🌱 Tony's Memex Tony's Intertwingled Memex
Digital Garden | OER Curriculum
Home / Digital Garden / Double Integrals over a Rectangular Region

Double Integrals over a Rectangular Region

Core Definition

For a continuous function of two variables f(x,y)f(x, y) defined over a closed rectangular domain R=[a,b]Γ—[c,d]={(x,y)∈R2∣a≀x≀b, c≀y≀d}R = [a, b] \times [c, d] = \{(x, y) \in \mathbb{R}^2 \mid a \le x \le b, \, c \le y \le d\}, the double integral ∬Rf(x,y) dA\iint_R f(x, y) \, dA evaluates the limit of Riemann sums over planar grid partitions:

∬Rf(x,y) dA=lim⁑Δxβ†’0Ξ”yβ†’0βˆ‘i=1mβˆ‘j=1nf(xijβˆ—,yijβˆ—) Δx Δy\iint_R f(x, y) \, dA = \lim_{\substack{\Delta x \to 0 \\ \Delta y \to 0}} \sum_{i=1}^m \sum_{j=1}^n f(x_{ij}^*, y_{ij}^*) \, \Delta x \, \Delta y
By Fubini's Theorem, the double integral equals the iterated single integrals evaluated in either order:
∬Rf(x,y) dA=∫cd∫abf(x,y) dx dy=∫ab∫cdf(x,y) dy dx\iint_R f(x, y) \, dA = \int_{c}^{d} \int_{a}^{b} f(x, y) \, dx \, dy = \int_{a}^{b} \int_{c}^{d} f(x, y) \, dy \, dx

Concept Explanation

When integrating over a rectangle in the xyxy-plane, all four boundaries are fixed geometric constants (x=a,x=b,y=c,y=dx = a, x = b, y = c, y = d). This geometric symmetry provides unique analytical simplifications:

1. Fubini's Theorem (Iterated Integrals)

If f(x,y)f(x, y) is continuous on the rectangle R=[a,b]Γ—[c,d]R = [a, b] \times [c, d], the double integral can be evaluated as two successive single-variable definite integrals:

  • Integrating dy dxdy \, dx (Vertical Slices First): Hold xx constant and evaluate the inner integral ∫cdf(x,y) dy\int_c^d f(x, y) \, dy to produce a single-variable function A(x)A(x) representing the cross-sectional area of the solid at position xx. Then evaluate ∫abA(x) dx\int_a^b A(x) \, dx.
  • Integrating dx dydx \, dy (Horizontal Slices First): Hold yy constant and evaluate the inner integral ∫abf(x,y) dx\int_a^b f(x, y) \, dx to produce A(y)A(y), then evaluate ∫cdA(y) dy\int_c^d A(y) \, dy.

Because the boundaries are constants, reversing the order of integration simply requires exchanging the differential order (dx dy↔dy dxdx \, dy \leftrightarrow dy \, dx) and swapping the corresponding constant limits of integration without altering boundary equations.

2. Product Separability Property

If the multivariable integrand factors cleanly into the product of a single-variable function of xx and a single-variable function of yy, such that f(x,y)=g(x)β‹…h(y)f(x, y) = g(x) \cdot h(y), then over a rectangular domain R=[a,b]Γ—[c,d]R = [a, b] \times [c, d]:

∬Rg(x)h(y) dA=(∫abg(x) dx)(∫cdh(y) dy)\iint_R g(x)h(y) \, dA = \left( \int_{a}^{b} g(x) \, dx \right) \left( \int_{c}^{d} h(y) \, dy \right)
This decouples the multivariable calculation into the product of two independent single-variable integrals, significantly accelerating evaluation.

3. Spatial Average Value Formula

In single-variable calculus, the average value of f(x)f(x) over [a,b][a, b] is favg=1bβˆ’a∫abf(x) dxf_{\text{avg}} = \frac{1}{b - a} \int_a^b f(x) \, dx. For a two-variable function f(x,y)f(x, y) over a region RR, the spatial average value is defined by dividing the total accumulated double integral by the planar surface area of the domain:

favg=1Area(R)∬Rf(x,y) dAf_{\text{avg}} = \frac{1}{\text{Area}(R)} \iint_R f(x, y) \, dA
For a rectangular domain R=[a,b]Γ—[c,d]R = [a, b] \times [c, d], the area is simply Area(R)=(bβˆ’a)(dβˆ’c)\text{Area}(R) = (b - a)(d - c).

Engineering Applications

  • Optoelectronics & Display Engineering: Evaluating average surface irradiance EavgE_{\text{avg}} and total emitted radiant luminous flux across flat-panel LED displays and solar photovoltaic panels.
  • Electrical & Computer Engineering: Calculating total electrostatic charge accumulation Q=∬RΟƒ(x,y) dAQ = \iint_R \sigma(x, y) \, dA across rectangular microchip dies and capacitive sensor pads.
  • Mechanical & Thermal Engineering: Determining total heat transfer rate q=∬Rh(x,y)(Tsβˆ’T∞) dAq = \iint_R h(x, y)(T_s - T_\infty) \, dA across rectangular radiator cooling fins and heat sinks.
  • Civil & Structural Engineering: Computing total contact load and average soil bearing pressure beneath rectangular concrete foundation footings.

Example Problems

Example 1: Basic Iterated Integration & Spatial Average

Evaluate ∬R(3x2βˆ’2y) dA\iint_R (3x^2 - 2y) \, dA over the rectangular region R=[0,2]Γ—[1,3]R = [0, 2] \times [1, 3], and determine the spatial average value favgf_{\text{avg}}.

Solution

Step 1: State Governing Formula
State Fubini's Theorem for Rectangular Regions:

∬Rf(x,y) dA=∫cd∫abf(x,y) dx dy\iint_R f(x, y) \, dA = \int_{c}^{d} \int_{a}^{b} f(x, y) \, dx \, dy
Here a=0,b=2a = 0, b = 2 and c=1,d=3c = 1, d = 3. Set up the iterated integral:
I=∫13∫02(3x2βˆ’2y) dx dyI = \int_{1}^{3} \int_{0}^{2} (3x^2 - 2y) \, dx \, dy

Step 2: Evaluate the Inner Integral (dxdx)
Treat yy as a constant:

∫02(3x2βˆ’2y) dx=[x3βˆ’2yx]x=0x=2=((2)3βˆ’2y(2))βˆ’0=8βˆ’4y\int_{0}^{2} (3x^2 - 2y) \, dx = \left[ x^3 - 2yx \right]_{x=0}^{x=2} = \Big((2)^3 - 2y(2)\Big) - 0 = 8 - 4y

Step 3: Evaluate the Outer Integral (dydy)

∫13(8βˆ’4y) dy=[8yβˆ’2y2]13=(8(3)βˆ’2(3)2)βˆ’(8(1)βˆ’2(1)2)\int_{1}^{3} (8 - 4y) \, dy = \left[ 8y - 2y^2 \right]_{1}^{3} = \Big(8(3) - 2(3)^2\Big) - \Big(8(1) - 2(1)^2\Big)
=(24βˆ’18)βˆ’(8βˆ’2)=6βˆ’6=0= (24 - 18) - (8 - 2) = 6 - 6 = 0

Step 4: Compute Spatial Average Value
State the Spatial Average Value Formula:

favg=1Area(R)∬Rf(x,y) dAf_{\text{avg}} = \frac{1}{\text{Area}(R)} \iint_R f(x, y) \, dA
The area of the rectangle is Area(R)=(2βˆ’0)(3βˆ’1)=2Γ—2=4\text{Area}(R) = (2 - 0)(3 - 1) = 2 \times 2 = 4.
favg=14(0)=0f_{\text{avg}} = \frac{1}{4} (0) = 0

Example 2: Strategic Order Selection via Fubini's Theorem

Evaluate the double integral:

∬Rxexy dAwhereΒ R=[0,1]Γ—[0,2]\iint_R x e^{xy} \, dA \quad \text{where } R = [0, 1] \times [0, 2]

Solution

Step 1: Analyze Integration Order Strategy
If we integrate with respect to xx first, the factor xx in xexyx e^{xy} forces integration by parts. However, if we integrate with respect to yy first, xx is treated as a constant multiplier that perfectly matches the internal derivative of the exponent u=xyβ€…β€ŠβŸΉβ€…β€Šdu=x dyu = xy \implies du = x \, dy. Therefore, we choose order dy dxdy \, dx.

Step 2: Set up the Iterated Integral
State Fubini's Theorem for Rectangular Regions:

∬Rxexy dA=∫01∫02xexy dy dx\iint_R x e^{xy} \, dA = \int_{0}^{1} \int_{0}^{2} x e^{xy} \, dy \, dx

Step 3: Evaluate Inner Integral (dydy)
Treating xx as constant:

∫02xexy dy=[exy]y=0y=2=e2xβˆ’e0=e2xβˆ’1\int_{0}^{2} x e^{xy} \, dy = \left[ e^{xy} \right]_{y=0}^{y=2} = e^{2x} - e^0 = e^{2x} - 1

Step 4: Evaluate Outer Integral (dxdx)

∫01(e2xβˆ’1) dx=[12e2xβˆ’x]01=(12e2βˆ’1)βˆ’(12e0βˆ’0)\int_{0}^{1} (e^{2x} - 1) \, dx = \left[ \frac{1}{2} e^{2x} - x \right]_{0}^{1} = \left( \frac{1}{2}e^2 - 1 \right) - \left( \frac{1}{2}e^0 - 0 \right)
=12e2βˆ’1βˆ’12=12e2βˆ’32= \frac{1}{2}e^2 - 1 - \frac{1}{2} = \frac{1}{2}e^2 - \frac{3}{2}


Connections & References