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Question: How do you find the arc length of the cardioid \(r=1+\cos \theta \) from \(0\) to \(2\pi \) ?...

How do you find the arc length of the cardioid r=1+cosθr=1+\cos \theta from 00 to 2π2\pi ?

Explanation

Solution

We have been given the equation of a cardioid whose arc length we have to find in a fixed interval. We shall use the formula of arc length as L=abr2+(drdθ)2.dθL=\int\limits_{a}^{b}{\sqrt{{{r}^{2}}+{{\left( \dfrac{dr}{d\theta } \right)}^{2}}}.d\theta }. Thus, to apply this formula, we will first find the derivative of the given function and then substitute it in the formula of arc length to integrate it within the provided interval.

Complete step by step solution:
Given that r=1+cosθr=1+\cos \theta .
We shall first differentiate the function r=1+cosθr=1+\cos \theta with respect to angle, θ\theta and find the derivative, drdθ\dfrac{dr}{d\theta }.
drdθ=ddθ(1+cosθ)\Rightarrow \dfrac{dr}{d\theta }=\dfrac{d}{d\theta }\left( 1+\cos \theta \right)
drdθ=ddθ(1)+ddθcosθ\Rightarrow \dfrac{dr}{d\theta }=\dfrac{d}{d\theta }\left( 1 \right)+\dfrac{d}{d\theta }\cos \theta
Here, we shall use a property of differentials ddxc=0\dfrac{d}{dx}c=0and ddxcosx=sinx\dfrac{d}{dx}\cos x=-\sin x
drdθ=sinθ\Rightarrow \dfrac{dr}{d\theta }=-\sin \theta …………………….. equation (1)
The formula of arc length, LL is given as:
L=abr2+(drdθ)2.dθL=\int\limits_{a}^{b}{\sqrt{{{r}^{2}}+{{\left( \dfrac{dr}{d\theta } \right)}^{2}}}.d\theta }
Where,
a=a= lower limit of integral
b=b= upper limit of integral
drdθ=\dfrac{dr}{d\theta }=derivative of the function
r=r=the equation of cardioid
Substituting the value of derivative of function, we get
L=02π(1+cosθ)2+(sinθ)2.dθL=\int\limits_{0}^{2\pi }{\sqrt{{{\left( 1+\cos \theta \right)}^{2}}+{{\left( -\sin \theta \right)}^{2}}}.d\theta }
The above function, L has the time period =π=\pi and thus we can use the property of definite integration 0nTf(x).dx=n0Tf(x).dx\int\limits_{0}^{nT}{f\left( x \right).dx}=n\int\limits_{0}^{T}{f\left( x \right).dx} where TT is the time period of f(x)f\left( x \right).
We will expand the terms within the square, (1+cosθ)2{{\left( 1+\cos \theta \right)}^{2}}using the algebraic property (ab)2=a2+b22ab{{\left( a-b \right)}^{2}}={{a}^{2}}+{{b}^{2}}-2ab.
L=20π(1+cos2θ+2cosθ)+(sin2θ).dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{\left( 1+{{\cos }^{2}}\theta +2\cos \theta \right)+\left( {{\sin }^{2}}\theta \right)}.d\theta }
Applying sin2θ+cos2θ=1{{\sin }^{2}}\theta +{{\cos }^{2}}\theta =1, we get
L=20π1+2cosθ+1.dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{1+2\cos \theta +1}.d\theta }
L=20π2+2cosθ.dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{2+2\cos \theta }.d\theta }
L=20π2(1+cosθ).dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{2\left( 1+\cos \theta \right)}.d\theta }
We will use the property of trigonometric function here according to which 1+cosθ=2sin2θ1+\cos \theta =2{{\sin }^{2}}\theta .
L=20π2(2cos2(θ2)).dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{2\left( 2{{\cos }^{2}}\left( \dfrac{\theta }{2} \right) \right)}.d\theta }
L=20π4cos2(θ2).dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{4{{\cos }^{2}}\left( \dfrac{\theta }{2} \right)}.d\theta }
We know that 2×2=42\times 2=4 or 22=4{{2}^{2}}=4. Substituting this value, we get
L=20π(22)cos2θ2.dθ\Rightarrow L=2\int\limits_{0}^{\pi }{\sqrt{\left( {{2}^{2}} \right){{\cos }^{2}}\dfrac{\theta }{2}}.d\theta }
L=20π2cosθ2.dθ\Rightarrow L=2\int\limits_{0}^{\pi }{2\cos \dfrac{\theta }{2}.d\theta }
Taking the constant 2, outside the integral, we get
L=40πcosθ2.dθ\Rightarrow L=4\int\limits_{0}^{\pi }{\cos \dfrac{\theta }{2}.d\theta }
L=4[2sinθ2]0π\Rightarrow L=4\left[ 2\sin \dfrac{\theta }{2} \right]_{0}^{\pi }
L=8[sinπ2sin0]\Rightarrow L=8\left[ \sin \dfrac{\pi }{2}-\sin 0 \right]
L=8[10]\Rightarrow L=8\left[ 1-0 \right]
L=8\Rightarrow L=8
Therefore, the arc length of the cardioid r=1+cosθr=1+\cos \theta from 00 to 2π2\pi is 8 units.

Note: We must have prior knowledge of the various formulae of integration and in order to proceed with such problems. The property of integration used in this problem is cosx.dx=sinx+C\int{\cos x.dx=\sin x+C} but since the limits of integration were already provided, thus we removed the constant of integration, C and substituted the upper and lower limits as 0 and 2π2\pi respectively.