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🎯⭐ INTERACTIVE LESSON

Parametric Curves & Calculus

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Parametric Curves & Calculus - Complete Interactive Lesson

Part 1: Parametric Equations

Parametric Curves & Calculus

Part 1 of 7 — Parametric Equations & Graphing

Parametric equations describe a curve using a parameter tt, giving both xx and yy as functions of tt. This is essential for modeling motion and curves that fail the vertical line test.

Parametric Equations

x=f(t),y=g(t),a≤t≤b\boxed{x = f(t), \quad y = g(t), \quad a \le t \le b}

The parameter tt typically represents time. As tt increases, the point (x(t),y(t))(x(t), y(t)) traces a curve with a specific direction (orientation).

Common Parametric Curves

Curvex(t)x(t)y(t)y(t)Shape
Circleacos⁡ta\cos tasin⁡ta\sin tCircle radius aa, CCW
Ellipseacos⁡ta\cos tbsin⁡tb\sin tEllipse
Linex0+atx_0 + aty0+bty_0 + btLine through (x0,y0)(x_0,y_0)
Parabolattt2t^2Standard parabola
Cycloidt−sin⁡tt - \sin t1−cos⁡t1 - \cos tArch shape

Key Fact: A single Cartesian curve can have many different parametric representations. What differs is the speed and direction of traversal.

Eliminating the Parameter

To convert from parametric to Cartesian, eliminate tt:

Example: x=2cos⁡tx = 2\cos t, y=2sin⁡ty = 2\sin t

  • cos⁡t=x/2\cos t = x/2, sin⁡t=y/2\sin t = y/2
  • cos⁡2t+sin⁡2t=1  ⟹  x24+y24=1  ⟹  x2+y2=4\cos^2 t + \sin^2 t = 1 \implies \frac{x^2}{4} + \frac{y^2}{4} = 1 \implies x^2 + y^2 = 4

Example: x=t+1x = t + 1, y=t2−3y = t^2 - 3

  • t=x−1t = x - 1, so y=(x−1)2−3y = (x-1)^2 - 3

Example: x=etx = e^t, y=e2t+1y = e^{2t} + 1

  • x=et  ⟹  e2t=x2x = e^t \implies e^{2t} = x^2, so y=x2+1y = x^2 + 1 (with x>0x > 0)

AP Tip: When eliminating the parameter, state any restrictions on xx or yy from the domain of tt.

Parametric Basics

Direction & Speed

The direction (orientation) is determined by increasing tt.

Speed along the curve at time tt: speed=(dxdt)2+(dydt)2\boxed{\text{speed} = \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}}

For x=3cos⁡tx = 3\cos t, y=3sin⁡ty = 3\sin t: speed=(−3sin⁡t)2+(3cos⁡t)2=9=3\text{speed} = \sqrt{(-3\sin t)^2 + (3\cos t)^2} = \sqrt{9} = 3

The particle moves at constant speed 33 along the circle. This is uniform circular motion.

Curve Identification

Speed Calculation

Key Takeaways — Part 1

  • Parametric equations: x=f(t)x = f(t), y=g(t)y = g(t)
  • Eliminate parameter using algebra or trig identities
  • Direction determined by increasing tt
  • Speed =(x′)2+(y′)2= \sqrt{(x')^2 + (y')^2}
  • Note any domain restrictions when converting to Cartesian

Coming Up: Part 2 covers derivatives of parametric curves — dy/dxdy/dx and d2y/dx2d^2y/dx^2.

Part 2: Second Derivative

Parametric Curves & Calculus

Part 2 of 7 — Derivatives of Parametric Curves

The chain rule gives us a formula for dy/dxdy/dx in terms of the parameter tt. This is one of the most-tested BC topics.

First Derivative

dydx=dy/dtdx/dtprovided dxdt≠0\boxed{\frac{dy}{dx} = \frac{dy/dt}{dx/dt} \quad \text{provided } \frac{dx}{dt} \ne 0}

This gives the slope of the tangent line to the parametric curve at the point corresponding to parameter tt.

Example: x=t2−1x = t^2 - 1, y=t3−3ty = t^3 - 3t

dxdt=2t,dydt=3t2−3\frac{dx}{dt} = 2t, \quad \frac{dy}{dt} = 3t^2 - 3

dydx=3t2−32t=3(t2−1)2t\frac{dy}{dx} = \frac{3t^2 - 3}{2t} = \frac{3(t^2-1)}{2t}

At t=2t = 2: dydx=3(4−1)4=94\frac{dy}{dx} = \frac{3(4-1)}{4} = \frac{9}{4} at the point (3,2)(3, 2).

Key Fact: Horizontal tangent when dy/dt=0dy/dt = 0 (and dx/dt≠0dx/dt \ne 0). Vertical tangent when dx/dt=0dx/dt = 0 (and dy/dt≠0dy/dt \ne 0).

Second Derivative

d2ydx2=ddt(dydx)dxdt\boxed{\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}}

Critical: This is NOT d2y/dt2d2x/dt2\frac{d^2y/dt^2}{d^2x/dt^2}! You must differentiate dy/dxdy/dx with respect to tt, then divide by dx/dtdx/dt.

Example (continued): dydx=3t2−32t=32t−32t\frac{dy}{dx} = \frac{3t^2-3}{2t} = \frac{3}{2}t - \frac{3}{2t}

ddt(dydx)=32+32t2\frac{d}{dt}\left(\frac{dy}{dx}\right) = \frac{3}{2} + \frac{3}{2t^2}

d2ydx2=32+32t22t=3t2+34t3\frac{d^2y}{dx^2} = \frac{\frac{3}{2} + \frac{3}{2t^2}}{2t} = \frac{3t^2 + 3}{4t^3}

At t=2t = 2: d2ydx2=1532\frac{d^2y}{dx^2} = \frac{15}{32} (concave up since positive).

Derivative Practice

Tangent Lines

The tangent line at t=t0t = t_0: y−y(t0)=dydx∣t=t0⋅(x−x(t0))y - y(t_0) = \frac{dy}{dx}\bigg|_{t=t_0} \cdot (x - x(t_0))

Example: x=t+sin⁡tx = t + \sin t, y=t−cos⁡ty = t - \cos t at t=0t = 0

Point: (0+0,0−1)=(0,−1)(0 + 0, 0 - 1) = (0, -1)

Slope: dydx=1+sin⁡t1+cos⁡t∣t=0=12\frac{dy}{dx} = \frac{1 + \sin t}{1 + \cos t}\bigg|_{t=0} = \frac{1}{2}

y+1=12(x−0)  ⟹  y=x2−1\boxed{y + 1 = \frac{1}{2}(x - 0) \implies y = \frac{x}{2} - 1}

AP Tip: Tangent line problems at specific parameter values are guaranteed on the BC exam. Always find the point AND the slope.

Classify the Tangent

Slope Computation

Key Takeaways — Part 2

FormulaExpression
First derivativedydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}
Second derivatived2ydx2=(d/dt)(dy/dx)dx/dt\frac{d^2y}{dx^2} = \frac{(d/dt)(dy/dx)}{dx/dt}
Horizontal tangentdy/dt=0dy/dt = 0, dx/dt≠0dx/dt \ne 0
Vertical tangentdx/dt=0dx/dt = 0, dy/dt≠0dy/dt \ne 0

Coming Up: Part 3 covers arc length of parametric curves.

Part 3: Arc Length (Parametric)

Parametric Curves & Calculus

Part 3 of 7 — Arc Length of Parametric Curves

The arc length formula for parametric curves is a direct extension of the Pythagorean theorem applied to infinitesimal segments.

Arc Length Formula

L=∫ab(dxdt)2+(dydt)2 dt\boxed{L = \int_a^b \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt}

Derivation: A tiny piece of the curve has horizontal change dxdx and vertical change dydy. By the Pythagorean theorem: ds=dx2+dy2=(dxdt)2+(dydt)2 dtds = \sqrt{dx^2 + dy^2} = \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt

Note: (dx/dt)2+(dy/dt)2\sqrt{(dx/dt)^2 + (dy/dt)^2} is the speed of the particle. So:

Arc length=∫abspeed dt\boxed{\text{Arc length} = \int_a^b \text{speed}\,dt}

Key Fact: Arc length equals the integral of speed — this makes physical sense! Distance = speed × time.

Example: Circle x=3cos⁡tx = 3\cos t, y=3sin⁡ty = 3\sin t, 0≤t≤2π0 \le t \le 2\pi

QuantityValue
dx/dtdx/dt−3sin⁡t-3\sin t
dy/dtdy/dt3cos⁡t3\cos t
Speed9sin⁡2t+9cos⁡2t=3\sqrt{9\sin^2 t + 9\cos^2 t} = 3
Arc length∫02π3 dt=6π\int_0^{2\pi} 3\,dt = 6\pi

This confirms: circumference of circle with radius 33 is 2π(3)=6π2\pi(3) = 6\pi. \checkmark

Example: x=t2x = t^2, y=t3y = t^3, 0≤t≤10 \le t \le 1

L=∫01(2t)2+(3t2)2 dt=∫014t2+9t4 dt=∫01t4+9t2 dtL = \int_0^1 \sqrt{(2t)^2 + (3t^2)^2}\,dt = \int_0^1 \sqrt{4t^2 + 9t^4}\,dt = \int_0^1 t\sqrt{4+9t^2}\,dt

Let u=4+9t2u = 4 + 9t^2: L=118⋅23[u3/2]413=127(1313−8)L = \frac{1}{18}\cdot\frac{2}{3}[u^{3/2}]_4^{13} = \frac{1}{27}(13\sqrt{13} - 8)

Arc Length Practice

Arc Length vs. Displacement

ConceptFormulaMeaning
Arc length∫ab(x′)2+(y′)2 dt\int_a^b \sqrt{(x')^2 + (y')^2}\,dtTotal distance traveled
Displacement(Δx)2+(Δy)2\sqrt{(\Delta x)^2 + (\Delta y)^2}Straight-line distance

Arc length ≥\ge displacement, with equality only for straight-line motion.

AP Tip: The AP exam often asks for distance traveled (arc length), not displacement. Read carefully!

Setup Practice

Computation

Key Takeaways — Part 3

L=∫ab(x′)2+(y′)2 dt=∫abspeed dtL = \int_a^b \sqrt{(x')^2 + (y')^2}\,dt = \int_a^b \text{speed}\,dt

  • Arc length = integral of speed
  • Always ≥\ge displacement
  • For circles: confirms C=2πrC = 2\pi r

Coming Up: Part 4 covers area enclosed by parametric curves.

Part 4: Area Under Parametric Curves

Parametric Curves & Calculus

Part 4 of 7 — Area Under Parametric Curves

The area formula for parametric curves converts the standard ∫y dx\int y\,dx into an integral over the parameter tt.

Area Formula

For a curve traced left to right (xx increasing with tt):

A=∫aby(t)⋅x′(t) dt\boxed{A = \int_a^b y(t) \cdot x'(t)\,dt}

This comes from substituting dx=x′(t) dtdx = x'(t)\,dt into A=∫y dxA = \int y\,dx.

For a curve traced right to left (xx decreasing): A=−∫aby(t)⋅x′(t) dtA = -\int_a^b y(t) \cdot x'(t)\,dt

Example: Area under one arch of the cycloid x=t−sin⁡tx = t - \sin t, y=1−cos⁡ty = 1 - \cos t

One arch: 0≤t≤2π0 \le t \le 2\pi. Since x′=1−cos⁡t≥0x' = 1 - \cos t \ge 0, the curve moves left to right:

A=∫02π(1−cos⁡t)(1−cos⁡t) dt=∫02π(1−cos⁡t)2 dtA = \int_0^{2\pi} (1-\cos t)(1-\cos t)\,dt = \int_0^{2\pi} (1-\cos t)^2\,dt

=∫02π(1−2cos⁡t+cos⁡2t) dt=2π−0+π=3π= \int_0^{2\pi} (1 - 2\cos t + \cos^2 t)\,dt = 2\pi - 0 + \pi = 3\pi

Area under one cycloid arch=3π\boxed{\text{Area under one cycloid arch} = 3\pi}

Area Enclosed by a Closed Curve

For a closed parametric curve traversed counterclockwise:

A=−∮y(t) x′(t) dt=∮x(t) y′(t) dtA = -\oint y(t)\,x'(t)\,dt = \oint x(t)\,y'(t)\,dt

Example: Ellipse x=acos⁡tx = a\cos t, y=bsin⁡ty = b\sin t, 0≤t≤2π0 \le t \le 2\pi

A=∫02πbsin⁡t⋅(−asin⁡t) dt=−ab∫02πsin⁡2t dt=−ab⋅πA = \int_0^{2\pi} b\sin t \cdot (-a\sin t)\,dt = -ab\int_0^{2\pi} \sin^2 t\,dt = -ab \cdot \pi

Since the curve goes counterclockwise and we get a negative result from y⋅x′y \cdot x', take the absolute value:

A=πab\boxed{A = \pi ab}

This confirms the well-known ellipse area formula.

AP Tip: Watch the sign! If the formula gives a negative area, the curve is traced in the opposite direction to what you assumed. Take ∣A∣|A|.

Area Practice

Setup the Integral

Area Computation

Key Takeaways — Part 4

FormulaUse
A=∫aby(t)x′(t) dtA = \int_a^b y(t)x'(t)\,dtArea under curve (left to right)
A=πabA = \pi abEllipse x=acos⁡tx = a\cos t, y=bsin⁡ty = b\sin t
Cycloid arch3π3\pi (for unit cycloid)

Coming Up: Part 5 covers surface area of revolution for parametric curves.

Part 5: Eliminating the Parameter

Parametric Curves & Calculus

Part 5 of 7 — Surface Area & Volume of Revolution

When parametric curves are revolved around an axis, we can compute the surface area and volume using modified integral formulas.

Surface Area of Revolution

Revolution about the xx-axis: SA=2π∫ab∣y(t)∣⋅(x′)2+(y′)2 dt\boxed{SA = 2\pi \int_a^b |y(t)| \cdot \sqrt{(x')^2 + (y')^2}\,dt}

Revolution about the yy-axis: SA=2π∫ab∣x(t)∣⋅(x′)2+(y′)2 dt\boxed{SA = 2\pi \int_a^b |x(t)| \cdot \sqrt{(x')^2 + (y')^2}\,dt}

The factor 2πr2\pi r comes from the circumference of revolution, and ds=(x′)2+(y′)2 dtds = \sqrt{(x')^2 + (y')^2}\,dt is the arc element.

Example: Sphere from x=Rcos⁡tx = R\cos t, y=Rsin⁡ty = R\sin t, 0≤t≤π0 \le t \le \pi

Revolving the upper semicircle about the xx-axis:

SA=2π∫0πRsin⁡t⋅R dt=2πR2∫0πsin⁡t dt=2πR2⋅2=4πR2SA = 2\pi \int_0^{\pi} R\sin t \cdot R\,dt = 2\pi R^2 \int_0^{\pi} \sin t\,dt = 2\pi R^2 \cdot 2 = 4\pi R^2

SAsphere=4πR2✓\boxed{SA_{\text{sphere}} = 4\pi R^2 \quad \checkmark}

Volume of Revolution (Disk/Washer)

About the xx-axis (using disks): V=π∫ab[y(t)]2⋅x′(t) dtV = \pi \int_a^b [y(t)]^2 \cdot x'(t)\,dt

Example: Sphere volume from semicircle

x=Rcos⁡tx = R\cos t, y=Rsin⁡ty = R\sin t, 0≤t≤π0 \le t \le \pi:

V=π∫0πR2sin⁡2t⋅(−Rsin⁡t) dt=−πR3∫0πsin⁡3t dtV = \pi \int_0^{\pi} R^2\sin^2 t \cdot (-R\sin t)\,dt = -\pi R^3 \int_0^{\pi} \sin^3 t\,dt

=πR3⋅43=43πR3= \pi R^3 \cdot \frac{4}{3} = \frac{4}{3}\pi R^3

Vsphere=43πR3✓\boxed{V_{\text{sphere}} = \frac{4}{3}\pi R^3 \quad \checkmark}

AP Tip: Volume problems with parametric curves often appear in BC FRQs. Set up the integral carefully, matching the revolution axis.

Surface Area & Volume

Identify the Setup

Quick Computation

Key Takeaways — Part 5

QuantityAbout xx-axisAbout yy-axis
Surface area$2\pi \inty
Volume (disk)π∫y2x′ dt\pi \int y^2 x'\,dtπ∫x2y′ dt\pi \int x^2 y'\,dt

Coming Up: Part 6 is a Problem-Solving Workshop with mixed parametric problems.

Part 6: Practice Workshop

Parametric Curves & Calculus

Part 6 of 7 — Problem-Solving Workshop

Mixed practice covering all parametric curve concepts: graphing, derivatives, arc length, area, and applications.

Workshop Problems

AP FRQ-Style Problem

A particle moves with x(t)=t3−3tx(t) = t^3 - 3t, y(t)=3t2−9y(t) = 3t^2 - 9 for −2≤t≤2-2 \le t \le 2.

(a) Find all times when the particle has a horizontal tangent.

dy/dt=6t=0  ⟹  t=0dy/dt = 6t = 0 \implies t = 0. Check: dx/dt=3(0)2−3=−3≠0dx/dt = 3(0)^2 - 3 = -3 \ne 0. \checkmark

Horizontal tangent at t=0t = 0: point (0,−9)(0, -9).

(b) Find all times when the particle has a vertical tangent.

dx/dt=3t2−3=3(t−1)(t+1)=0  ⟹  t=±1dx/dt = 3t^2 - 3 = 3(t-1)(t+1) = 0 \implies t = \pm 1

At t=1t = 1: dy/dt=6≠0dy/dt = 6 \ne 0. Point: (−2,−6)(-2, -6). \checkmark At t=−1t = -1: dy/dt=−6≠0dy/dt = -6 \ne 0. Point: (2,−6)(2, -6). \checkmark

(c) Find dy/dxdy/dx at t=2t = 2.

dydx=6(2)3(4)−3=129=43\frac{dy}{dx} = \frac{6(2)}{3(4)-3} = \frac{12}{9} = \frac{4}{3}

Mixed Practice

FRQ Computation

Workshop Recap

FRQ Strategy for Parametric Problems:

  1. Find derivatives: dx/dtdx/dt, dy/dtdy/dt, dy/dxdy/dx
  2. Identify special points: horizontal/vertical tangents
  3. Set up and evaluate integrals: arc length, area
  4. Interpret results in context of motion

Coming Up: Part 7 is the Comprehensive Review of parametric curves.

Part 7: Final Assessment

Parametric Curves & Calculus

Part 7 of 7 — Comprehensive Review

Master all parametric curve concepts: equations, derivatives, arc length, area, and surface area.

ConceptKey Formula
Slopedydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}
Second Derivatived2ydx2=ddt(dy/dx)dx/dt\frac{d^2y}{dx^2} = \frac{\frac{d}{dt}(dy/dx)}{dx/dt}
Arc LengthL=∫ab(dx/dt)2+(dy/dt)2 dtL = \int_a^b \sqrt{(dx/dt)^2+(dy/dt)^2}\,dt
AreaA=∫aby(t) x′(t) dtA = \int_a^b y(t)\,x'(t)\,dt (or −∫y x′ dt-\int y\,x'\,dt)
Speedv=(dx/dt)2+(dy/dt)2v = \sqrt{(dx/dt)^2+(dy/dt)^2}

Comprehensive Assessment

Quick-Reference Decision Guide

Given a parametric problem, identify what is asked:

Asked ForSet Up
Tangent line slopedy/dx=(dy/dt)/(dx/dt)dy/dx = (dy/dt)/(dx/dt) at given tt
Horizontal tangentSolve dy/dt=0dy/dt = 0, verify dx/dt≠0dx/dt \ne 0
Vertical tangentSolve dx/dt=0dx/dt = 0, verify dy/dt≠0dy/dt \ne 0
ConcavityCompute d2y/dx2d^2y/dx^2
Distance traveled∫ab(x′)2+(y′)2 dt\int_a^b \sqrt{(x')^2+(y')^2}\,dt
Area enclosed−∮y dx=−∫aby(t) x′(t) dt-\oint y\,dx = -\int_a^b y(t)\,x'(t)\,dt
Surface area (about xx-axis)2π∫y (x′)2+(y′)2 dt2\pi\int y\,\sqrt{(x')^2+(y')^2}\,dt

AP Key Fact: On the AP exam, distinguish between distance traveled (always positive, involves speed integral) and displacement (Δx,Δy\Delta x, \Delta y separately). They ask both!

Concept Connections

Final Computation

Parametric Curves Complete!

You have mastered:

  • Parametric equations, elimination, and graphing
  • First and second derivatives via the chain rule
  • Arc length and speed computations
  • Area under and enclosed by parametric curves
  • Surface area and volume of revolution

AP Exam Note: Parametric/polar/vector questions appear as a dedicated FRQ (usually problem 2 or 3). Practice computing derivatives and integrals quickly since both calculator and non-calculator parts appear.