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Mathematics · 术语表

什么是 Elementary domains?

又称: area of a plane domain

Definition 20.11 University Mathematics — Year 2 · 第 20 章 — Line Integrals and Multiple Integrals

A domain D⊆R2D \subseteq \R^2 is yy-elementary if

D={(x,y):a≤x≤b, φ1(x)≤y≤φ2(x)}D = \{(x, y) : a \leq x \leq b,\ \varphi_1(x) \leq y \leq \varphi_2(x)\}

with φ1≤φ2\varphi_1 \leq \varphi_2 continuous on [a,b][a,b] (xx-elementary: symmetrically). For ff continuous on a yy-elementary DD,

∬Df=∫ab(∫φ1(x)φ2(x)f(x,y)  ⁣dy) ⁣dx,\iint_D f = \int_a^b\Bigl( \int_{\varphi_1(x)}^{\varphi_2(x)} f(x,y)\,\dd y\Bigr)\dd x ,

and one checks (by extending ff by an approximation argument, or by subdividing) that when DD is elementary in both directions the two iterated integrals agree. Domains cut into finitely many elementary pieces are handled by additivity, and the area of DD is Area⁡(D)=∬D1\operatorname {Area}(D) = \iint_D 1.

示例

Example 20.12

On the triangle D={0≤x≤1, 0≤y≤x}D = \{0 \leq x \leq 1,\ 0 \leq y \leq x\}:

∬Dxy  ⁣dx  ⁣dy=∫01x(∫0xy  ⁣dy) ⁣dx=∫01x⋅x22  ⁣dx=18.\iint_D xy \,\dd x\,\dd y = \int_0^1 x\Bigl(\int_0^x y\,\dd y\Bigr)\dd x = \int_0^1 x\cdot\frac{x^2}{2}\,\dd x = \frac18 .

Swapping the order (xx from yy to 11): ∫01y(∫y1x  ⁣dx) ⁣dy=∫01y 1−y22  ⁣dy=18\int_0^1 y\bigl(\int_y^1 x\,\dd x\bigr)\dd y = \int_0^1 y\,\frac{1 - y^2}{2}\,\dd y = \frac18 — same value, different computation: choosing the order of integration well is half the craft.

Example 20.13 (When only one order works)

Compute I=∫01 ⁣ ⁣∫x1ey2  ⁣dy  ⁣dxI = \displaystyle\int_0^1\!\!\int_x^1 \eu^{y^2}\,\dd y\,\dd x. As written, the inner integral ∫ey2 ⁣dy\int\eu^{y^2}\dd y has no elementary antiderivative: the computation is stuck. But the domain is the triangle 0≤x≤y≤10 \leq x \leq y \leq 1, which is elementary in both directions; swapping the order,

I=∫01 ⁣ ⁣∫0yey2  ⁣dx  ⁣dy=∫01y ey2  ⁣dy=[12ey2]01=e−12.I = \int_0^1\!\!\int_0^y \eu^{y^2}\,\dd x\,\dd y = \int_0^1 y\,\eu^{y^2}\,\dd y = \Bigl[\tfrac12\eu^{y^2}\Bigr]_0^1 = \frac{\eu - 1}{2} .

The inner variable xx appeared nowhere in the integrand, so integrating it first produced exactly the factor yy that makes the outer integral immediate. Moral: Fubini is not just a license to iterate — it is a license to choose, and the right order can turn an impossible integral into a one-liner. Always sketch the domain and read off both descriptions before starting.

Example 20.18 (Affine changes of variables)

For an affine map Φ(u,v)=M(u,v)T+C\Phi(u, v) = M(u, v)^{\mathsf T} + C with MM invertible, the Jacobian is the constant matrix MM: areas are multiplied by the constant factor ∣det⁡M∣\abs{\det M} — the promise made in Chapter 17 is now a theorem. Two immediate uses. The ellipse x2a2+y2b2≤1\frac{x^2}{a^2} + \frac{y^2}{b^2} \leq 1 is the image of the unit disk under (u,v)↦(au,bv)(u, v) \mapsto (au, bv), so its area is ab⋅πab \cdot \pi — no computation. And for the integral of f(x+y)f(x + y) over the square K=[0, 1]2K = \intcc01^2, the shear Φ(u,v)=(u−v,v)\Phi(u, v) = (u - v, v) (determinant 11) turns it into an integral of f(u)f(u) over a parallelogram, which Fubini slices at constant uu: with f=exp⁡f = \exp,

∬Kex+y  ⁣dx  ⁣dy=(∫01ex  ⁣dx)2=(e−1)2,\iint_K \eu^{x+y}\,\dd x\,\dd y = \Bigl(\int_0^1 \eu^x\,\dd x\Bigr)^2 = (\eu - 1)^2,

as the product structure confirms. Choosing coordinates adapted to the integrand — not to the domain — is the other half of the craft.

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