To find the area enclosed by one loop of the curve given by the polar equation r = sin(2θ), we can use the formula for area in polar coordinates:
A = (1/2) ∫ r² dθ
For the given curve, we start by figuring out the limits of integration. One loop of the curve occurs when r = 0 again. Setting sin(2θ) = 0, we can determine:
2θ = nπfor integersnθ = nπ/2
For the first loop, we can choose n = 0 leading to:
θ = 0 to θ = π/2.
Now we can set up the integral for the area:
A = (1/2) ∫ (sin(2θ))² dθ
Next, we apply the double angle identity:
(sin(2θ))² = (1 - cos(4θ))/2
Thus, the integral becomes:
A = (1/2) ∫ (1 - cos(4θ))/2 dθ
Now, integrating from 0 to π/2:
A = (1/4) ∫ (1 - cos(4θ)) dθ
This can be split into two integrals:
A = (1/4)(∫ dθ - ∫ cos(4θ) dθ)
Calculating each part:
∫ dθ = θ and ∫ cos(4θ) dθ = (1/4)sin(4θ)
Now evaluate from 0 to π/2:
A = (1/4)[θ - (1/4)sin(4θ)]_0^{π/2}
Plugging in the upper limit:
A = (1/4)[(π/2) - (1/4)sin(2π)] - (1/4)[0 - (1/4)sin(0)]
This simplifies to:
A = (1/4)(π/2) = π/8
Hence, the area enclosed by one loop of the curve r = sin(2θ) is:
π/8.