Parametric Equations

Sections 8.6–8.7 — x and y as separate functions of time t

MAT 172 — Final Prep
Parametric equations describe x and y separately using a third variable t — usually time. A regular equation tells you the shape of a path. Parametric equations tell you the shape AND how something moves along it — direction, speed, position at any moment.
The key ideaInstead of y = f(x), you have x = f(t) AND y = g(t). Both x and y depend on a third variable t. As t increases, you get a sequence of (x, y) points that trace a path — with direction built in.
x = f(t)    y = g(t)    t ∈ [a, b]
The point at time t is (f(t), g(t)). t is the parameter. As t increases, the point traces a path with direction.
Live animation — watch the point trace the path
t = 0.00  ·  x =  ·  y =
Why parametric vs regular equations?Some curves aren't functions of x — a circle, for example, fails the vertical line test. Parametric equations describe any curve including ones that loop back on themselves or go left and right freely. They also encode direction: which way does the curve trace as t increases?
x = t + 1, y = t² − 2, for t ∈ [−2, 2]
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Choose t values in the interval, evaluate both equations
tx = t + 1y = t² − 2Point (x, y)
−2−12(−1, 2)
−10−1(0, −1)
01−2(1, −2)
12−1(2, −1)
232(3, 2)
2
Plot the points in order and draw arrows showing direction of increasing t
Curve traces left-to-right as t increases. Shape: parabola opening upward.
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Orientation — arrows are everything
The orientation of a parametric curve is the direction it traces as t increases. Always mark this with arrows on your graph.

Two parametric equations can produce the same rectangular curve but with opposite orientations — they look identical on paper but are different parametrizations. The exam will ask about this.

Example: x = cos(t), y = sin(t) traces the unit circle counterclockwise. x = cos(−t), y = sin(−t) traces it clockwise. Same circle, opposite direction.
Eliminating the parameterConverting parametric equations to a rectangular equation (y in terms of x). Solve one equation for t, substitute into the other. Always carry over domain restrictions — the rectangular equation may look familiar but only covers part of it.
x = t + 2, y = t² — eliminate t
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Solve x equation for t: x = t + 2 → t = x − 2
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Substitute into y: y = t² = (x − 2)²
3
Check restrictions: if t ∈ [−2, 2], then x = t+2 ∈ [0, 4]. So restrict x to [0, 4].
y = (x − 2)², x ∈ [0, 4] — a parabola but only the portion for x between 0 and 4
x = 2t − 1, y = 3t + 4 — eliminate t (linear)
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Solve for t from x: t = (x + 1)/2
2
Substitute: y = 3·(x+1)/2 + 4 = (3x+3)/2 + 4 = (3x + 11)/2
y = (3x + 11)/2 — a straight line
x = 3cos(t), y = 2sin(t) — eliminate t
1
Isolate trig functions: cos(t) = x/3, sin(t) = y/2
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Use identity sin²t + cos²t = 1: (y/2)² + (x/3)² = 1
3
Rewrite: x²/9 + y²/4 = 1
x²/9 + y²/4 = 1 — an ellipse with a = 3, b = 2
x = cos(t), y = sin(t) — eliminate t
1
cos(t) = x, sin(t) = y
2
sin²t + cos²t = 1 → x² + y² = 1
x² + y² = 1 — the unit circle, traced counterclockwise
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The restriction trap — most common exam mistake
When you eliminate t, the rectangular equation may look like a familiar full curve — but parametric equations usually only trace PART of it.

x = t², y = t for t ≥ 0 eliminates to x = y², but only for y ≥ 0. The full parabola goes both up and down; this version only traces the top half.

Always ask: what values does x take as t varies over its interval? Those are your x-restrictions on the rectangular equation.
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Connection to conics — the big picture
Every conic section has a parametric form:

Circle: x = r·cos(t), y = r·sin(t)
Ellipse: x = a·cos(t), y = b·sin(t)
Parabola: x = t, y = t² (or x = t², y = t)
Hyperbola: x = a·sec(t), y = b·tan(t)

This is why parametric equations and conics appear in the same chapter — they're two ways of describing the same curves.
Common parametric shapesKnow these cold. On the exam you'll likely see one of these or a variation. The key is recognizing the form and knowing how the orientation works.
Line: x = at + h, y = bt + k
Linear in t → straight line. Slope = b/a. Point at t = 0: (h, k). Direction: moving in direction (a, b) as t increases.
Eliminate: y − k = (b/a)(x − h) — slope-intercept form
Parabola: x = t, y = at² + bt + c (or x and y swapped)
x = t → just substitute: y = at² + bt + c becomes y = ax² + bx + c (vertical parabola)
y = t, x = at² → x = ay² (horizontal parabola)
The squared variable determines which way it opens
Circle/Ellipse: x = a·cos(t), y = b·sin(t)
a = b: circle of radius a, centered at origin
a ≠ b: ellipse with semi-axes a (horizontal) and b (vertical)
Orientation: counterclockwise as t goes from 0 to 2π
x²/a² + y²/b² = 1 — recognizable from conic sections chapter
Reversed orientation: x = a·cos(−t), y = b·sin(−t)
cos(−t) = cos(t) (even), sin(−t) = −sin(t) (odd)
Same ellipse/circle shape, but traced clockwise instead
Same rectangular equation x²/a² + y²/b² = 1, opposite orientation
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How to identify shape from parametric form
Both linear in t? → Line
One linear, one quadratic? → Parabola (squared one determines direction)
Both trig (cos/sin)? → Circle or ellipse
sec and tan? → Hyperbola

Quick check: eliminate t and see what you get. The rectangular form is the shape without direction.
Projectile motionThe biggest real-world application of parametric equations. Horizontal and vertical motion are independent — gravity only affects vertical. x and y each get their own equation, both depending on time t.
x(t) = (v₀ cos θ) t     y(t) = −½gt² + (v₀ sin θ)t + h₀
v₀ = initial speed · θ = launch angle · g = 32 ft/s² or 9.8 m/s² · h₀ = initial height
Interactive projectile launcher
45°
60 ft/s
0 ft
Max height
Range (distance)
Time in air
Equations

45° gives maximum range on flat ground · Try different angles to see why

A ball is launched at 80 ft/s at 30°, from ground level. Find: time in air, range, max height.
1
Set up: x(t) = 80cos(30°)t = 80(√3/2)t = 40√3 t. y(t) = −16t² + 80sin(30°)t = −16t² + 40t. (g = 32, so ½g = 16)
2
Time in air: Solve y(t) = 0. −16t² + 40t = 0 → t(−16t + 40) = 0 → t = 0 or t = 40/16 = 2.5 sec
3
Range: x(2.5) = 40√3(2.5) = 100√3 ≈ 173.2 ft
4
Max height: Vertex of y(t). t_max = −b/(2a) = −40/(2·(−16)) = 40/32 = 1.25 sec. y(1.25) = −16(1.5625) + 40(1.25) = −25 + 50 = 25 ft
Time in air: 2.5 sec · Range: 100√3 ≈ 173.2 ft · Max height: 25 ft
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The three projectile questions and how to answer each
Time in air: Set y(t) = 0, solve for t. Discard t = 0 (launch). The positive t is when it lands.

Range (horizontal distance): Plug the landing time into x(t).

Maximum height: The vertex of y(t). Use t = −b/(2a) to find when, then plug in to find height.

Height at a given distance: Set x(t) = distance, solve for t, plug t into y(t).

g values: 32 ft/s² or 9.8 m/s². The ½ in ½gt² makes it 16 ft/s² or 4.9 m/s² in the equation.
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Why 45° maximizes range (the math)
Range = (v₀²/g) · sin(2θ). This is maximized when sin(2θ) = 1, which means 2θ = 90°, so θ = 45°.

Also: complementary angles give the same range. 30° and 60° produce the same horizontal distance — try it in the simulator above.

Higher angle → more time in air but less horizontal speed. Lower angle → more horizontal speed but less time. 45° is the perfect balance.
Build your own parametric curve. Enter any expressions for x(t) and y(t) using the sliders, and watch the curve trace live with orientation arrows.
Parametric explorer
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3

Arrows show orientation — direction of increasing t

Identify the curve: x = 4cos(t), y = 3sin(t), t ∈ [0, 2π]
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Both involve cos and sin of same t → ellipse form
2
Isolate: cos(t) = x/4, sin(t) = y/3
3
Identity: (x/4)² + (y/3)² = 1 → x²/16 + y²/9 = 1
4
Orientation: at t=0: (4, 0). At t=π/2: (0, 3). Moving counterclockwise.
Ellipse: x²/16 + y²/9 = 1, a=4, b=3, traced counterclockwise starting at (4,0)