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Calculus- Early Transcendentals, 2021a

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494 Multiple Integration<br />

Figure 14.6: Intersection of three cylinders.<br />

Exercise 14.1.31 Prove that if f (x,y) is integrable and if g(x,y) =<br />

f (x,y).<br />

∫ x ∫ y<br />

a b<br />

Exercise 14.1.32 Reverse the order of integration on each of the following integrals<br />

f (s,t) dt ds then g xy = g yx =<br />

(a)<br />

(b)<br />

(c)<br />

(d)<br />

∫ 9 ∫ √ 9−y<br />

0 0<br />

∫ 2 ∫ lnx<br />

1 0<br />

∫ 1 ∫ π/2<br />

0 arcsiny<br />

∫ 1 ∫ 4<br />

0 4x<br />

f (x,y) dx dy<br />

f (x,y) dy dx<br />

f (x,y) dx dy<br />

f (x,y) dy dx<br />

(e)<br />

∫ 3 ∫ √ 9−y 2<br />

0 0<br />

f (x,y) dx dy<br />

Exercise 14.1.33 What are the parallels between Fubini’s Theorem and Clairaut’s Theorem?<br />

14.2 Double Integrals in Polar Coordinates<br />

Suppose we have a surface given in polar coordinates as z = f (r,θ) andwewishtofindtheintegralover<br />

some region. We could attempt to translate into rectangular coordinates and do the integration there, but it<br />

is often easier to stay in polar coordinates.<br />

How might we approximate the volume under such a surface in a way that uses polar coordinates<br />

directly? The basic idea is the same as before: we divide the region into many small regions, multiply<br />

the area of each small region by the height of the surface somewhere in that little region, and add them<br />

up. What changes is the shape of the small regions; in order to have a nice representation in terms of r

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