Area of Region Common to r=4sinθ & r=4cosθ

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The area of the region common to the polar equations r = 4sinθ and r = 4cosθ is determined by finding the limits of integration, which are θ = 0 and θ = π/6. The intersection points occur at (0,0) and θ = π/6 for r = 4sinθ, while θ = 0 for r = 4cosθ. To calculate the area, the formula A = 1/2∫r^2dθ is applied, leading to the integration of both functions over the specified limits. The final area is computed as 2π/3 - √3 square units. This solution effectively utilizes symmetry and the properties of polar coordinates.
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Find the area of the region common to r=4\sin\theta and r=4\cos\theta

How can I find the limits of integration? I know one of the limits is pi/4 by setting r1 = r2 but I can't find the other one because it is different for each equation. The graph shows it intersecting at (0,0), but that's a different theta for each equation.
 
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The easy way to do this is to use the symmetry. Integrate r= 4 sin(\theta) for \theta= 0 to \frac{\pi}{4}, then double it.
 


To find the limits of integration for this problem, we can use the fact that the two equations intersect at (0,0). This means that at this point, both r values are equal to 4. So, we can set r1 = r2 and solve for theta to find the common limit of integration.

For r = 4sinθ, we have 4sinθ = 4, which gives us θ = π/6.

Similarly, for r = 4cosθ, we have 4cosθ = 4, which gives us θ = 0.

Therefore, the limits of integration for the region common to both equations are θ = 0 and θ = π/6.

To find the area of this region, we can use the formula for the area of a polar region, which is A = 1/2∫r^2dθ.

Substituting in our limits of integration and the given equations, we get:

A = 1/2∫(4sinθ)^2dθ - 1/2∫(4cosθ)^2dθ

= 1/2∫16sin^2θdθ - 1/2∫16cos^2θdθ

= 1/2(8θ - 1/2sin2θ)∣∣∣π/6 0 - 1/2(8θ + 1/2sin2θ)∣∣∣0 π/6

= 1/2(4π/3 - √3) - 1/2(0 + 0)

= 2π/3 - √3

Therefore, the area of the region common to r = 4sinθ and r = 4cosθ is 2π/3 - √3 units squared.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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