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Chapter 5 · Continuity and Differentiability

Exercise 5.6 · Q11: Show dydx=−yx\frac{dy}{dx}=-\frac yx for x=asin⁡−1tx=\sqrt{a^{\sin^{-1}t}}⁠, y=acos⁡−1ty=\sqrt{a^{\cos^{-1}t}}

Exercise 5.6Parametric differentiation · Section 5.6
The question

11. If x=asin⁡−1tx = \sqrt{a^{\sin^{-1}t}}⁠, y=acos⁡−1ty = \sqrt{a^{\cos^{-1}t}}⁠, show that dydx=−yx\dfrac{dy}{dx} = -\dfrac{y}{x}⁠.

Exam answer

Here x=a12sin⁡−1tx = a^{\frac12\sin^{-1}t}⁠, y=a12cos⁡−1ty = a^{\frac12\cos^{-1}t} (a>0a > 0⁠, a≠1a \ne 1⁠, −1<t<1-1 \lt t \lt 1⁠). By the chain rule,

dxdt=a12sin⁡−1tlog⁡a⋅121−t2=xlog⁡a21−t2,dydt=a12cos⁡−1tlog⁡a⋅−121−t2=−ylog⁡a21−t2\begin{aligned} \frac{dx}{dt} &= a^{\frac12\sin^{-1}t}\log a\cdot\frac{1}{2\sqrt{1 - t^2}} \\ &= \frac{x\log a}{2\sqrt{1 - t^2}}, \\ \frac{dy}{dt} &= a^{\frac12\cos^{-1}t}\log a\cdot\frac{-1}{2\sqrt{1 - t^2}} \\ &= -\frac{y\log a}{2\sqrt{1 - t^2}} \end{aligned} dydx=dy/dtdx/dt=−ylog⁡a21−t2⋅21−t2xlog⁡a\begin{aligned} \frac{dy}{dx} &= \frac{dy/dt}{dx/dt} \\ &= -\frac{y\log a}{2\sqrt{1 - t^2}}\cdot\frac{2\sqrt{1 - t^2}}{x\log a} \end{aligned}

∴ dydx=−yx\therefore\ \dfrac{dy}{dx} = -\dfrac{y}{x}⁠. Hence proved.

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

The one idea this problem is built on

Treat tt as a parameter and use dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}⁠. Each coordinate is an exponential, x=a12sin⁡−1tx = a^{\frac12\sin^{-1}t}⁠, so its derivative is itself times log⁡a\log a times the derivative of the exponent. Because sin⁡−1t\sin^{-1}t and cos⁡−1t\cos^{-1}t have derivatives that differ only in sign, the two rates are x⋅kx\cdot k and −y⋅k-y\cdot k with the same kk⁠, and the ratio is −yx-\frac{y}{x}⁠.

Given, to find, and the plan
Given
x=asin⁡−1tx = \sqrt{a^{\sin^{-1}t}}⁠, y=acos⁡−1ty = \sqrt{a^{\cos^{-1}t}}⁠. For a power with a real exponent the base must be positive, so a>0a \gt 0⁠; and sin⁡−1t\sin^{-1}t⁠, cos⁡−1t\cos^{-1}t need −1≤t≤1-1 \leq t \leq 1⁠. We also need a≠1a \neq 1⁠: if a=1a = 1⁠, then x=y=1x = y = 1 for every tt⁠, a single point with no slope.
To show
dydx=−yx\dfrac{dy}{dx} = -\dfrac{y}{x}⁠.
Plan
Rewrite xx and yy as powers of aa⁠; differentiate each with respect to tt by the chain rule; check that dxdt≠0\frac{dx}{dt} \neq 0 for −1<t<1-1 \lt t \lt 1⁠; divide.

Basics you need

1Square root of a power

For a>0a \gt 0⁠, am=(am)12=am2\sqrt{a^m} = (a^m)^{\frac12} = a^{\frac{m}{2}}⁠. Basics: exponentials and logarithms

2Derivative of aua^u

dduau=aulog⁡a\frac{d}{du}a^u = a^u\log a for a positive constant aa (Example 28). With the chain rule, ddtau=aulog⁡a⋅dudt\frac{d}{dt}a^{u} = a^{u}\log a\cdot\frac{du}{dt}⁠. Lesson: exponential and logarithmic functions

3Derivatives of sin⁡−1\sin^{-1} and cos⁡−1\cos^{-1}

For −1<t<1-1 \lt t \lt 1⁠:

ddtsin⁡−1t=11−t2,ddtcos⁡−1t=−11−t2.\begin{aligned} \tfrac{d}{dt}\sin^{-1}t &= \tfrac{1}{\sqrt{1 - t^2}}, \\ \tfrac{d}{dt}\cos^{-1}t &= -\tfrac{1}{\sqrt{1 - t^2}}. \end{aligned}

(Section 5.3.3: Example 24 and the table after it.) At t=±1t = \pm1 these derivatives do not exist. Lesson: derivatives of inverse trig functions

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. Rewrite xx and yy as powers of aa

    By Basic 1 (since a>0a \gt 0⁠),

    x=a12sin⁡−1t,y=a12cos⁡−1t.x = a^{\frac12\sin^{-1}t}, \qquad y = a^{\frac12\cos^{-1}t}.
    A square root of a power is awkward to differentiate; a single power of aa is easy, because we know the derivative of aua^u⁠. Note that x>0x \gt 0 and y>0y \gt 0⁠, since a power of a positive number is positive.
    (am)n=amn(a^m)^n = a^{mn} for a>0a \gt 0⁠. Basics: exponentials and logarithms
  2. Differentiate xx with respect to tt

    Chain rule with outer function aua^u and inner function u=12sin⁡−1tu = \frac12\sin^{-1}t⁠, for −1<t<1-1 \lt t \lt 1⁠:

    dxdt=a12sin⁡−1t⋅log⁡a⋅121−t2=xlog⁡a21−t2.\begin{aligned} \frac{dx}{dt} &= a^{\frac12\sin^{-1}t}\cdot\log a\cdot\frac{1}{2\sqrt{1 - t^2}} \\ &= \frac{x\log a}{2\sqrt{1 - t^2}}. \end{aligned}
    The outer function aua^u differentiates to aulog⁡aa^u\log a (Basic 2), evaluated at the inner function; that is xlog⁡ax\log a⁠. The inner function 12sin⁡−1t\frac12\sin^{-1}t differentiates to 12⋅11−t2\frac12\cdot\frac{1}{\sqrt{1 - t^2}} (Basic 3). We must keep tt strictly between −1-1 and 11⁠, where this exists.
    Chain rule (Theorem 4, Section 5.3.1); Example 28; Section 5.3.3. Lesson: chain rule
  3. Differentiate yy with respect to tt

    Same method, inner function u=12cos⁡−1tu = \frac12\cos^{-1}t⁠:

    dydt=a12cos⁡−1t⋅log⁡a⋅−121−t2=−ylog⁡a21−t2.\begin{aligned} \frac{dy}{dt} &= a^{\frac12\cos^{-1}t}\cdot\log a\cdot\frac{-1}{2\sqrt{1 - t^2}} \\ &= -\frac{y\log a}{2\sqrt{1 - t^2}}. \end{aligned}
    Everything is the same as in Step 2 except the sign of the inner derivative, because ddtcos⁡−1t=−11−t2\frac{d}{dt}\cos^{-1}t = -\frac{1}{\sqrt{1 - t^2}}⁠.
    Basic 3, second line.
  4. Check that the formula may be used

    For −1<t<1-1 \lt t \lt 1⁠: x>0x \gt 0 (Step 1), 1−t2>0\sqrt{1 - t^2} \gt 0⁠, and log⁡a≠0\log a \neq 0 because a≠1a \neq 1⁠. So

    dxdt=xlog⁡a21−t2≠0.\frac{dx}{dt} = \frac{x\log a}{2\sqrt{1 - t^2}} \neq 0.
    The formula divides by dxdt\frac{dx}{dt}⁠, so we must be sure it is never zero. Each factor is nonzero, so the product is nonzero. This is where the condition a≠1a \neq 1 is really used: log⁡1=0\log 1 = 0⁠.
    log⁡a=0  ⟺  a=1\log a = 0 \iff a = 1⁠. Basics: exponentials and logarithms
  5. Divide

    For −1<t<1-1 \lt t \lt 1⁠,

    dydx=dy/dtdx/dt=−ylog⁡a21−t2xlog⁡a21−t2=−yx.\frac{dy}{dx} = \frac{dy/dt}{dx/dt} = \frac{-\dfrac{y\log a}{2\sqrt{1 - t^2}}}{\dfrac{x\log a}{2\sqrt{1 - t^2}}} = -\frac{y}{x}.

    The common factor log⁡a21−t2\frac{\log a}{2\sqrt{1 - t^2}} is not zero (Step 4), so it cancels. This is what we had to show.

    The two rates are the same expression multiplied by xx and by −y-y⁠, so their ratio is −yx-\frac{y}{x}⁠. Unlike Exercises 1 to 10, the required answer is in terms of xx and yy⁠, and since x>0x \gt 0 it is always defined.
    Parametric formula, Section 5.6. Lesson: parametric differentiation
  6. Picture the curve

    As tt runs from −1-1 to 11⁠, sin⁡−1t\sin^{-1}t runs from −π2-\frac{\pi}{2} to π2\frac{\pi}{2} and cos⁡−1t\cos^{-1}t from π\pi down to 00⁠, so for a>1a \gt 1 the point moves from (a−π4,aπ2)\big(a^{-\frac{\pi}{4}}, a^{\frac{\pi}{2}}\big) down to (aπ4,1)\big(a^{\frac{\pi}{4}}, 1\big)⁠. At the two ends the derivatives of sin⁡−1t\sin^{-1}t and cos⁡−1t\cos^{-1}t do not exist, so we have shown dydx=−yx\frac{dy}{dx} = -\frac{y}{x} at every point except the two end points.

    x y O 1 2 3 1 2 3 t = 1/√2 t = 0 t = −1 t = 1 the curve for a = 2, t from −1 to 1 t = 1/√2: x = y, so the slope −y/x is −1 the whole hyperbola xy = 2^(π/4)
    The curve for a=2a = 2 (equal scales): an arc of the dashed curve xy=2π4xy = 2^{\frac{\pi}{4}}⁠, from t=−1t = -1 to t=1t = 1⁠. At t=0t = 0 the point is (1,2π4)\big(1, 2^{\frac{\pi}{4}}\big)⁠; at t=12t = \frac{1}{\sqrt2}⁠, where sin⁡−1t=cos⁡−1t=π4\sin^{-1}t = \cos^{-1}t = \frac{\pi}{4}⁠, it is (2π8,2π8)\big(2^{\frac{\pi}{8}}, 2^{\frac{\pi}{8}}\big) and the slope is −yx=−1-\frac{y}{x} = -1⁠.
    The picture shows a piece of a rectangular hyperbola xy=constantxy = \text{constant}⁠, whose slope is always −yx-\frac{y}{x}⁠. The check below explains why the product xyxy is constant.
    Principal ranges: sin⁡−1t∈[−π2,π2]\sin^{-1}t \in [-\frac{\pi}{2}, \frac{\pi}{2}]⁠, cos⁡−1t∈[0,π]\cos^{-1}t \in [0, \pi] (Chapter 2, Section 2.2).
Result dydx=−yx,\frac{dy}{dx} = -\frac{y}{x},

at every point with −1<t<1-1 \lt t \lt 1 (where a>0a \gt 0⁠, a≠1a \neq 1⁠), as was to be shown.

Check it with numbers

A short chord. Take a=2a = 2⁠, t=0.5t = 0.5⁠: the point is (1.1989732, 1.4375367)(1.1989732,\ 1.4375367) and the predicted slope is −yx≈−1.1989732-\frac{y}{x} \approx -1.1989732⁠. The points at t=0.499t = 0.499 and t=0.501t = 0.501 are (1.198493621, 1.438111897)(1.198493621,\ 1.438111897) and (1.199453252, 1.436961325)(1.199453252,\ 1.436961325)⁠, so

ΔyΔx=−0.0011505720.000959632≈−1.19897.\frac{\Delta y}{\Delta x} = \frac{-0.001150572}{0.000959632} \approx -1.19897.

A second route (eliminating tt⁠, only as a check). Let α=sin⁡−1t\alpha = \sin^{-1}t⁠, so −π2≤α≤π2-\frac{\pi}{2} \leq \alpha \leq \frac{\pi}{2} and sin⁡α=t\sin\alpha = t⁠. Then π2−α\frac{\pi}{2} - \alpha lies in [0,π][0, \pi]⁠, the principal range of cos⁡−1\cos^{-1}⁠, and cos⁡(π2−α)=sin⁡α=t\cos(\frac{\pi}{2} - \alpha) = \sin\alpha = t⁠, so cos⁡−1t=π2−α\cos^{-1}t = \frac{\pi}{2} - \alpha⁠. Hence sin⁡−1t+cos⁡−1t=π2\sin^{-1}t + \cos^{-1}t = \frac{\pi}{2} and

xy=a12(sin⁡−1t+cos⁡−1t)=aπ4,xy = a^{\frac12(\sin^{-1}t + \cos^{-1}t)} = a^{\frac{\pi}{4}},

a constant. Differentiating xy=aπ4xy = a^{\frac{\pi}{4}} with respect to xx by the product rule, y+xdydx=0y + x\frac{dy}{dx} = 0⁠, so dydx=−yx\frac{dy}{dx} = -\frac{y}{x}⁠. The same answer. (At t=0.5t = 0.5 with a=2a = 2⁠: xy≈1.7235679xy \approx 1.7235679⁠, which is 2π42^{\frac{\pi}{4}}⁠.)

Common mistakes
  1. Treating aua^u like unu^n⁠. The variable is in the exponent: dduau=aulog⁡a\frac{d}{du}a^u = a^u\log a⁠, not uau−1ua^{u-1}⁠.
  2. Forgetting the 12\frac12⁠. The square root halves the exponent; the 12\frac12 appears in both rates and cancels, but it must be there.
  3. Sign of ddtcos⁡−1t\frac{d}{dt}\cos^{-1}t⁠. It is −11−t2-\frac{1}{\sqrt{1 - t^2}}⁠; this minus sign is the minus sign in the answer.
  4. Ignoring the conditions. a>0a \gt 0 for the powers, a≠1a \neq 1 so that dxdt≠0\frac{dx}{dt} \neq 0⁠, and −1<t<1-1 \lt t \lt 1 for the derivatives of sin⁡−1\sin^{-1} and cos⁡−1\cos^{-1}⁠.
What to take away
  1. Rewrite roots of powers as single powers before differentiating.
  2. ddtau=aulog⁡a dudt\frac{d}{dt}a^{u} = a^{u}\log a\,\frac{du}{dt}⁠: the function reappears in its own derivative, which is why the answer can be written with xx and yy⁠.
  3. sin⁡−1t+cos⁡−1t=π2\sin^{-1}t + \cos^{-1}t = \frac{\pi}{2} explains the result: xyxy is constant, so the curve is part of a rectangular hyperbola.

Every fact used, and where it comes from

FactUsed inSource
am=am2\sqrt{a^m} = a^{\frac{m}{2}} for a>0a \gt 0⁠; log⁡a=0  ⟺  a=1\log a = 0 \iff a = 1Steps 1, 4Section 5.4 (Basics: exponentials and logarithms)
dduau=aulog⁡a\frac{d}{du}a^u = a^u\log a⁠, a>0a \gt 0Steps 2, 3Example 28, Section 5.5 (Lesson: exponential and logarithmic functions)
Chain ruleSteps 2, 3Theorem 4, Section 5.3.1 (Lesson: chain rule)
ddtsin⁡−1t=11−t2\frac{d}{dt}\sin^{-1}t = \frac{1}{\sqrt{1 - t^2}}⁠, ddtcos⁡−1t=−11−t2\frac{d}{dt}\cos^{-1}t = -\frac{1}{\sqrt{1 - t^2}} on (−1,1)(-1, 1)Steps 2, 3Example 24 and the table in Section 5.3.3 (Lesson: derivatives of inverse trig functions)
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)
Principal ranges of sin⁡−1\sin^{-1} and cos⁡−1\cos^{-1}Step 6, checkChapter 2, Section 2.2
cos⁡(π2−α)=sin⁡α\cos(\frac{\pi}{2} - \alpha) = \sin\alpha⁠; product ruleCheckClass XI, Trigonometric Functions; Section 5.3
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