TheoremComplete

Fubini's Theorem

Fubini's theorem is the rigorous justification for computing multiple integrals as iterated single integrals. It guarantees that the order of integration can be interchanged under mild conditions.


The Theorem

Theorem9.4Fubini's Theorem

Let ff be continuous on a rectangle R=[a,b]×[c,d]R = [a,b] \times [c,d]. Then the double integral exists and equals either iterated integral: ∬Rf(x,y) dA=∫ab(∫cdf(x,y) dy)dx=∫cd(∫abf(x,y) dx)dy\iint_R f(x,y)\,dA = \int_a^b \left(\int_c^d f(x,y)\,dy\right)dx = \int_c^d \left(\int_a^b f(x,y)\,dx\right)dy

Theorem9.5Fubini's Theorem for General Regions

Let ff be continuous on a region DD of type I: D={(x,y):a≤x≤b,  g1(x)≤y≤g2(x)}D = \{(x,y) : a \leq x \leq b,\; g_1(x) \leq y \leq g_2(x)\} where g1,g2g_1, g_2 are continuous. Then ∬Df(x,y) dA=∫ab∫g1(x)g2(x)f(x,y) dy dx\iint_D f(x,y)\,dA = \int_a^b \int_{g_1(x)}^{g_2(x)} f(x,y)\,dy\,dx Analogously for type II regions where xx varies between functions of yy.


Changing the Order of Integration

ExampleSimplification by reversing order

Evaluate ∫01∫x1ey2 dy dx\int_0^1 \int_x^1 e^{y^2}\,dy\,dx. The inner integral ∫x1ey2 dy\int_x^1 e^{y^2}\,dy has no closed form. Reversing: the region is {(x,y):0≤y≤1,  0≤x≤y}\{(x,y) : 0 \leq y \leq 1,\; 0 \leq x \leq y\}, so ∫01∫0yey2 dx dy=∫01yey2 dy=12(e−1)\int_0^1 \int_0^y e^{y^2}\,dx\,dy = \int_0^1 y e^{y^2}\,dy = \frac{1}{2}(e - 1)

ExampleFubini fails without absolute convergence

Consider f(x,y)=x2−y2(x2+y2)2f(x,y) = \frac{x^2 - y^2}{(x^2 + y^2)^2} on (0,1]×(0,1](0,1] \times (0,1]. One can verify: ∫01∫01f(x,y) dy dx=π4,∫01∫01f(x,y) dx dy=−π4\int_0^1\int_0^1 f(x,y)\,dy\,dx = \frac{\pi}{4}, \quad \int_0^1\int_0^1 f(x,y)\,dx\,dy = -\frac{\pi}{4} The iterated integrals differ because ∬∣f∣ dA=∞\iint |f|\,dA = \infty. This shows Fubini's theorem requires integrability (or continuity) of ff.


RemarkTonelli's theorem for non-negative functions

Tonelli's theorem states that for measurable f≥0f \geq 0, the double integral and both iterated integrals always agree (even if they are all +∞+\infty). This is useful because it allows one to check integrability by computing either iterated integral of ∣f∣|f| first, then applying Fubini.