Parametric Equations Solver

Parametric form, conversion to Cartesian, and derivatives of parametric curves
x = 2t + 1, y = t - 3 โ€” eliminate the parameter
Parametric equation of the circle centred (3, -2) with radius 5
dy/dx for x = t^2, y = t^3 - 3t at t = 2
Parametric form of the line through (1, 4) with direction (2, -3)

What Parametric Form Is

In Cartesian form a curve is a relation between xx and yy. In parametric form both coordinates are written as functions of a third variable, the parameter, usually tt:

x=f(t),y=g(t)x = f(t), \qquad y = g(t)

Each value of tt produces one point (f(t),g(t))(f(t), g(t)), and as tt runs through its interval the point traces the curve. Think of tt as time and the curve as the path of a moving object.

This buys you three things Cartesian form cannot give:

  • Curves that fail the vertical line test. A full circle is not a function of xx, but x=cosโกtx = \cos t, y=sinโกty = \sin t describes it in one piece.
  • Direction and speed. The parametrisation says which way the point moves and how fast โ€” information the picture alone does not carry.
  • A natural extension to 3D, where xx, yy and zz are each functions of tt.

Because the same set of points can be traced by many different parametrisations, a parametric description carries strictly more information than the picture alone: it records where the motion starts and how fast it passes each point.

Standard Parametrisations and Converting Back

Line through the point (x0,y0)(x_0, y_0) with direction vector โŸจa,bโŸฉ\langle a, b \rangle:

x=x0+at,y=y0+btx = x_0 + at, \qquad y = y_0 + bt

Circle of radius rr centred at (h,k)(h, k):

x=h+rcosโกt,y=k+rsinโกt,0โ‰คt<2ฯ€x = h + r\cos t, \qquad y = k + r\sin t, \qquad 0 \le t < 2\pi

Ellipse with semi-axes aa and bb: x=h+acosโกtx = h + a\cos t, y=k+bsinโกty = k + b\sin t.

To convert to Cartesian, eliminate tt. For polynomial equations, solve the simpler equation for tt and substitute into the other. For trigonometric ones, isolate cosโกt\cos t and sinโกt\sin t and use cosโก2t+sinโก2t=1\cos^2 t + \sin^2 t = 1.

To differentiate, divide the two rates rather than trying to find y(x)y(x):

dydx=dy/dtdx/dt,dxdtโ‰ 0\frac{dy}{dx} = \frac{dy/dt}{dx/dt}, \qquad \frac{dx}{dt} \neq 0

Common Mistakes to Avoid

  • Losing the domain. x=t2x = t^2, y=ty = t traces only the half of the parabola x=y2x = y^2 with xโ‰ฅ0x \ge 0 โ€” eliminating tt silently adds points the original curve never visits. State the restriction.
  • Treating the parametrisation as unique. x=t,y=2tx = t, y = 2t and x=3t,y=6tx = 3t, y = 6t draw the same line at different speeds. Both are correct answers.
  • Computing dy/dxdy/dx as dydtโ‹…dxdt\frac{dy}{dt} \cdot \frac{dx}{dt}. It is a quotient, not a product.
  • Mixing tt into a Cartesian answer. Once eliminated, the parameter must not appear anywhere in the final equation.
  • Ignoring where dx/dt=0dx/dt = 0. Those are the points with a vertical tangent, and the quotient formula fails there โ€” handle them separately.
  • Forgetting the second derivative rule: d2ydx2=ddtโ€‰โฃ(dydx)รทdxdt\frac{d^2y}{dx^2} = \frac{d}{dt}\!\left(\frac{dy}{dx}\right) \div \frac{dx}{dt}, not d2y/dt2d2x/dt2\frac{d^2y/dt^2}{d^2x/dt^2}.

Examples

Step 1: The yy equation is simpler, so solve it for tt: t=y+3t = y + 3.
Step 2: Substitute into the xx equation: x=2(y+3)+1=2y+7x = 2(y + 3) + 1 = 2y + 7.
Step 3: Rearrange for yy: y=xโˆ’72y = \frac{x - 7}{2}.
Step 4: Check at t=0t = 0: the parametric form gives (1,โˆ’3)(1, -3), and 1โˆ’72=โˆ’3\frac{1 - 7}{2} = -3 โœ“
Answer: y=xโˆ’72y = \dfrac{x - 7}{2}, a line of slope 12\tfrac{1}{2}

Step 1: Apply the standard form: x=3+5cosโกtx = 3 + 5\cos t, y=โˆ’2+5sinโกty = -2 + 5\sin t for 0โ‰คt<2ฯ€0 \le t < 2\pi.
Step 2: Isolate the trig functions: cosโกt=xโˆ’35\cos t = \frac{x - 3}{5} and sinโกt=y+25\sin t = \frac{y + 2}{5}.
Step 3: Use cosโก2t+sinโก2t=1\cos^2 t + \sin^2 t = 1: (xโˆ’3)225+(y+2)225=1\frac{(x-3)^2}{25} + \frac{(y+2)^2}{25} = 1.
Step 4: Multiply through by 25: (xโˆ’3)2+(y+2)2=25(x - 3)^2 + (y + 2)^2 = 25 โ€” the expected circle equation โœ“
Answer: x=3+5cosโกtx = 3 + 5\cos t, y=โˆ’2+5sinโกty = -2 + 5\sin t, equivalent to (xโˆ’3)2+(y+2)2=25(x-3)^2 + (y+2)^2 = 25

Step 1: Differentiate each coordinate with respect to tt: dxdt=2t\frac{dx}{dt} = 2t and dydt=3t2โˆ’3\frac{dy}{dt} = 3t^2 - 3.
Step 2: Divide: dydx=3t2โˆ’32t\frac{dy}{dx} = \frac{3t^2 - 3}{2t}.
Step 3: At t=2t = 2: numerator =3(4)โˆ’3=9= 3(4) - 3 = 9, denominator =2(2)=4= 2(2) = 4.
Step 4: So dydx=94\frac{dy}{dx} = \frac{9}{4}.
Step 5: The point of tangency is x=22=4x = 2^2 = 4, y=8โˆ’6=2y = 8 - 6 = 2.
Answer: dydx=94\dfrac{dy}{dx} = \dfrac{9}{4} at the point (4,2)(4, 2)

Frequently Asked Questions

It is a pair of functions x(t) and y(t) that together describe a curve, with t as an independent parameter rather than one of the coordinates. Every value of t gives one point, so the curve is traced out in a definite order and direction as t increases.

Because many curves are not functions of x. A circle, an ellipse and any looping path fail the vertical line test, yet each has a simple parametric description. Parametric form also records the direction and speed of motion along the curve, which is essential in physics and in calculus problems about velocity.

Eliminate the parameter. For polynomial equations, solve the easier one for t and substitute into the other. For sine and cosine, isolate cos t and sin t and use the identity cos squared plus sin squared equals one. Always state any restriction on x or y that the original parametrisation imposed.

No. The same curve has infinitely many parametrisations, differing in starting point, direction and speed. Replacing t with 2t or with -t traces the identical set of points, so any correct parametrisation is an acceptable answer unless the question specifies the motion.

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