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Chapter 5 · Continuity and Differentiability

Exercise 5.6 · Q7: dydx\frac{dy}{dx} when x=sin⁡3tcos⁡2tx=\frac{\sin^3t}{\sqrt{\cos2t}}⁠, y=cos⁡3tcos⁡2ty=\frac{\cos^3t}{\sqrt{\cos2t}}

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}⁠.

7. x=sin⁡3tcos⁡2tx = \dfrac{\sin^3 t}{\sqrt{\cos 2t}}⁠, y=cos⁡3tcos⁡2ty = \dfrac{\cos^3 t}{\sqrt{\cos 2t}}

Exam answer

Here x=sin⁡3t (cos⁡2t)−12x = \sin^3 t\,(\cos 2t)^{-\frac12}⁠, cos⁡2t>0\cos 2t > 0⁠. By the product and chain rules,

dxdt=3sin⁡2tcos⁡t (cos⁡2t)−12+sin⁡3tsin⁡2t (cos⁡2t)−32=Nx(cos⁡2t)32,\begin{aligned} \frac{dx}{dt} &= 3\sin^2 t\cos t\,(\cos 2t)^{-\frac12} \\ &\quad + \sin^3 t\sin 2t\,(\cos 2t)^{-\frac32} \\ &= \frac{N_x}{(\cos 2t)^{\frac32}}, \end{aligned}

where, using sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t⁠, cos⁡2t=1−2sin⁡2t\cos 2t = 1 - 2\sin^2 t and sin⁡3t=3sin⁡t−4sin⁡3t\sin 3t = 3\sin t - 4\sin^3 t⁠,

Nx=3sin⁡2tcos⁡tcos⁡2t+sin⁡3tsin⁡2t=sin⁡2tcos⁡t×(3cos⁡2t+2sin⁡2t)=sin⁡2tcos⁡t (3−4sin⁡2t)=sin⁡tcos⁡tsin⁡3t\begin{aligned} N_x &= 3\sin^2 t\cos t\cos 2t \\ &\quad + \sin^3 t\sin 2t \\ &= \sin^2 t\cos t \\ &\quad\times(3\cos 2t + 2\sin^2 t) \\ &= \sin^2 t\cos t\,(3 - 4\sin^2 t) \\ &= \sin t\cos t\sin 3t \end{aligned}

Similarly, y=cos⁡3t (cos⁡2t)−12y = \cos^3 t\,(\cos 2t)^{-\frac12} gives dydt=Ny(cos⁡2t)32\frac{dy}{dt} = \frac{N_y}{(\cos 2t)^{\frac32}}⁠, where, using cos⁡2t=2cos⁡2t−1\cos 2t = 2\cos^2 t - 1 and cos⁡3t=4cos⁡3t−3cos⁡t\cos 3t = 4\cos^3 t - 3\cos t⁠,

Ny=−3cos⁡2tsin⁡tcos⁡2t+cos⁡3tsin⁡2t=cos⁡2tsin⁡t×(2cos⁡2t−3cos⁡2t)=cos⁡2tsin⁡t (3−4cos⁡2t)=−sin⁡tcos⁡tcos⁡3t\begin{aligned} N_y &= -3\cos^2 t\sin t\cos 2t \\ &\quad + \cos^3 t\sin 2t \\ &= \cos^2 t\sin t \\ &\quad\times(2\cos^2 t - 3\cos 2t) \\ &= \cos^2 t\sin t\,(3 - 4\cos^2 t) \\ &= -\sin t\cos t\cos 3t \end{aligned} dydx=dy/dtdx/dt=NyNx=−sin⁡tcos⁡tcos⁡3tsin⁡tcos⁡tsin⁡3t\begin{aligned} \frac{dy}{dx} &= \frac{dy/dt}{dx/dt} = \frac{N_y}{N_x} \\ &= \frac{-\sin t\cos t\cos 3t}{\sin t\cos t\sin 3t} \end{aligned}

∴ dydx=−cot⁡3t\therefore\ \dfrac{dy}{dx} = -\cot 3t (t≠nπ)(t \ne n\pi)

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

The one idea this problem is built on

The method is the usual one, dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}⁠, but the two derivatives are messy. The key is to tidy each numerator with the triple-angle formulas

sin⁡3t=3sin⁡t−4sin⁡3t,cos⁡3t=4cos⁡3t−3cos⁡t.\begin{aligned} \sin 3t &= 3\sin t - 4\sin^3 t, \\ \cos 3t &= 4\cos^3 t - 3\cos t. \end{aligned}

Then dxdt\frac{dx}{dt} and dydt\frac{dy}{dt} share everything except sin⁡3t\sin 3t and −cos⁡3t-\cos 3t⁠, and the ratio is −cot⁡3t-\cot 3t⁠.

Given, to find, and the plan
Given
x=sin⁡3tcos⁡2tx = \frac{\sin^3 t}{\sqrt{\cos 2t}}⁠, y=cos⁡3tcos⁡2ty = \frac{\cos^3 t}{\sqrt{\cos 2t}}⁠. The square root must be real and the denominator nonzero, so cos⁡2t>0\cos 2t \gt 0⁠, that is tt lies in one of the intervals nπ−π4<t<nπ+π4n\pi - \frac{\pi}{4} \lt t \lt n\pi + \frac{\pi}{4}⁠, n∈Zn \in \Z⁠.
To find
dydx\dfrac{dy}{dx}⁠, without eliminating tt⁠.
Plan
Write each coordinate as a product with (cos⁡2t)−12(\cos 2t)^{-\frac12}⁠; differentiate with the product and chain rules; simplify each numerator with the double- and triple-angle formulas; find where dxdt=0\frac{dx}{dt} = 0⁠; divide; picture the curve.

Basics you need

1Product rule

(uv)′=u′v+uv′(uv)' = u'v + uv' (Section 5.3, algebra of derivatives). Basics: derivative rules

2Chain rule for powers

ddtun=nun−1dudt\frac{d}{dt}u^n = nu^{n-1}\frac{du}{dt}⁠. For example ddtsin⁡3t=3sin⁡2tcos⁡t\frac{d}{dt}\sin^3 t = 3\sin^2 t\cos t (outer u3u^3⁠, inner u=sin⁡tu = \sin t⁠), and

ddt(cos⁡2t)−12=−12(cos⁡2t)−32(−2sin⁡2t)=sin⁡2t (cos⁡2t)−32.\begin{aligned} \tfrac{d}{dt}(\cos 2t)^{-\frac12} &= -\tfrac12(\cos 2t)^{-\frac32}(-2\sin 2t) \\ &= \sin 2t\,(\cos 2t)^{-\frac32}. \end{aligned}

Here the chain rule is used twice: outer u−12u^{-\frac12} with u=cos⁡2tu = \cos 2t⁠, and inside it ddtcos⁡2t=−2sin⁡2t\frac{d}{dt}\cos 2t = -2\sin 2t⁠. Lesson: chain rule

3Double- and triple-angle formulas

sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t⁠, cos⁡2t=1−2sin⁡2t=2cos⁡2t−1\cos 2t = 1 - 2\sin^2 t = 2\cos^2 t - 1⁠, sin⁡3t=3sin⁡t−4sin⁡3t\sin 3t = 3\sin t - 4\sin^3 t⁠, cos⁡3t=4cos⁡3t−3cos⁡t\cos 3t = 4\cos^3 t - 3\cos t (Class XI). Basics: trigonometric identities

4The parametric formula (Section 5.6)

dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}⁠, provided dxdt≠0\frac{dx}{dt} \neq 0⁠. Lesson: parametric differentiation

Solution

  1. Differentiate xx⁠: product rule and chain rule

    Write x=sin⁡3t⋅(cos⁡2t)−12x = \sin^3 t\cdot(\cos 2t)^{-\frac12}⁠. By the product rule and Basic 2,

    dxdt=3sin⁡2tcos⁡t (cos⁡2t)−12+sin⁡3tsin⁡2t (cos⁡2t)−32.\begin{aligned} \frac{dx}{dt} &= 3\sin^2 t\cos t\,(\cos 2t)^{-\frac12} \\ &\quad + \sin^3 t\sin 2t\,(\cos 2t)^{-\frac32}. \end{aligned}

    Put both terms over (cos⁡2t)32(\cos 2t)^{\frac32} (multiply the first by cos⁡2tcos⁡2t\frac{\cos 2t}{\cos 2t}⁠):

    dxdt=Nx(cos⁡2t)32,\frac{dx}{dt} = \frac{N_x}{(\cos 2t)^{\frac32}},

    where

    Nx=3sin⁡2tcos⁡tcos⁡2t+sin⁡3tsin⁡2t.N_x = 3\sin^2 t\cos t\cos 2t + \sin^3 t\sin 2t.
    Writing 1cos⁡2t\frac{1}{\sqrt{\cos 2t}} as the power (cos⁡2t)−12(\cos 2t)^{-\frac12} turns a quotient into a product, which is easier to differentiate. A common denominator then lets us study the numerator NxN_x on its own. Since cos⁡2t>0\cos 2t \gt 0⁠, the denominator (cos⁡2t)32(\cos 2t)^{\frac32} is a positive number.
    Product rule (Section 5.3); chain rule (Theorem 4, Section 5.3.1). Lesson: chain rule
  2. Simplify the numerator NxN_x

    Use sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t in the second term and take out sin⁡2tcos⁡t\sin^2 t\cos t⁠:

    Nx=3sin⁡2tcos⁡tcos⁡2t+2sin⁡4tcos⁡t=sin⁡2tcos⁡t (3cos⁡2t+2sin⁡2t).\begin{aligned} N_x &= 3\sin^2 t\cos t\cos 2t + 2\sin^4 t\cos t \\ &= \sin^2 t\cos t\,(3\cos 2t + 2\sin^2 t). \end{aligned}

    Now 3cos⁡2t=3−6sin⁡2t3\cos 2t = 3 - 6\sin^2 t⁠, so the bracket is 3−4sin⁡2t3 - 4\sin^2 t⁠, and

    Nx=sin⁡tcos⁡t (3sin⁡t−4sin⁡3t)=sin⁡tcos⁡tsin⁡3t.\begin{aligned} N_x &= \sin t\cos t\,(3\sin t - 4\sin^3 t) \\ &= \sin t\cos t\sin 3t. \end{aligned}

    Therefore

    dxdt=sin⁡tcos⁡tsin⁡3t(cos⁡2t)32.\frac{dx}{dt} = \frac{\sin t\cos t\sin 3t}{(\cos 2t)^{\frac32}}.
    The aim is a product of simple factors, so that we can see where dxdt\frac{dx}{dt} vanishes and what cancels later. Writing everything in sin⁡t\sin t turns the bracket into 3−4sin⁡2t3 - 4\sin^2 t⁠; one more sin⁡t\sin t makes it 3sin⁡t−4sin⁡3t3\sin t - 4\sin^3 t⁠, which is exactly sin⁡3t\sin 3t⁠.
    cos⁡2t=1−2sin⁡2t\cos 2t = 1 - 2\sin^2 t and sin⁡3t=3sin⁡t−4sin⁡3t\sin 3t = 3\sin t - 4\sin^3 t (Basic 3). Basics: trigonometric identities
  3. Differentiate yy and simplify the same way

    Write y=cos⁡3t⋅(cos⁡2t)−12y = \cos^3 t\cdot(\cos 2t)^{-\frac12}⁠. With ddtcos⁡3t=−3cos⁡2tsin⁡t\frac{d}{dt}\cos^3 t = -3\cos^2 t\sin t⁠,

    dydt=Ny(cos⁡2t)32,\frac{dy}{dt} = \frac{N_y}{(\cos 2t)^{\frac32}},

    where

    Ny=−3cos⁡2tsin⁡tcos⁡2t+cos⁡3tsin⁡2t.N_y = -3\cos^2 t\sin t\cos 2t + \cos^3 t\sin 2t.

    Use sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t⁠, take out cos⁡2tsin⁡t\cos^2 t\sin t⁠, and use 3cos⁡2t=6cos⁡2t−33\cos 2t = 6\cos^2 t - 3⁠:

    Ny=cos⁡2tsin⁡t (−3cos⁡2t+2cos⁡2t)=cos⁡2tsin⁡t (3−4cos⁡2t)=−sin⁡tcos⁡t (4cos⁡3t−3cos⁡t)=−sin⁡tcos⁡tcos⁡3t.\begin{aligned} N_y &= \cos^2 t\sin t\,(-3\cos 2t + 2\cos^2 t) \\ &= \cos^2 t\sin t\,(3 - 4\cos^2 t) \\ &= -\sin t\cos t\,(4\cos^3 t - 3\cos t) \\ &= -\sin t\cos t\cos 3t. \end{aligned}

    Therefore

    dydt=−sin⁡tcos⁡tcos⁡3t(cos⁡2t)32.\frac{dy}{dt} = \frac{-\sin t\cos t\cos 3t}{(\cos 2t)^{\frac32}}.
    Exactly the same plan as for xx⁠, with the roles of sine and cosine swapped. This time the bracket is written in cos⁡t\cos t⁠, and 4cos⁡3t−3cos⁡t4\cos^3 t - 3\cos t is cos⁡3t\cos 3t⁠; the minus sign comes from taking −1-1 out of 3−4cos⁡2t3 - 4\cos^2 t⁠.
    ddtcos⁡3t=3cos⁡2t⋅(−sin⁡t)\frac{d}{dt}\cos^3 t = 3\cos^2 t\cdot(-\sin t) (chain rule); cos⁡2t=2cos⁡2t−1\cos 2t = 2\cos^2 t - 1⁠; cos⁡3t=4cos⁡3t−3cos⁡t\cos 3t = 4\cos^3 t - 3\cos t⁠.
  4. Find where dxdt=0\frac{dx}{dt} = 0

    Remember that tt lies where cos⁡2t>0\cos 2t \gt 0⁠. The derivative dxdt\frac{dx}{dt} is zero exactly when sin⁡t\sin t⁠, cos⁡t\cos t or sin⁡3t\sin 3t is zero. Check each against the domain:

    • cos⁡t=0\cos t = 0 would give cos⁡2t=2cos⁡2t−1=−1<0\cos 2t = 2\cos^2 t - 1 = -1 \lt 0⁠: never in the domain.
    • sin⁡t=0\sin t = 0 at t=nπt = n\pi⁠, where cos⁡2t=1>0\cos 2t = 1 \gt 0⁠: these are in the domain.
    • sin⁡3t=0\sin 3t = 0 at t=kπ3t = \frac{k\pi}{3}⁠, k∈Zk \in \Z⁠. Then cos⁡2t=cos⁡2kπ3\cos 2t = \cos\frac{2k\pi}{3}⁠, which is 11 when kk is a multiple of 3 and −12-\frac12 otherwise. So only t=nπt = n\pi again is in the domain.

    So dxdt≠0\frac{dx}{dt} \neq 0 at every tt of the domain except t=nπt = n\pi⁠.

    The formula divides by dxdt\frac{dx}{dt}⁠, so we must know exactly where it vanishes, and only inside the domain, because outside it there is no curve at all. Checking each factor against cos⁡2t>0\cos 2t \gt 0 shows that the only trouble is at t=nπt = n\pi⁠.
    sin⁡3t=0  ⟺  3t=kπ\sin 3t = 0 \iff 3t = k\pi⁠; cos⁡2π3=cos⁡4π3=−12\cos\frac{2\pi}{3} = \cos\frac{4\pi}{3} = -\frac12⁠. Basics: trigonometric identities
  5. Divide

    For tt in the domain with t≠nπt \neq n\pi⁠,

    dydx=dy/dtdx/dt=−sin⁡tcos⁡tcos⁡3tsin⁡tcos⁡tsin⁡3t=−cos⁡3tsin⁡3t=−cot⁡3t.\begin{aligned} \frac{dy}{dx} &= \frac{dy/dt}{dx/dt} = \frac{-\sin t\cos t\cos 3t}{\sin t\cos t\sin 3t} \\ &= -\frac{\cos 3t}{\sin 3t} = -\cot 3t. \end{aligned}
    The common denominator (cos⁡2t)32(\cos 2t)^{\frac32} cancels at once, and the common factor sin⁡tcos⁡t\sin t\cos t is not zero by Step 4. What remains is −cos⁡3tsin⁡3t-\frac{\cos 3t}{\sin 3t}⁠, which is −cot⁡3t-\cot 3t⁠; it is defined because sin⁡3t≠0\sin 3t \neq 0 (Step 4).
    Parametric formula, Section 5.6. Lesson: parametric differentiation
  6. Picture the curve and the points t=nπt = n\pi

    At t=nπt = n\pi both dxdt\frac{dx}{dt} and dydt\frac{dy}{dt} are zero (both contain sin⁡t\sin t⁠). The point is (0,1)(0, 1) for even nn and (0,−1)(0, -1) for odd nn⁠. As tt increases through 00⁠, xx goes from negative to positive, while the slope −cot⁡3t-\cot 3t is very large and positive just before t=0t = 0 and very large and negative just after: the curve rises steeply into (0,1)(0, 1) and falls steeply out of it, a sharp tip (a cusp) where dydx\frac{dy}{dx} does not exist.

    The slope is 00 where cos⁡3t=0\cos 3t = 0 inside the domain. On the upper branch this happens at t=±π6t = \pm\frac{\pi}{6} (there cos⁡2t=12>0\cos 2t = \frac12 \gt 0⁠): two low points (±28, 368)≈(±0.18, 0.92)\big(\pm\frac{\sqrt2}{8},\ \frac{3\sqrt6}{8}\big) \approx (\pm 0.18,\ 0.92)⁠, just below the cusp. On the lower branch it happens at t=π±π6t = \pi \pm \frac{\pi}{6}⁠, and since replacing tt by t+πt + \pi changes (x,y)(x, y) into (−x,−y)(-x, -y)⁠, these are the two high points (±28, −368)\big(\pm\frac{\sqrt2}{8},\ -\frac{3\sqrt6}{8}\big)⁠, just above the cusp (0,−1)(0, -1)⁠.

    x y O −2 −1 1 2 −2 −1 1 2 t = 2π/9 t = 0 t = π upper branch: −π/4 < t < π/4; lower: 3π/4 < t < 5π/4 t = 2π/9: slope −cot(2π/3) = 1/√3 t = nπ: dx/dt = dy/dt = 0, cusps (0, ±1) the lines y = x and y = −x, approached far out
    The curve (equal scales). For −π4<t<π4-\frac{\pi}{4} \lt t \lt \frac{\pi}{4} we get the upper branch, with its cusp at (0,1)(0, 1) when t=0t = 0⁠; for 3π4<t<5π4\frac{3\pi}{4} \lt t \lt \frac{5\pi}{4} the lower branch, with its cusp at (0,−1)(0, -1)⁠. As tt approaches the ends of these intervals the points run off along the dashed lines y=±xy = \pm x⁠. At t=2π9t = \frac{2\pi}{9} the slope is −cot⁡2π3=13-\cot\frac{2\pi}{3} = \frac{1}{\sqrt3}⁠.
    The picture shows what the restriction t≠nπt \neq n\pi means: those are exactly the two cusps. Other values of nn give nothing new, because replacing tt by t+2πt + 2\pi does not change xx or yy⁠, so all the curve is traced by the two intervals in the caption.
    A cusp is a sharp tip of a curve; no single tangent line fits there. Basics: slope at a point
Result dydx=−cot⁡3t,\frac{dy}{dx} = -\cot 3t,

for every tt with cos⁡2t>0\cos 2t \gt 0 and t≠nπt \neq n\pi⁠, n∈Zn \in \Z⁠. At t=nπt = n\pi the curve has a cusp. (Textbook answer: −cot⁡3t-\cot 3t⁠.)

Check it with numbers

A short chord. At t=0.3t = 0.3 (where cos⁡0.6>0\cos 0.6 \gt 0⁠) the point is (0.0284084, 0.9597405)(0.0284084,\ 0.9597405) and the predicted slope is −cot⁡0.9≈−0.7935511-\cot 0.9 \approx -0.7935511⁠. The points at t=0.299t = 0.299 and t=0.301t = 0.301 are (0.028114504, 0.959974375)(0.028114504,\ 0.959974375) and (0.028704397, 0.959506269)(0.028704397,\ 0.959506269)⁠, so

ΔyΔx=−0.0004681060.000589893≈−0.79354,\frac{\Delta y}{\Delta x} = \frac{-0.000468106}{0.000589893} \approx -0.79354,

which differs from −cot⁡0.9-\cot 0.9 by only about 0.000010.00001 (the chord is not quite the tangent, and here the slope changes quickly with tt⁠).

Symmetry. Replacing tt by −t-t changes xx into −x-x and leaves yy alone, so the curve is symmetric about the yy-axis and the slope must change sign. It does: −cot⁡(−3t)=cot⁡3t-\cot(-3t) = \cot 3t⁠.

Common mistakes
  1. Forgetting the inner derivative of cos⁡2t\cos 2t⁠. ddt(cos⁡2t)−12\frac{d}{dt}(\cos 2t)^{-\frac12} needs −12(cos⁡2t)−32-\frac12(\cos 2t)^{-\frac32} times −2sin⁡2t-2\sin 2t⁠.
  2. Not recognising sin⁡3t\sin 3t and cos⁡3t\cos 3t⁠. Without the triple-angle formulas the answer stays as a long fraction; it is correct, but the book's −cot⁡3t-\cot 3t is hidden in it.
  3. Ignoring the domain. xx and yy exist only where cos⁡2t>0\cos 2t \gt 0⁠; the zeros of cos⁡t\cos t and most zeros of sin⁡3t\sin 3t lie outside it.
  4. Missing the cusps. At t=nπt = n\pi both rates vanish and the formula does not apply.
What to take away
  1. Turn quotients with roots into products with negative fractional powers, then use the product and chain rules.
  2. Bring each derivative to a common denominator and factorise the numerator; recognise 3sin⁡t−4sin⁡3t=sin⁡3t3\sin t - 4\sin^3 t = \sin 3t and 4cos⁡3t−3cos⁡t=cos⁡3t4\cos^3 t - 3\cos t = \cos 3t⁠.
  3. Look for the zeros of dxdt\frac{dx}{dt} inside the domain only.

Every fact used, and where it comes from

FactUsed inSource
Product rule (uv)′=u′v+uv′(uv)' = u'v + uv'Steps 1, 3Section 5.3, algebra of derivatives (Basics: derivative rules)
Chain rule; ddtun=nun−1dudt\frac{d}{dt}u^n = nu^{n-1}\frac{du}{dt}Steps 1, 3Theorem 4, Section 5.3.1; Table 5.3 (Lesson: chain rule)
sin⁡2t=2sin⁡tcos⁡t\sin 2t = 2\sin t\cos t⁠, cos⁡2t=1−2sin⁡2t=2cos⁡2t−1\cos 2t = 1 - 2\sin^2 t = 2\cos^2 t - 1Steps 2, 3, 4Class XI, double-angle formulas (Basics: trigonometric identities)
sin⁡3t=3sin⁡t−4sin⁡3t\sin 3t = 3\sin t - 4\sin^3 t⁠, cos⁡3t=4cos⁡3t−3cos⁡t\cos 3t = 4\cos^3 t - 3\cos tSteps 2, 3Class XI, triple-angle formulas
dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}⁠, dxdt≠0\frac{dx}{dt} \neq 0Steps 4, 5Section 5.6 (Lesson: parametric differentiation)
cot⁡u=cos⁡usin⁡u\cot u = \frac{\cos u}{\sin u}Step 5Class XI, Trigonometric Functions
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