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Find the area in the interior of 
r=1-sin theta above the polar axis. Use your calculator to integrate.

33. Find the area in the interior of r=1sinθ r=1-\sin \theta above the polar axis. Use your calculator to integrate.

Full solution

Q. 33. Find the area in the interior of r=1sinθ r=1-\sin \theta above the polar axis. Use your calculator to integrate.
  1. Set up integral limits: To find the area inside the curve r=1sin(θ)r = 1 - \sin(\theta) above the polar axis, we need to set up an integral with the appropriate limits of integration. The curve crosses the polar axis at θ=π2\theta = \frac{\pi}{2} and θ=3π2\theta = \frac{3\pi}{2}. Since we are looking for the area above the polar axis, we will integrate from θ=0\theta = 0 to θ=π\theta = \pi.
  2. Area formula for polar curve: The formula for the area AA enclosed by a polar curve r(θ)r(\theta) from θ=a\theta = a to θ=b\theta = b is given by A=12ab(r(θ))2dθA = \frac{1}{2} \int_{a}^{b} (r(\theta))^2 d\theta. For our curve r=1sin(θ)r = 1 - \sin(\theta), the area AA above the polar axis is A=120π(1sin(θ))2dθA = \frac{1}{2} \int_{0}^{\pi} (1 - \sin(\theta))^2 d\theta.
  3. Expand integrand: We need to expand the integrand (1sin(θ))2(1 - \sin(\theta))^2 before integrating. Expanding gives us (1sin(θ))2=12sin(θ)+sin2(θ)(1 - \sin(\theta))^2 = 1 - 2\sin(\theta) + \sin^2(\theta). Now we can integrate each term separately.
  4. Integrate 11 and 2sin(θ)-2\sin(\theta): The integral of 11 with respect to θ\theta from 00 to π\pi is simply θ\theta evaluated from 00 to π\pi, which gives us π\pi. The integral of 2sin(θ)-2\sin(\theta) with respect to θ\theta from 00 to π\pi is 1133 evaluated from 00 to π\pi, which gives us 1166. The integral of 1177 is more complex and requires a trigonometric identity.
  5. Integrate sin2(θ)\sin^2(\theta): We use the power-reduction identity sin2(θ)=1212cos(2θ)\sin^2(\theta) = \frac{1}{2} - \frac{1}{2}\cos(2\theta) to integrate sin2(θ)\sin^2(\theta). The integral of sin2(θ)\sin^2(\theta) with respect to θ\theta from 00 to π\pi is then the integral of 1212cos(2θ)\frac{1}{2} - \frac{1}{2}\cos(2\theta) from 00 to π\pi, which is sin2(θ)=1212cos(2θ)\sin^2(\theta) = \frac{1}{2} - \frac{1}{2}\cos(2\theta)00 evaluated from 00 to π\pi.
  6. Evaluate sin2(θ)\sin^2(\theta) integral: Evaluating the integral of 1212cos(2θ)\frac{1}{2} - \frac{1}{2}\cos(2\theta) from 00 to π\pi gives us 12π14sin(2π)+14sin(0)=12π\frac{1}{2}\pi - \frac{1}{4}\sin(2\pi) + \frac{1}{4}\sin(0) = \frac{1}{2}\pi. The sin\sin terms vanish because sin(2π)=sin(0)=0\sin(2\pi) = \sin(0) = 0.
  7. Sum up integrals: Now we add up the results of the integrals: π\pi (from the integral of 11) - 44 (from the integral of 2sin(θ)-2\sin(\theta)) + 12π\frac{1}{2}\pi (from the integral of sin2(θ)\sin^2(\theta)). This gives us π4+12π=32π4\pi - 4 + \frac{1}{2}\pi = \frac{3}{2}\pi - 4.
  8. Final area calculation: Finally, we multiply the result by 1/21/2 to get the area AA, because the formula for the area in polar coordinates includes a 1/21/2 factor. So, A=1/2×(3/2π4)=3/4π2A = 1/2 \times (3/2\pi - 4) = 3/4\pi - 2.

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