This theorem implies that a double integral over a rectangle region can be always calculated from two iterated integrals. If z=f(x,y) is integrable over D={(x,y)∣a≤x≤b,c≤y≤d}, the double integral over D is ∬Df(x,y)dA=∫ab∫cdf(x,y)dydx=∫cd∫abf(x,y)dxdy
If some variables are included in the interval of integration, the strong Fubini’s theorem is a workaround, which switches the order of integration.
Definite Integral to Double Integral
The definite integral is about the limit of the area surrounded by a closed curve, while the double integral is about the limit of the volume surrounded by the closed curve.
Case 1. Area Surrounded by One Curve and Two Lines
As shown in the right figure, the area S surrounded by the curve f(x) and two lines x=x1 and x=x2 is S=∫x1x2f(x)dx=∫x1x2∫0f(x)dydx
Case 2. Area Surrounded by Two Curves and Two Lines
As shown in the right figure, the area S surrounded by the curves f(x) and g(x), and two lines x=x1 and x=x2 is S=∫x1x2f(x)−g(x)dx=∫x1x2∫g(x)f(x)dydx
Note that the order of the interval [g(x),f(x)] can be changed depending on the graphs of f(x) and g(x).
Choosing Proper Axis
This is based on the fact that the area is the same whether with respect to the x-axis or y-axis.
Case 1. Area Below a Line
With respect to each axis, the area surrounded by the line y=x, x=1, and x-axis can be obtained as follows. ⎩⎨⎧Sx=∫01xdx=∫01∫0xdydxSy=∫01(1−y)dy=∫01∫y1dxdy(x-axis)(y-axis)
Case 2. Area Below a Parabola
With respect to each axis, the area surrounded by the line y=x2, x=1, and x-axis can be obtained as follows. ⎩⎨⎧Sx=∫01x2dx=∫01∫0x2dydxSy=∫01(1−y)dy=∫01∫y1dxdy(x-axis)(y-axis)
Inequalities Representing the Area
To represent the area of a double integral as inequalities, use the relation with the close integral variable first. ∫01∫0x2dydx(x-axis)∫02∫y21dxdy(y-axis)⟹D={(x,y)∣0≤x≤1,0≤y≤x2}⟹D={(y,x)∣0≤y≤2,y2≤x≤1}
How to Switch the Order of Integration
When a double integral is impossible, changing the order of integration is a workaround.
After getting the inequalities, switch the base axis from the y-axis to the x-axis.
Then, update Dy to Dx, and reorder the integration. Dx={(x,y)∣0≤x≤21,0≤y≤2x}⟹∫021∫02xdydx(x-axis)
Example 3
∫01∫x1dydx(x-axis)⟹Dx={(x,y)∣0≤x≤1,x≤y≤1}
After getting the inequalities, switch the base axis from the x-axis to the y-axis.
Then, update Dx to Dy, and reorder the integration. Dy={(y,x)∣0≤y≤1,0≤x≤y2}⟹∫01∫0y2dxdy(y-axis)
Reordering Techniques
Case 1. Only The Lower Bound of the Outer Integral is 0 (Counterclockwise Rotation)
In this case, the form of the double integral looks like ∫0a∫f(x)f(a)f(x,y)dydx. For example, the following reordering is allowed. ∫01∫y1dxdy=∫01∫0x2dydx
The technique is as follows.
The outer integral
The lower bound is 0.
The upper bound is the same as the upper bound of the inner integral of the original double integral.
The inner integral
The lower bound is 0.
To determine the upper bound, set the lower bound of the inner integral of the original double integral to another variable, say, x. In this example, y=x. Then, the upper bound is y, which is x2.
Similar other examples are as follows.
∫01∫y1dxdy=∫01∫0xdydx,
∫0π∫yπdxdy=∫0π∫0xdydx,
∫0π∫yπdxdy=∫0π∫0xdydx,
∫01∫3x3dydx=∫03∫03ydxdy,
∫02∫2y1dxdy=∫01∫02xdydx,
∫04∫2x2dydx=∫02∫02ydxdy,
∫02∫y24dxdy=∫04∫0xdydx,
∫01∫y311dxdy=∫01∫0x3dydx,
∫01∫sin−1y2πdxdy=∫02π∫0sinxdydx.
Case 2. The Upper Bound of the Inner Integral is a Variable
For example, the following reordering is allowed. ∫01∫x2xdydx=∫01∫yydxdy
The technique is as follows.
The outer integral
The lower bound is 0.
Let a be the upper bound of the outer integral of the original double integral. Also, let a function f be the upper bound of the inner integral of the original double integral since it is not a constant. Then, the upper bound is f(a).
The inner integral
To determine the lower bound, set the upper bound of the inner integral of the original double integral to another variable, say, y. In this example, x=y. Then, the lower bound is x, which is y.
To determine the upper bound, set the lower bound of the inner integral of the original double integral to another variable, say, y. In this example, x2=y. Then, the upper bound is x, which is y.
Similar other examples are as follows.
∫02∫x22xdydx=∫04∫2yydxdy,
∫08∫4y3ydxdy=∫02∫x34xdydx.
Case 3. The Upper Bound of the Inner Integral is cos (Not Passing Through the Origin)
For example, the following reordering is allowed. ∫02π∫0acosydxdy=∫0a∫0cos−1axdydx
The technique is as follows.
The outer integral
The lower bound is 0.
Let a be the lower bound of the outer integral of the original double integral. Also, let a function f be the upper bound of the inner integral of the original double integral since it is not a constant. Then, the upper bound is f(a).
The inner integral
The lower bound is 0.
To determine the upper bound, set the upper bound of the inner integral of the original double integral to another variable, say, x. In this example, acosy=x. Then, the upper bound is y, which is cos−1(x/a).
After getting the inequalities, switch the base axis from the x-axis to the y-axis. Then, update Dx to Dy, and reorder the integration. ⟹⟹⟹∫01∫x1(1+y2)25dydxDx={(x,y)∣0≤x≤1,x≤y≤1}Dy={(y,x)∣0≤y≤1,0≤x≤y}∫01∫0y(1+y2)25dxdy
Now, this integral can be calculated as follows. ∫01∫0y(1+y2)25dxdy=∫01y(1+y2)25dxdy=[71(1+y2)27]01=782−1
From the formula, ∫0π∫yπxcosxdxdy=∫0π∫0xxcosxdydx=∫0πxcosxxdx=[sinx]0π=0
Example 3. Calculate
∫01∫0xxex2−y2dydx+∫12∫x−11xex2−y2dydx
After drawing each inequality from the two integrals, it can be noticed that two regions can be merged. ∫01∫yy+1xex2−y2dxdy
Now, this integral can be directly calculated as follows. ∫01∫yy+1xex2−y2dxdy=∫012e2y+1−1dy=4e3−e−2
Example 4. Calculate
∫0∞xtan−1πx−tan−1xdx
Using the following known integral result, this can be changed to a double integral. ⟹∫1+x21=tan−1x∫0∞xtan−1πx−tan−1xdx=∫0∞x[tan−1xy]1πdx=∫0∞∫1π1+x2y21dydx
Then, from the definition of Fubini’s theorem, this can be calculated as follows. ∫0∞∫1π1+x2y21dydx=∫1π∫0∞1+x2y21dxdy=∫1π[ytan−1xy]0∞dy=2π∫1πy1dy=2π[lny]1π=2πlnπ
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