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Chapter 5 · Continuity and Differentiability

Exercise 5.6 · Q10: dydx\frac{dy}{dx} when x=a(cos⁡θ+θsin⁡θ)x=a(\cos\theta+\theta\sin\theta)⁠, y=a(sin⁡θ−θcos⁡θ)y=a(\sin\theta-\theta\cos\theta)

Exercise 5.6Parametric differentiation · Section 5.6
The question

If xx and yy are connected parametrically by the equations given in Exercises 1 to 10, without eliminating the parameter, Find dydx\dfrac{dy}{dx}⁠.

10. x=a(cos⁡θ+θsin⁡θ)x = a(\cos\theta + \theta\sin\theta)⁠, y=a(sin⁡θ−θcos⁡θ)y = a(\sin\theta - \theta\cos\theta)

Exam answer dxdθ=a(−sin⁡θ+sin⁡θ+θcos⁡θ)=aθcos⁡θ,dydθ=a(cos⁡θ−cos⁡θ+θsin⁡θ)=aθsin⁡θ\begin{aligned} \frac{dx}{d\theta} &= a(-\sin\theta + \sin\theta + \theta\cos\theta) \\ &= a\theta\cos\theta, \\ \frac{dy}{d\theta} &= a(\cos\theta - \cos\theta + \theta\sin\theta) \\ &= a\theta\sin\theta \end{aligned} dydx=dy/dθdx/dθ=aθsin⁡θaθcos⁡θ\begin{aligned} \frac{dy}{dx} &= \frac{dy/d\theta}{dx/d\theta} = \frac{a\theta\sin\theta}{a\theta\cos\theta} \end{aligned}

∴ dydx=tan⁡θ\therefore\ \dfrac{dy}{dx} = \tan\theta (θ≠0, cos⁡θ≠0)(\theta \ne 0,\ \cos\theta \ne 0)

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

Use dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}⁠. The terms θsin⁡θ\theta\sin\theta and θcos⁡θ\theta\cos\theta are products, so they need the product rule. When we do that, two terms cancel in each rate, leaving the very simple

dxdθ=aθcos⁡θ,dydθ=aθsin⁡θ,\frac{dx}{d\theta} = a\theta\cos\theta, \qquad \frac{dy}{d\theta} = a\theta\sin\theta,

and the ratio is tan⁡θ\tan\theta⁠.

Given, to find, and the plan
Given
x=a(cos⁡θ+θsin⁡θ)x = a(\cos\theta + \theta\sin\theta)⁠, y=a(sin⁡θ−θcos⁡θ)y = a(\sin\theta - \theta\cos\theta)⁠, with aa a nonzero constant and θ\theta the parameter.
To find
dydx\dfrac{dy}{dx}⁠, without eliminating θ\theta⁠.
Plan
Differentiate xx and yy with respect to θ\theta⁠, using the product rule on θsin⁡θ\theta\sin\theta and θcos⁡θ\theta\cos\theta⁠; find where dxdθ=0\frac{dx}{d\theta} = 0⁠; divide; picture the curve.

Basics you need

1Product rule

(uv)′=u′v+uv′(uv)' = u'v + uv' (Section 5.3). So

ddθ(θsin⁡θ)=sin⁡θ+θcos⁡θ,ddθ(θcos⁡θ)=cos⁡θ−θsin⁡θ.\begin{aligned} \tfrac{d}{d\theta}(\theta\sin\theta) &= \sin\theta + \theta\cos\theta, \\ \tfrac{d}{d\theta}(\theta\cos\theta) &= \cos\theta - \theta\sin\theta. \end{aligned}

Basics: derivative rules

2The parametric formula (Section 5.6)

dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}⁠, provided dxdθ≠0\frac{dx}{d\theta} \neq 0⁠. Lesson: parametric differentiation

3Zeros of cosine

cos⁡θ=0  ⟺  θ=(2n+1)π2\cos\theta = 0 \iff \theta = (2n+1)\frac{\pi}{2}⁠, n∈Zn \in \Z⁠; there sin⁡θ=±1\sin\theta = \pm1⁠. Basics: trigonometric identities

Solution

  1. Differentiate xx with respect to θ\theta

    Sum rule, with the product rule on θsin⁡θ\theta\sin\theta (Basic 1):

    dxdθ=a(−sin⁡θ+sin⁡θ+θcos⁡θ)=aθcos⁡θ.\begin{aligned} \frac{dx}{d\theta} &= a\left(-\sin\theta + \sin\theta + \theta\cos\theta\right) \\ &= a\theta\cos\theta. \end{aligned}
    cos⁡θ\cos\theta gives −sin⁡θ-\sin\theta⁠. The product θsin⁡θ\theta\sin\theta gives "derivative of the first times the second plus the first times the derivative of the second", 1⋅sin⁡θ+θcos⁡θ1\cdot\sin\theta + \theta\cos\theta⁠. The −sin⁡θ-\sin\theta and +sin⁡θ+\sin\theta cancel.
    Product rule (Section 5.3); ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\theta (Table 5.3). Basics: derivative rules
  2. Differentiate yy with respect to θ\theta

    dydθ=a(cos⁡θ−(cos⁡θ−θsin⁡θ))=aθsin⁡θ.\begin{aligned} \frac{dy}{d\theta} &= a\left(\cos\theta - (\cos\theta - \theta\sin\theta)\right) \\ &= a\theta\sin\theta. \end{aligned}
    sin⁡θ\sin\theta gives cos⁡θ\cos\theta⁠; the product θcos⁡θ\theta\cos\theta gives cos⁡θ−θsin⁡θ\cos\theta - \theta\sin\theta⁠, and it is subtracted, so the bracket is needed. The two cos⁡θ\cos\theta terms cancel and −(−θsin⁡θ)=+θsin⁡θ-(-\theta\sin\theta) = +\theta\sin\theta⁠.
    Basic 1, second line.
  3. Find where the formula may be used

    We need aθcos⁡θ≠0a\theta\cos\theta \neq 0⁠. Since a≠0a \neq 0⁠, this means

    θ≠0andcos⁡θ≠0,\theta \neq 0 \quad\text{and}\quad \cos\theta \neq 0,

    that is, θ≠0\theta \neq 0 and θ≠(2n+1)π2\theta \neq (2n+1)\frac{\pi}{2}⁠.

    A product is zero only when one of its factors is zero, and there are two variable factors here, θ\theta and cos⁡θ\cos\theta⁠. It is easy to forget the factor θ\theta⁠.
    Basic 3: the zeros of cosine.
  4. Divide

    For θ≠0\theta \neq 0 and cos⁡θ≠0\cos\theta \neq 0⁠,

    dydx=dy/dθdx/dθ=aθsin⁡θaθcos⁡θ=tan⁡θ.\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta} = \frac{a\theta\sin\theta}{a\theta\cos\theta} = \tan\theta.
    The common factor aθa\theta is not zero (Step 3), so it cancels, and sin⁡θcos⁡θ=tan⁡θ\frac{\sin\theta}{\cos\theta} = \tan\theta⁠.
    Parametric formula, Section 5.6. Lesson: parametric differentiation
  5. Picture the curve: the involute of a circle

    Two kinds of excluded value behave differently:

    • At θ=0\theta = 0 both rates are zero. The point is (a,0)(a, 0)⁠. Replacing θ\theta by −θ-\theta leaves xx unchanged and changes yy into −y-y⁠, so the part of the curve with θ<0\theta \lt 0 is the mirror image in the xx-axis of the part with θ>0\theta \gt 0⁠, and the two parts meet at (a,0)(a, 0) in a sharp tip (a cusp). The figure shows only θ≥0\theta \geq 0⁠.
    • At cos⁡θ=0\cos\theta = 0⁠, θ≠0\theta \neq 0⁠, we have dxdθ=0\frac{dx}{d\theta} = 0 but dydθ=aθsin⁡θ=±aθ≠0\frac{dy}{d\theta} = a\theta\sin\theta = \pm a\theta \neq 0⁠: the point moves straight up or down, the tangent is vertical, and there is no slope.
    x y O −4 −2 a a 2 θ = 0 θ = π/2 θ = π θ = 3π/4 θ = 3π/4: slope tan(3π/4) = −1 θ = π: slope 0; dashed: the string, length πa θ = 0: cusp; θ = π/2: vertical tangent circle of radius a (a = 1)
    The curve for a=1a = 1 and 0≤θ≤3π20 \leq \theta \leq \frac{3\pi}{2} (equal scales). It starts at (a,0)(a, 0)⁠; the tangent is vertical at θ=π2\theta = \frac{\pi}{2}⁠, the point (πa2,a)\big(\frac{\pi a}{2}, a\big)⁠, and horizontal at θ=π\theta = \pi⁠, the point (−a,πa)(-a, \pi a)⁠. At θ=3π4\theta = \frac{3\pi}{4} the slope is tan⁡3π4=−1\tan\frac{3\pi}{4} = -1⁠.

    The curve is the path traced by the end of a string unwound from a circle of radius aa⁠. Write T=(acos⁡θ, asin⁡θ)T = (a\cos\theta,\ a\sin\theta)⁠, a point of the circle. Then

    P−T=(aθsin⁡θ, −aθcos⁡θ),P - T = (a\theta\sin\theta,\ -a\theta\cos\theta),

    a segment of length ∣aθ∣|a\theta|⁠, which is the length of the arc of the circle from (a,0)(a, 0) to TT⁠: the unwound string. Our answer says the tangent at PP has the direction of (cos⁡θ, sin⁡θ)(\cos\theta,\ \sin\theta)⁠, the direction of the radius OTOT⁠, so it is perpendicular to the string. In the figure, at θ=π\theta = \pi the string (dashed) is vertical and the tangent horizontal.

    This explains the answer tan⁡θ\tan\theta⁠: the tangent to the curve is always parallel to the radius to the point where the string leaves the circle. The excluded value θ=0\theta = 0 is where the string has zero length, so the end of the string starts from rest.
    Slope of the direction (p,q)(p, q) is qp\frac{q}{p}⁠; here sin⁡θcos⁡θ=tan⁡θ\frac{\sin\theta}{\cos\theta} = \tan\theta⁠. Basics: slope at a point
Result dydx=tan⁡θ,\frac{dy}{dx} = \tan\theta,

for every θ\theta with θ≠0\theta \neq 0 and cos⁡θ≠0\cos\theta \neq 0⁠. (Textbook answer: tan⁡θ\tan\theta⁠.)

Check it with numbers

A short chord. Take a=1a = 1⁠, θ=2\theta = 2⁠: the point is (1.4024480, 1.7415911)(1.4024480,\ 1.7415911) and the predicted slope is tan⁡2≈−2.1850399\tan 2 \approx -2.1850399⁠. The points at θ=1.999\theta = 1.999 and θ=2.001\theta = 2.001 are (1.403279194, 1.739772544)(1.403279194,\ 1.739772544) and (1.401614606, 1.743409733)(1.401614606,\ 1.743409733)⁠, so

ΔyΔx=0.003637189−0.001664588≈−2.18504.\frac{\Delta y}{\Delta x} = \frac{0.003637189}{-0.001664588} \approx -2.18504.

The string. At θ=π\theta = \pi (a=1a = 1⁠): T=(−1,0)T = (-1, 0)⁠, and PP has x=cos⁡π+πsin⁡π=−1x = \cos\pi + \pi\sin\pi = -1⁠, y=sin⁡π−πcos⁡π=πy = \sin\pi - \pi\cos\pi = \pi⁠, so P=(−1,π)P = (-1, \pi)⁠. The string TPTP is vertical with length π\pi⁠, half the circumference, and the slope there is tan⁡π=0\tan\pi = 0⁠.

Common mistakes
  1. Differentiating θsin⁡θ\theta\sin\theta as cos⁡θ\cos\theta⁠. It is a product: sin⁡θ+θcos⁡θ\sin\theta + \theta\cos\theta⁠.
  2. Sign error with the bracket. In yy⁠, the whole derivative of θcos⁡θ\theta\cos\theta is subtracted: −(cos⁡θ−θsin⁡θ)-(\cos\theta - \theta\sin\theta)⁠.
  3. Forgetting θ≠0\theta \neq 0⁠. The factor θ\theta in dxdθ=aθcos⁡θ\frac{dx}{d\theta} = a\theta\cos\theta also vanishes.
  4. Dividing the wrong way round. dx/dθdy/dθ=cot⁡θ\frac{dx/d\theta}{dy/d\theta} = \cot\theta is dxdy\frac{dx}{dy}⁠.
What to take away
  1. Products of θ\theta with a trigonometric function need the product rule; look out for terms that cancel.
  2. Check every factor of dxdθ\frac{dx}{d\theta} for zeros, including a bare θ\theta⁠.
  3. Where both rates vanish, expect a cusp; where only dxdθ\frac{dx}{d\theta} vanishes, a vertical tangent.

Every fact used, and where it comes from

FactUsed inSource
Sum and product rulesSteps 1, 2Section 5.3, algebra of derivatives (Basics: derivative rules)
ddθsin⁡θ=cos⁡θ\frac{d}{d\theta}\sin\theta = \cos\theta⁠, ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\thetaSteps 1, 2Table 5.3
cos⁡θ=0  ⟺  θ=(2n+1)π2\cos\theta = 0 \iff \theta = (2n+1)\frac{\pi}{2}Steps 3, 5Class XI, Trigonometric Functions (Basics: trigonometric identities)
dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}⁠, dxdθ≠0\frac{dx}{d\theta} \neq 0Steps 3, 4Section 5.6 (Lesson: parametric differentiation)
Arc length of a circle: ∣a∣|a| times the angleStep 5Class XI, Trigonometric Functions (radian measure)
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