a) We can express the region R using polar coordinates with limits on θ between 0 and π/2, and limits on r between 2 and 3.
Hence,
we have:
![JJRdA/(x²+y²+1) = ∫[θ=0]^[π/2] ∫[r=2]^[3] (r / (r² + 1)) drd](https://img.qammunity.org/2024/formulas/physics/high-school/eexxnrto4371xhokke7lbybnmzwxjgrwm5.png)
Using substitution method,
let u = r² + 1.
Then,
du = 2r dr.
We can then use this substitution in our integral to get:
JRdA/(x²+y²+1) = ∫[θ=0]^[π/2] \
∫[u=5]^[10] (1/2)
du dθ = ∫[θ=0]^[π/2] (1/2)
[u]5^10 dθ = ∫[θ=0]^[π/2]
(1/2) (10 - 5)
dθ= 5/4 (π/2)= (5π)/8b)
We can write the given function in polar form as:
2x² + y² = 2r² cos² θ + r² sin² θ
= r² (2 cos² θ + sin² θ) =
r² (2 cos² θ + 1 - cos² θ)
= r² (cos² θ + 1)
Hence,
the integral becomes:
JJR2x² + y²
dA = ∫[θ=0]^[2π] ∫[r=0]^[2 cos θ] r² (cos² θ + 1)
drdθ= ∫[θ=0]^[2π] [(2/3) cos³ θ + 2 cos θ]
dθ= (8π)/3
We can sketch the two regions as follows:1.
Region R lies in the upper second quadrant between the concentric circles (origin-centered) of radii 2 and 3.2.
Region R2 lies inside the circle x² + y² = 4.
To know more abo