Parametric Equations and Polar Coordinates Study Notes

PARAMETRIZATIONS OF PLANE CURVES

Definition of Parametric Equations

  • When the coordinates xx and yy of a point P(x,y)P(x, y) on a curve are given as functions of a third variable tt (called the parameter), the equations are known as parametric equations.

  • The set of points (x,y)(x, y) generated as tt varies over an interval is called the graph of the equations.

Algebraic Method: Converting to Cartesian Equations

  • To identify a curve defined by parametric equations, one can often eliminate the parameter tt to obtain a Cartesian equation relating xx and yy.

  • Example 1: Determine the Cartesian equation and sketch the curve defined by x=t2x = t^2, y=t+1y = t + 1 for -\infty < t < \infty.

    • Solution: From y=t+1y = t + 1, we find t=y1t = y - 1.

    • Substituting into the expression for xx yields: x=(y1)2x = (y - 1)^2.

    • This is a parabola opening to the right with its vertex at (0,1)(0, 1).

Examples of Parametric Path Identification

  • Example (a): x=tx = \sqrt{t}, y=ty = t, for t0t \geq 0.

    • Squaring xx gives x2=tx^2 = t. Since y=ty = t, the Cartesian equation is y=x2y = x^2.

    • Because x=tx = \sqrt{t}, the domain is restricted to x0x \geq 0.

  • Example (b): x=cos(t)x = \cos(t), y=sin(t)y = \sin(t), for 0tπ0 \leq t \leq \pi.

    • Using the identity cos2(t)+sin2(t)=1\cos^2(t) + \sin^2(t) = 1, we get x2+y2=1x^2 + y^2 = 1.

    • For the interval 0tπ0 \leq t \leq \pi, yy remains non-negative (y0y \geq 0), representing the upper semi-circle.

  • Example (c): x=1+sin(2t)x = 1 + \sin(2t), y=cos(2t)2y = \cos(2t) - 2, for 0t3π40 \leq t \leq \frac{3\pi}{4}.

    • Isolate the trigonometric terms: sin(2t)=x1\sin(2t) = x - 1 and cos(2t)=y+2\cos(2t) = y + 2.

    • Apply the identity sin2(2t)+cos2(2t)=1\sin^2(2t) + \cos^2(2t) = 1.

    • The Cartesian equation is (x1)2+(y+2)2=1(x - 1)^2 + (y + 2)^2 = 1.

    • The path is an arc of a circle centered at (1,2)(1, -2) with radius 11.

Additional Examples from Practice

  • Linear Path: x=2t5x = 2t - 5, y=4t7y = 4t - 7 for - \infty < t < \infty .

    • t=x+52t = \frac{x + 5}{2}.

    • y=4(x+52)7=2(x+5)7=2x+107=2x+3y = 4\left(\frac{x + 5}{2}\right) - 7 = 2(x + 5) - 7 = 2x + 10 - 7 = 2x + 3.

  • Parabolic Path: x=4t+3x = 4t + 3, y=16t29y = 16t^2 - 9 for 1t1-1 \leq t \leq 1.

    • t=x34t = \frac{x - 3}{4}.

    • y=16(x34)29=16((x3)216)9=(x3)29y = 16\left(\frac{x - 3}{4}\right)^2 - 9 = 16\left(\frac{(x - 3)^2}{16}\right) - 9 = (x - 3)^2 - 9.

  • Exponential Path: x=e2t+1x = e^{2t} + 1, y=ety = e^t.

    • Recognize that e2t=(et)2e^{2t} = (e^t)^2.

    • Therefore, x=y2+1x = y^2 + 1.

CALCULUS WITH PARAMETRIC CURVES

Tangents of Parametrized Curves

  • If x=f(t)x = f(t) and y=g(t)y = g(t) are differentiable, then the slope dydx\frac{dy}{dx} is calculated using the chain rule:     dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy / dt}{dx / dt}, provided dx/dt0dx / dt \neq 0.

  • Example 1: If x=t2+3x = t^2 + 3 and y=t21y = t^2 - 1, find dydx\frac{dy}{dx} at t=6t = 6.

    • dxdt=2t\frac{dx}{dt} = 2t, dydt=2t\frac{dy}{dt} = 2t.

    • dydx=2t2t=1\frac{dy}{dx} = \frac{2t}{2t} = 1.

    • At t=6t = 6, dydx=1\frac{dy}{dx} = 1.

  • Example 2: Find the tangent to the curve x=sec(t)x = \sec(t), y=tan(t)y = \tan(t) for \frac{-\pi}{2} < t < \frac{\pi}{2} at the point (2,1)(\sqrt{2}, 1) where t=π4t = \frac{\pi}{4}.

    • dxdt=sec(t)tan(t)\frac{dx}{dt} = \sec(t)\tan(t), dydt=sec2(t)\frac{dy}{dt} = \sec^2(t).

    • dydx=sec2(t)sec(t)tan(t)=sec(t)tan(t)=csc(t)\frac{dy}{dx} = \frac{\sec^2(t)}{\sec(t)\tan(t)} = \frac{\sec(t)}{\tan(t)} = \csc(t).

    • At t=π4t = \frac{\pi}{4}, dydx=csc(π4)=2\frac{dy}{dx} = \csc\left(\frac{\pi}{4}\right) = \sqrt{2}.

    • Equation of tangent: y1=2(x2)y=2x2+1y=2x1y - 1 = \sqrt{2}(x - \sqrt{2}) \Rightarrow y = \sqrt{2}x - 2 + 1 \Rightarrow y = \sqrt{2}x - 1.

Second Order Derivatives

  • The second derivative d2ydx2\frac{d^2y}{dx^2} for a parametric curve is defined as:     d2ydx2=ddx(dydx)=ddt(dydx)dxdt\frac{d^2y}{dx^2} = \frac{d}{dx}\left(\frac{dy}{dx}\right) = \frac{\frac{d}{dt}\left(\frac{dy}{dx}\right)}{\frac{dx}{dt}}.

  • Example 3: Find d2ydx2\frac{d^2y}{dx^2} as a function of tt if x=t2tx = t^2 - t and y=t3ty = t^3 - t.

    • dxdt=2t1\frac{dx}{dt} = 2t - 1, dydt=3t21\frac{dy}{dt} = 3t^2 - 1.

    • dydx=3t212t1\frac{dy}{dx} = \frac{3t^2 - 1}{2t - 1}.

    • ddt(3t212t1)=(2t1)(6t)(3t21)(2)(2t1)2=12t26t6t2+2(2t1)2=6t26t+2(2t1)2\frac{d}{dt}\left(\frac{3t^2 - 1}{2t - 1}\right) = \frac{(2t - 1)(6t) - (3t^2 - 1)(2)}{(2t - 1)^2} = \frac{12t^2 - 6t - 6t^2 + 2}{(2t - 1)^2} = \frac{6t^2 - 6t + 2}{(2t - 1)^2}.

    • d2ydx2=6t26t+2(2t1)3\frac{d^2y}{dx^2} = \frac{6t^2 - 6t + 2}{(2t - 1)^3}.

Length of a Parametrically Defined Curve (Arc Length)

  • If x=f(t)x = f(t) and y=g(t)y = g(t) for atba \leq t \leq b, and the derivatives are continuous, the arc length LL is given by:     L=ab(dxdt)2+(dydt)2dtL = \int_a^b \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2}\,dt.

  • Example 4: Find the length of a circle of radius rr defined by x=rcos(t)x = r\cos(t), y=rsin(t)y = r\sin(t) for 0 \leq t \n\leq 2\pi .

    • dxdt=rsin(t)\frac{dx}{dt} = -r\sin(t), dydt=rcos(t)\frac{dy}{dt} = r\cos(t).

    • (dxdt)2+(dydt)2=r2sin2(t)+r2cos2(t)=r2\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2 = r^2\sin^2(t) + r^2\cos^2(t) = r^2.

    • L=02πr2dt=02πrdt=[rt]02π=2πrL = \int_0^{2\pi} \sqrt{r^2}\,dt = \int_0^{2\pi} r\,dt = [rt]_0^{2\pi} = 2\pi r.

POLAR COORDINATES

Fundamentals and Representation

  • Definition: Points are represented as (r,θ)(r, \theta), where rr is the directed distance from the origin (pole) and θ\theta is the directed angle from the positive x-axis (initial ray).

  • Non-uniqueness: A single point in the plane can have multiple polar representations:

    • (r,θ)(r, \theta) is the same as (r,θ+2nπ)(r, \theta + 2n\pi) for any integer nn.

    • (r,θ)(r, \theta) is the same as (r,θ+π)(-r, \theta + \pi).

  • Sign Conventions:

    • θ\theta is positive in the anticlockwise direction.

    • θ\theta is negative in the clockwise direction.

    • A point (r,θ)(-r, \theta) lies in the opposite direction of (r,θ)(r, \theta).

Exercises: Polar Representations

  • Point (a): (3, 225°)

    • Equivalent representations: (3,1350˘026deg;)(3, -135\text{\u0026deg;}), (3,450˘026deg;)(-3, 45\text{\u0026deg;}), (3,3150˘026deg;)(-3, -315\text{\u0026deg;}).

  • Point (d): (2, -225°)

    • Visualized as 1350˘026deg;135\text{\u0026deg;} anticlockwise.

    • Equivalent: (2,1350˘026deg;)(2, 135\text{\u0026deg;}), (2,450˘026deg;)(-2, -45\text{\u0026deg;}), (2,3150˘026deg;)(-2, 315\text{\u0026deg;}).

Basic Polar Graphs

  1. Circles: If r=ar = a (constant), the graph is a circle of radius a|a| centered at the origin.

  2. Lines: If θ=θ0\theta = \theta_0 (constant), the graph is a line passing through the origin making an angle θ0\theta_0 with the initial ray.

Relating Polar and Cartesian Coordinates

  • Equations for Conversion:

    • x=rcos(θ)x = r\cos(\theta)

    • y=rsin(θ)y = r\sin(\theta)

    • r2=x2+y2r^2 = x^2 + y^2

    • tan(θ)=yx\tan(\theta) = \frac{y}{x}

  • Example 1b: Convert (4,2π3)(4, \frac{-2\pi}{3}) to Cartesian.

    • x=4cos(2π3)=4(12)=2x = 4\cos\left(\frac{-2\pi}{3}\right) = 4\left(\frac{-1}{2}\right) = -2.

    • y=4sin(2π3)=4(32)=23y = 4\sin\left(\frac{-2\pi}{3}\right) = 4\left(\frac{-\sqrt{3}}{2}\right) = -2\sqrt{3}.

  • Equation Conversion Example 3a: r=4csc(θ)r = 4\csc(\theta).

    • r=4sin(θ)rsin(θ)=4y=4r = \frac{4}{\sin(\theta)} \Rightarrow r\sin(\theta) = 4 \Rightarrow y = 4. (A horizontal line).

  • Equation Conversion Example 4d: (x2+y22y)2=4(x2+y2)(x^2 + y^2 - 2y)^2 = 4(x^2 + y^2).

    • (r22rsin(θ))2=4r2(r^2 - 2r\sin(\theta))^2 = 4r^2.

    • r22rsin(θ)=±2rr2sin(θ)=±2r^2 - 2r\sin(\theta) = \pm 2r \Rightarrow r - 2\sin(\theta) = \pm 2.

    • Resulting in equations like r=2+2sin(θ)r = 2 + 2\sin(\theta) (a cardioid).

GRAPHING IN POLAR COORDINATES

Symmetries in Polar Graphs

  • Symmetry about the x-axis: Equation remains unchanged when θ\theta is replaced by θ-\theta (or (r,θ)(r, -\theta)).

  • Symmetry about the y-axis: Equation remains unchanged when θ\theta is replaced by πθ\pi - \theta (or (r,θ)(-r, -\theta)).

  • Symmetry about the Origin: Equation remains unchanged when rr is replaced by r-r (or θ\theta is replaced by π+θ\pi + \theta).

Common Curves

  • Cardioids: e.g., r=a(1±cos(θ))r = a(1 \pm \cos(\theta)) or r=a(1±sin(θ))r = a(1 \pm \sin(\theta)).

  • Limaçons: r=a±bcos(θ)r = a \pm b\cos(\theta) or r=a±bsin(θ)r = a \pm b\sin(\theta).

  • Rose Petals: r=acos(nθ)r = a\cos(n\theta) or r=asin(nθ)r = a\sin(n\theta).

    • If nn is odd, there are nn petals.

    • If nn is even, there are 2n2n petals.

  • Lemniscates: r2=a2cos(2θ)r^2 = a^2\cos(2\theta) or r2=a2sin(2θ)r^2 = a^2\sin(2\theta).

Slope of a Polar Curve

  • The slope of the curve r=f(θ)r = f(\theta) at the point (r,θ)(r, \theta) is:     dydx=dfdθsin(θ)+f(θ)cos(θ)dfdθcos(θ)f(θ)sin(θ)\frac{dy}{dx} = \frac{\frac{df}{d\theta}\sin(\theta) + f(\theta)\cos(\theta)}{\frac{df}{d\theta}\cos(\theta) - f(\theta)\sin(\theta)}.

AREAS AND LENGTHS IN POLAR COORDINATES

Area in the Plane

  • Area of a Fan-Shaped Region: The area of the region between the origin and the curve r=f(θ)r = f(\theta) from θ=α\theta = \alpha to θ=β\theta = \beta is:     A=αβ12r2dθ=αβ12(f(θ))2dθA = \int_{\alpha}^{\beta} \frac{1}{2}r^2\,d\theta = \int_{\alpha}^{\beta} \frac{1}{2}(f(\theta))^2\,d\theta.

  • Area Between Two Curves: If 0r1(θ)rr2(θ)0 \leq r_1(\theta) \leq r \leq r_2(\theta), the area is:     A=αβ12(r22r12)dθA = \int_{\alpha}^{\beta} \frac{1}{2}(r_2^2 - r_1^2)\,d\theta.

Length of a Polar Curve

  • If r=f(θ)r = f(\theta) has a continuous derivative for αθβ\alpha \leq \theta \leq \beta, the arc length LL is:     L=αβr2+(drdθ)2dθL = \int_{\alpha}^{\beta} \sqrt{r^2 + \left(\frac{dr}{d\theta}\right)^2}\,d\theta.

  • Example: Find the length of the cardioid r=1cos(θ)r = 1 - \cos(\theta).

    • drdθ=sin(θ)\frac{dr}{d\theta} = \sin(\theta).

    • r2+(drdθ)2=(1cos(θ))2+sin2(θ)=12cos(θ)+cos2(θ)+sin2(θ)=22cos(θ)r^2 + (\frac{dr}{d\theta})^2 = (1 - \cos(\theta))^2 + \sin^2(\theta) = 1 - 2\cos(\theta) + \cos^2(\theta) + \sin^2(\theta) = 2 - 2\cos(\theta).

    • Use identity: 22cos(θ)=4sin2(θ2)2 - 2\cos(\theta) = 4\sin^2\left(\frac{\theta}{2}\right).

    • L=02π4sin2(θ/2)dθ=02π2sin(θ/2)dθ=[4cos(θ/2)]02π=4(4)=8L = \int_0^{2\pi} \sqrt{4\sin^2(\theta/2)}\,d\theta = \int_0^{2\pi} 2\sin(\theta/2)\,d\theta = [-4\cos(\theta/2)]_0^{2\pi} = 4 - (-4) = 8.

CONIC SECTIONS

Parabolas

  • Standard Forms (Vertex at (0,0)(0, 0)):

    • x2=4pyx^2 = 4py: Opens Up (Focus at (0,p)(0, p), Directrix y=py = -p).

    • x2=4pyx^2 = -4py: Opens Down (Focus at (0,p)(0, -p), Directrix y=py = p).

    • y2=4pxy^2 = 4px: Opens Right (Focus at (p,0)(p, 0), Directrix x=px = -p).

    • y2=4pxy^2 = -4px: Opens Left (Focus at (p,0)(-p, 0), Directrix x=px = p).

  • Parameter pp: Distance from the vertex to the focus or directrix.

Ellipses

  • Definition: The set of points where the sum of distances from two fixed foci is constant (2a2a).

  • Standard Equations (Center at Origin):

    • Horizontal Major Axis: x2a2+y2b2=1\frac{x^2}{a^2} + \frac{y^2}{b^2} = 1 (a > b).

    • Vertical Major Axis: x2b2+y2a2=1\frac{x^2}{b^2} + \frac{y^2}{a^2} = 1 (a > b).

  • Constants:

    • c=a2b2c = \sqrt{a^2 - b^2} (Center-to-focus distance).

    • Vertices: (±a,0)(\pm a, 0) or (0,±a)(0, \pm a).

    • Foci: (±c,0)(\pm c, 0) or (0,±c)(0, \pm c).

Hyperbolas

  • Standard Equations (Center at Origin):

    • Horizontal Transverse Axis: x2a2y2b2=1\frac{x^2}{a^2} - \frac{y^2}{b^2} = 1.

    • Vertical Transverse Axis: y2a2x2b2=1\frac{y^2}{a^2} - \frac{x^2}{b^2} = 1.

  • Constants:

    • c=a2+b2c = \sqrt{a^2 + b^2} (Center-to-focus distance).

    • Asymptotes: y=±baxy = \pm \frac{b}{a}x (horizontal) or y=±abxy = \pm \frac{a}{b}x (vertical).

CONIC SECTIONS IN POLAR COORDINATES

Eccentricity (ee)

  • Defines the type of conic based on the ratio of the distance from a point PP to the focus FF (PFPF) versus the distance to the directrix DD (PDPD):     PF=ePDPF = e \cdot PD.

    • Parabola: e=1e = 1.

    • Ellipse: e < 1 .

    • Hyperbola: e > 1 .

  • For ellipses and hyperbolas, e=ca=distance between focidistance between verticese = \frac{c}{a} = \frac{\text{distance between foci}}{\text{distance between vertices}}.

Polar Equations of Conics

  • A conic with a focus at the origin and a directrix at x=kx = k (to the right) has the equation:     r=ke1+ecos(θ)r = \frac{ke}{1 + e\cos(\theta)}.

  • General variations depending on directrix position (left, right, above, below):     r=ke1±ecos(θ)r = \frac{ke}{1 \pm e\cos(\theta)} or r=ke1±esin(θ)r = \frac{ke}{1 \pm e\sin(\theta)}.

Lines and Circles in Polar Form

  • Lines: A line through P0(r0,θ0)P_0(r_0, \theta_0) perpendicular to the ray from the origin to P0P_0 has equation:     rcos(θθ0)=r0r\cos(\theta - \theta_0) = r_0.

  • Circles: A circle of radius aa centered at P0(r0,θ0)P_0(r_0, \theta_0) follows the law of cosines:     a2=r2+r022rr0cos(θθ0)a^2 = r^2 + r_0^2 - 2rr_0\cos(\theta - \theta_0).

    • If the center is on the positive x-axis (a,0)(a, 0): r=2acos(θ)r = 2a\cos(\theta).

    • If the center is on the positive y-axis (0,a)(0, a): r=2asin(θ)r = 2a\sin(\theta).