3=−x+2appy - ap^3 = -x + 2ap, so

x+py=2ap+ap3.x + py = 2ap + ap^3.

Marker's note: one mark for dydx=p\frac{dy}{dx} = p, one for the normal gradient, one for the point-gradient equation, one for rearranging to the required form. (At p=0p = 0 the normal is the vertical line x=0x = 0, which the formula also gives.)

exam3 marks
A curve is given by x=sin⁡tx = \sin t, y=cos⁡2ty = \cos 2t for −π2≤t≤π2-\frac{\pi}{2} \leq t \leq \frac{\pi}{2}. Find dydx\frac{dy}{dx} in terms of tt and show that dydx=−4x\frac{dy}{dx} = -4x wherever it is defined.
Show worked solution →

Differentiate. dxdt=cos⁡t\frac{dx}{dt} = \cos t and dydt=−2sin⁡2t\frac{dy}{dt} = -2\sin 2t, so

dydx=−2sin⁡2tcos⁡t=−4sin⁡tcos⁡tcos⁡t=−4sin⁡t,cos⁡t≠0.\frac{dy}{dx} = \frac{-2 \sin 2t}{\cos t} = \frac{-4 \sin t \cos t}{\cos t} = -4 \sin t, \quad \cos t \neq 0.

In terms of xx. Since x=sin⁡tx = \sin t, dydx=−4x\frac{dy}{dx} = -4x.

Check with the Cartesian equation. y=cos⁡2t=1−2sin⁡2t=1−2x2y = \cos 2t = 1 - 2\sin^2 t = 1 - 2x^2, and ddx(1−2x2)=−4x\frac{d}{dx}(1 - 2x^2) = -4x.

Marker's note: one mark for the quotient of derivatives, one for the double-angle simplification, one for −4x-4x.

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