Class 12 Maths, Worked in Full Past papersGet updates
Chapter 5 · Continuity and Differentiability

Example 33: dydx\frac{dy}{dx} when x=a(θ+sin⁡θ)x=a(\theta+\sin\theta)⁠, y=a(1−cos⁡θ)y=a(1-\cos\theta)

ExamplesParametric differentiation · Section 5.6
The question

Find dydx\dfrac{dy}{dx}⁠, if x=a(θ+sin⁡θ)x = a(\theta + \sin\theta)⁠, y=a(1−cos⁡θ)y = a(1 - \cos\theta)⁠.

Exam answer

Here x=a(θ+sin⁡θ)x = a(\theta + \sin\theta) and y=a(1−cos⁡θ)y = a(1 - \cos\theta)⁠.

Differentiating w.r.t. θ\theta⁠,

dxdθ=a(1+cos⁡θ)dydθ=asin⁡θ\begin{aligned} \frac{dx}{d\theta} &= a(1 + \cos\theta) \\ \frac{dy}{d\theta} &= a\sin\theta \end{aligned} dydx=dy/dθdx/dθ=asin⁡θa(1+cos⁡θ)\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta} = \frac{a\sin\theta}{a(1 + \cos\theta)}

Using sin⁡θ=2sin⁡θ2cos⁡θ2\sin\theta = 2\sin\frac{\theta}{2}\cos\frac{\theta}{2} and 1+cos⁡θ=2cos⁡2θ21 + \cos\theta = 2\cos^2\frac{\theta}{2}⁠,

dydx=2sin⁡θ2cos⁡θ22cos⁡2θ2\frac{dy}{dx} = \frac{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}}{2\cos^2\frac{\theta}{2}}

∴ dydx=tan⁡θ2\therefore\ \dfrac{dy}{dx} = \tan\dfrac{\theta}{2} (θ≠(2n+1)π, n∈Z)(\theta \ne (2n + 1)\pi,\ n \in \Z)⁠.

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

The one idea this problem is built on

As in every parametric problem, the slope is the ratio of the two θ\theta-rates:

dydx=dy/dθdx/dθ,\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta},

wherever dxdθ≠0\frac{dx}{d\theta} \neq 0⁠. The ratio here is sin⁡θ1+cos⁡θ\frac{\sin\theta}{1+\cos\theta}⁠, and the half-angle formulas collapse it to the single value tan⁡θ2\tan\frac{\theta}{2}⁠.

Given, to find, and the plan
Given
x=a(θ+sin⁡θ)x = a(\theta + \sin\theta)⁠, y=a(1−cos⁡θ)y = a(1 - \cos\theta)⁠, with aa a nonzero constant and θ\theta the parameter.
To find
dydx\dfrac{dy}{dx}⁠.
Plan
Differentiate xx and yy with respect to θ\theta⁠; find where dxdθ=0\frac{dx}{d\theta} = 0⁠; divide; simplify with sin⁡θ=2sin⁡θ2cos⁡θ2\sin\theta = 2\sin\frac{\theta}{2}\cos\frac{\theta}{2} and 1+cos⁡θ=2cos⁡2θ21 + \cos\theta = 2\cos^2\frac{\theta}{2}⁠, checking that the factor we cancel is not zero. Finally look at the excluded points on a picture of the curve.

Basics you need

1Derivatives you need

ddθθ=1\frac{d}{d\theta}\theta = 1⁠, ddθsin⁡θ=cos⁡θ\frac{d}{d\theta}\sin\theta = \cos\theta⁠, ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\theta⁠, and the derivative of a constant is 00 (Table 5.3 and the sum rule). Basics: derivative rules

2The parametric formula (Section 5.6)

dydx=g′(θ)f′(θ)\frac{dy}{dx} = \frac{g'(\theta)}{f'(\theta)} when x=f(θ)x = f(\theta)⁠, y=g(θ)y = g(\theta) and f′(θ)≠0f'(\theta) \neq 0⁠. Lesson: parametric differentiation

3Half-angle formulas

From the double-angle formulas with θ=2⋅θ2\theta = 2\cdot\frac{\theta}{2}⁠:

sin⁡θ=2sin⁡θ2cos⁡θ2,1+cos⁡θ=2cos⁡2θ2.\begin{aligned} \sin\theta &= 2\sin\tfrac{\theta}{2}\cos\tfrac{\theta}{2}, \\ 1 + \cos\theta &= 2\cos^2\tfrac{\theta}{2}. \end{aligned}

The second comes from cos⁡θ=2cos⁡2θ2−1\cos\theta = 2\cos^2\frac{\theta}{2} - 1⁠. Both hold for every θ\theta⁠. Basics: trigonometric identities

4When is cos⁡θ=−1\cos\theta = -1⁠?

Exactly when θ\theta is an odd multiple of π\pi⁠: θ=(2n+1)π\theta = (2n+1)\pi⁠, n∈Zn \in \Z⁠. Then θ2=(2n+1)π2\frac{\theta}{2} = (2n+1)\frac{\pi}{2}⁠, where cos⁡θ2=0\cos\frac{\theta}{2} = 0⁠. Basics: trigonometric identities

Solution

  1. Differentiate xx with respect to θ\theta

    x=a(θ+sin⁡θ)x = a(\theta + \sin\theta) is a constant times a sum, so differentiate each term:

    dxdθ=a(1+cos⁡θ).\frac{dx}{d\theta} = a\left(1 + \cos\theta\right).
    The parametric formula needs both θ\theta-rates. The sum rule lets us differentiate θ\theta (giving 1) and sin⁡θ\sin\theta (giving cos⁡θ\cos\theta⁠) separately, and aa stays in front.
    Sum rule (u+v)′=u′+v′(u+v)' = u' + v' (Section 5.3). Basics: derivative rules
  2. Differentiate yy with respect to θ\theta

    dydθ=a(0−(−sin⁡θ))=asin⁡θ.\frac{dy}{d\theta} = a\left(0 - (-\sin\theta)\right) = a\sin\theta.
    The constant 1 has derivative 0, and −cos⁡θ-\cos\theta has derivative −(−sin⁡θ)=+sin⁡θ-(-\sin\theta) = +\sin\theta⁠. The two minus signs cancel, which is why the book writes simply asin⁡θa\sin\theta⁠.
    ddθcos⁡θ=−sin⁡θ\frac{d}{d\theta}\cos\theta = -\sin\theta (Table 5.3).
  3. Find where the formula may be used

    We need dxdθ≠0\frac{dx}{d\theta} \neq 0⁠. Since a≠0a \neq 0⁠,

    a(1+cos⁡θ)≠0  ⟺  cos⁡θ≠−1  ⟺  θ≠(2n+1)π.\begin{aligned} a(1 + \cos\theta) \neq 0 &\iff \cos\theta \neq -1 \\ &\iff \theta \neq (2n+1)\pi. \end{aligned}

    So from now on θ\theta is not an odd multiple of π\pi⁠.

    Dividing by zero is meaningless, so the excluded values must be found before dividing. We will see in Step 6 what the curve does at these values.
    Basic 4: cos⁡θ=−1\cos\theta = -1 only at odd multiples of π\pi⁠.
  4. Divide

    For θ≠(2n+1)π\theta \neq (2n+1)\pi⁠,

    dydx=dy/dθdx/dθ=asin⁡θa(1+cos⁡θ)=sin⁡θ1+cos⁡θ.\begin{aligned} \frac{dy}{dx} &= \frac{dy/d\theta}{dx/d\theta} = \frac{a\sin\theta}{a(1 + \cos\theta)} \\ &= \frac{\sin\theta}{1 + \cos\theta}. \end{aligned}
    The yy-rate goes on top. The factor aa cancels because a≠0a \neq 0⁠. This is already a correct answer; Step 5 simplifies it.
    Parametric formula, Section 5.6. Lesson: parametric differentiation
  5. Simplify with the half-angle formulas

    Rewrite top and bottom using Basic 3:

    sin⁡θ1+cos⁡θ=2sin⁡θ2cos⁡θ22cos⁡2θ2=sin⁡θ2cos⁡θ2=tan⁡θ2.\begin{aligned} \frac{\sin\theta}{1 + \cos\theta} &= \frac{2\sin\frac{\theta}{2}\cos\frac{\theta}{2}}{2\cos^2\frac{\theta}{2}} \\ &= \frac{\sin\frac{\theta}{2}}{\cos\frac{\theta}{2}} = \tan\frac{\theta}{2}. \end{aligned}

    Cancelling 2cos⁡θ22\cos\frac{\theta}{2} is allowed: by Step 3, θ≠(2n+1)π\theta \neq (2n+1)\pi⁠, so θ2≠(2n+1)π2\frac{\theta}{2} \neq (2n+1)\frac{\pi}{2} and cos⁡θ2≠0\cos\frac{\theta}{2} \neq 0⁠. Hence

    dydx=tan⁡θ2(θ≠(2n+1)π).\frac{dy}{dx} = \tan\frac{\theta}{2} \qquad (\theta \neq (2n+1)\pi).
    Both sin⁡θ\sin\theta and 1+cos⁡θ1 + \cos\theta contain the factor cos⁡θ2\cos\frac{\theta}{2} once we write them in half-angles. Spotting this common factor is the whole trick. Notice also that the condition for the original formula (Step 3) is exactly the condition for tan⁡θ2\tan\frac{\theta}{2} to be defined, so nothing is lost or gained by the simplification.
    tan⁡u=sin⁡ucos⁡u\tan u = \frac{\sin u}{\cos u}⁠, defined when cos⁡u≠0\cos u \neq 0⁠. Basics: trigonometric identities
  6. Picture the curve and the excluded points

    At θ=(2n+1)π\theta = (2n+1)\pi both rates are zero: dxdθ=a(1+cos⁡θ)=0\frac{dx}{d\theta} = a(1 + \cos\theta) = 0 and dydθ=asin⁡θ=0\frac{dy}{d\theta} = a\sin\theta = 0⁠. The point there is (a(2n+1)π, 2a)\big(a(2n+1)\pi,\ 2a\big)⁠. As θ\theta approaches π\pi from either side, tan⁡θ2\tan\frac{\theta}{2} grows without bound in size, so the curve comes into that point steeper and steeper, and leaves it the same way: the point is a sharp tip (a cusp), and dydx\frac{dy}{dx} does not exist there.

    x y O −aπ aπ a 2a θ = π/2 θ = −π/2 θ = 0 θ = −π θ = π tangent slope tan(θ/2): 1 at θ = π/2, −1 at θ = −π/2 θ = 0: slope tan 0 = 0, horizontal tangent θ = ±π: dx/dθ = dy/dθ = 0, a cusp
    The curve for a=1a = 1⁠, θ\theta from about −π−0.8-\pi - 0.8 to π+0.8\pi + 0.8⁠. At θ=0\theta = 0 it is at its lowest point with slope tan⁡0=0\tan 0 = 0⁠; at θ=±π2\theta = \pm\frac{\pi}{2}⁠, the points (±(π2+1),1)\big(\pm(\frac{\pi}{2}+1), 1\big)⁠, the slope is tan⁡(±π4)=±1\tan(\pm\frac{\pi}{4}) = \pm 1⁠; at θ=±π\theta = \pm\pi the curve has cusps, where both θ\theta-rates are zero.

    For −π<θ<π-\pi \lt \theta \lt \pi the answer has a neat meaning: the slope is tan⁡θ2\tan\frac{\theta}{2} with −π2<θ2<π2-\frac{\pi}{2} \lt \frac{\theta}{2} \lt \frac{\pi}{2}⁠, so the tangent makes the angle θ2\frac{\theta}{2} with the xx-axis.

    The figure shows why the condition of Step 3 matters: the excluded values are not a technicality but the sharp tips of the curve. (Putting θ=φ+π\theta = \varphi + \pi turns the equations into x=aπ+a(φ−sin⁡φ)x = a\pi + a(\varphi - \sin\varphi)⁠, y=2a−a(1−cos⁡φ)y = 2a - a(1 - \cos\varphi)⁠: this is the cycloid, the path of a point on the rim of a rolling wheel, shifted and turned upside down.)
    A line with angle of inclination α\alpha has slope tan⁡α\tan\alpha (Class XI, Straight Lines). Basics: slope at a point
Result dydx=sin⁡θ1+cos⁡θ=tan⁡θ2,\frac{dy}{dx} = \frac{\sin\theta}{1+\cos\theta} = \tan\frac{\theta}{2},

for every θ≠(2n+1)π\theta \neq (2n+1)\pi⁠, n∈Zn \in \Z⁠. At θ=(2n+1)π\theta = (2n+1)\pi the curve has a cusp and dydx\frac{dy}{dx} does not exist. (Book's answer: tan⁡θ2\tan\frac{\theta}{2}⁠.) As the book's Note says, dydx\frac{dy}{dx} is expressed in terms of the parameter only, without using xx and yy⁠.

Check it with numbers

Take a=2a = 2⁠, θ=1\theta = 1 (radian). The point is (2(1+sin⁡1), 2(1−cos⁡1))(2(1+\sin 1),\ 2(1-\cos 1))⁠, approximately (3.6829420, 0.9193954)(3.6829420,\ 0.9193954)⁠. Predicted slope: tan⁡0.5≈0.5463025\tan 0.5 \approx 0.5463025⁠, and sin⁡11+cos⁡1≈0.84147101.5403023≈0.5463025\frac{\sin 1}{1+\cos 1} \approx \frac{0.8414710}{1.5403023} \approx 0.5463025⁠, so the two forms agree.

Chord from θ=0.999\theta = 0.999 to θ=1.001\theta = 1.001⁠: the points are (3.6798605, 0.9177130)(3.6798605,\ 0.9177130) and (3.6860217, 0.9210789)(3.6860217,\ 0.9210789)⁠, so

ΔyΔx≈0.00336590.0061612≈0.54630,\frac{\Delta y}{\Delta x} \approx \frac{0.0033659}{0.0061612} \approx 0.54630,

agreeing with tan⁡0.5\tan 0.5 to five decimal places.

Common mistakes
  1. Sign slip in dydθ\frac{dy}{d\theta}⁠. ddθ(1−cos⁡θ)=+sin⁡θ\frac{d}{d\theta}(1 - \cos\theta) = +\sin\theta⁠. Writing −sin⁡θ-\sin\theta leads to −tan⁡θ2-\tan\frac{\theta}{2}⁠.
  2. Using the wrong half-angle formula. 1+cos⁡θ=2cos⁡2θ21 + \cos\theta = 2\cos^2\frac{\theta}{2}⁠, while 1−cos⁡θ=2sin⁡2θ21 - \cos\theta = 2\sin^2\frac{\theta}{2}⁠. Mixing them up gives cot⁡θ2\cot\frac{\theta}{2}⁠.
  3. Cancelling without a condition. cos⁡θ2\cos\frac{\theta}{2} may be cancelled only because it is not zero when θ≠(2n+1)π\theta \neq (2n+1)\pi⁠. State it.
  4. Assuming a slope exists everywhere. At θ=±π\theta = \pm\pi both rates vanish and the curve has a sharp tip: there is no tangent slope.
What to take away
  1. The parametric method gives sin⁡θ1+cos⁡θ\frac{\sin\theta}{1+\cos\theta} at once; the half-angle formulas then reduce it to tan⁡θ2\tan\frac{\theta}{2}⁠.
  2. sin⁡θ1+cos⁡θ=tan⁡θ2\frac{\sin\theta}{1+\cos\theta} = \tan\frac{\theta}{2} is worth remembering. The same half-angle simplification is needed again in Exercise 5.6, Question 6, where 1−cos⁡θ=2sin⁡2θ21 - \cos\theta = 2\sin^2\frac{\theta}{2} is the formula to use.
  3. When dxdθ\frac{dx}{d\theta} and dydθ\frac{dy}{d\theta} are both zero, expect something special on the curve, such as a cusp.

Every fact used, and where it comes from

FactUsed inSource
Sum rule; derivatives of θ\theta⁠, sin⁡θ\sin\theta⁠, cos⁡θ\cos\theta⁠, constantsSteps 1, 2Section 5.3, Table 5.3
dydx=g′(θ)f′(θ)\frac{dy}{dx} = \frac{g'(\theta)}{f'(\theta)}⁠, f′(θ)≠0f'(\theta) \neq 0Steps 3, 4Section 5.6 (Lesson: parametric differentiation)
cos⁡θ=−1  ⟺  θ=(2n+1)π\cos\theta = -1 \iff \theta = (2n+1)\piSteps 3, 5Class XI, Trigonometric Functions
sin⁡θ=2sin⁡θ2cos⁡θ2\sin\theta = 2\sin\frac{\theta}{2}\cos\frac{\theta}{2}⁠, 1+cos⁡θ=2cos⁡2θ21+\cos\theta = 2\cos^2\frac{\theta}{2}Step 5Double-angle formulas, Class XI (Basics: trigonometric identities)
Slope =tan⁡(angle of inclination)= \tan(\text{angle of inclination})Step 6Class XI, Straight Lines
dydx\frac{dy}{dx} in terms of the parameter onlyResultNote after Example 33, Section 5.6
Found an error, or want more?

Tell us if something on this page is wrong or unclear, or if you would like a fuller explanation, another method or a new feature. Send feedback on this problem →