Math Problem Statement

Please find the area of the inside loop of the Limacon r=1+2cos(theta) in terms of square roots and pi.

Solution

To find the area of the inner loop of the limaçon r=1+2cosθr = 1 + 2\cos\theta, we’ll follow these steps:

  1. Identify the range of θ\theta that defines the inner loop.

    The inner loop appears when r=1+2cosθr = 1 + 2\cos\theta is negative. To find when r=0r = 0, set: 1+2cosθ=01 + 2\cos\theta = 0 Solving for cosθ\cos\theta, we get: cosθ=12\cos\theta = -\frac{1}{2} This happens at θ=2π3\theta = \frac{2\pi}{3} and θ=4π3\theta = \frac{4\pi}{3}. Therefore, the inner loop is traced from θ=2π3\theta = \frac{2\pi}{3} to θ=4π3\theta = \frac{4\pi}{3}.

  2. Set up the area integral for the inner loop.

    The area AA inside a polar curve r=f(θ)r = f(\theta) from θ=a\theta = a to θ=b\theta = b is given by: A=12abr2dθA = \frac{1}{2} \int_a^b r^2 \, d\theta For the inner loop, a=2π3a = \frac{2\pi}{3} and b=4π3b = \frac{4\pi}{3}, so we have: A=122π34π3(1+2cosθ)2dθA = \frac{1}{2} \int_{\frac{2\pi}{3}}^{\frac{4\pi}{3}} (1 + 2\cos\theta)^2 \, d\theta

  3. Expand (1+2cosθ)2(1 + 2\cos\theta)^2 and simplify the integral.

    Expanding (1+2cosθ)2(1 + 2\cos\theta)^2 gives: (1+2cosθ)2=1+4cosθ+4cos2θ(1 + 2\cos\theta)^2 = 1 + 4\cos\theta + 4\cos^2\theta Using the identity cos2θ=1+cos(2θ)2\cos^2\theta = \frac{1 + \cos(2\theta)}{2}, we substitute: 1+4cosθ+4cos2θ=1+4cosθ+4(1+cos(2θ)2)1 + 4\cos\theta + 4\cos^2\theta = 1 + 4\cos\theta + 4\left(\frac{1 + \cos(2\theta)}{2}\right) Simplifying further: =1+4cosθ+2+2cos(2θ)=3+4cosθ+2cos(2θ)= 1 + 4\cos\theta + 2 + 2\cos(2\theta) = 3 + 4\cos\theta + 2\cos(2\theta)

  4. Evaluate the integral.

    Substitute back into the integral: A=122π34π3(3+4cosθ+2cos(2θ))dθA = \frac{1}{2} \int_{\frac{2\pi}{3}}^{\frac{4\pi}{3}} \left(3 + 4\cos\theta + 2\cos(2\theta)\right) d\theta We can now integrate each term separately over [2π3,4π3]\left[\frac{2\pi}{3}, \frac{4\pi}{3}\right]:

    • For 2π34π33dθ=3(4π32π3)=32π3=2π\int_{\frac{2\pi}{3}}^{\frac{4\pi}{3}} 3 \, d\theta = 3\left(\frac{4\pi}{3} - \frac{2\pi}{3}\right) = 3 \cdot \frac{2\pi}{3} = 2\pi.

    • The integrals of cosθ\cos\theta and cos(2θ)\cos(2\theta) over this symmetric interval are zero, since they average out to zero over a complete cycle.

    Thus, we find: A=122π=πA = \frac{1}{2} \cdot 2\pi = \pi

Answer:

The area of the inner loop of the limaçon r=1+2cosθr = 1 + 2\cos\theta is: A=πA = \pi

Would you like more details or have any questions?

Relative Questions

  1. How do you find the area of a polar curve in general?
  2. Why does r=1+2cosθr = 1 + 2\cos\theta produce an inner loop, and what does that mean geometrically?
  3. What is the significance of symmetry in simplifying integrals over trigonometric functions?
  4. Could the area of the outer loop for this limaçon be calculated in a similar way?
  5. How would the solution change if the equation were r=1+2sinθr = 1 + 2\sin\theta?

Tip:

When integrating trigonometric functions over symmetric intervals, check if parts of the function (like cosθ\cos \theta or cos(2θ)\cos(2\theta)) average to zero—it can save time on calculations!

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Math Problem Analysis

Mathematical Concepts

Polar Coordinates
Area Calculation
Trigonometric Functions

Formulas

Area of a polar curve: A = 0.5 * ∫ r^2 dθ
Trigonometric identity: cos^2(θ) = (1 + cos(2θ)) / 2

Theorems

Symmetry in Trigonometric Functions

Suitable Grade Level

Undergraduate Mathematics