6 Applications of surface integration over rectangular areas

6.1 Force on a dam

At the beginning of this Section, the total force on a dam was given by the surface integral

A k ( h y ) d A

Imagine that the dam is rectangular in profile with a width of 100 m and a height h of 40 m. The expression d A is replaced by d x d y and the limits on the variables x and y are 0 to 100 m and 0 to 40 m respectively. The constant k may be assumed to be 1 0 4 kg m 2 s 2 . The surface integral becomes the double integral

0 40 0 100 k ( h y ) d x d y that is 0 40 0 100 1 0 4 ( 40 y ) d x d y

As the integral in this double integral does not contain x , the integral may be written

0 40 0 100 1 0 4 ( 40 y ) d x d y = ( 100 0 ) 0 40 1 0 4 ( 40 y ) d y = 100 × 1 0 4 40 y y 2 2 0 40 = 1 0 6 [ ( 40 × 40 4 0 2 2 ) 0 ] = 1 0 6 × 800 = 8 × 1 0 8  N

that is the total force is 800 meganewtons.

6.2 Centre of pressure

We wish to find the centre of pressure ( x p , y p ) of a plane area immersed vertically in a fluid. Take the x axis to be in the surface of the fluid and the y axis to be vertically down, so that the plane O x y contains the area.

Figure 7

No alt text was set. Please request alt text from the person who provided you with this resource.

We require the following results:

  1. The pressure p is proportional to the depth h , so that p = ω h where ω is a constant.
  2. The force F on an area δ A subjected to constant pressure p is given by F = p δ A

Consider a small element of area δ A at the position shown. The pressure at δ A is ω y . Then the force acting on δ A is ω y δ A . Hence the total force acting on the area A is A ω y d A = ω A y d A .

Moment of force on δ A about O y = ω x y δ A Total moment of force on δ A about O y = ω A x y d A Moment of force on δ A about O x = ω y 2 δ A Total moment of force on δ A about O x = ω A y 2 d A

Taking moments about O y :

total force × x p = total moment ω A y d A x p = ω A x y d A x p A y d A = A x y d A

Taking moments about O x :

total force × y p = total moment ω A y d A y p = ω A y 2 d A y p A y d A = A y 2 d A

Hence

x p = A x y d A A y d A and y p = A y 2 d A A y d A .

Example 6

A rectangle of sides a and b is immersed vertically in a fluid with one of its edges in the surface as shown in Figure 8. Where is the centre of pressure?

Figure 8

No alt text was set. Please request alt text from the person who provided you with this resource.

Solution

To express the surface integral as double integrals we will use cartesian coordinates and vertical slices. We need the following integrals.

A y d A = 0 b 0 a y d y d x = 0 b 1 2 y 2 0 a d x = 0 b 1 2 a 2 d x = 1 2 a 2 x 0 b = 1 2 a 2 b A x y d A = 0 b 0 a x y d y d x = 0 b 1 2 x y 2 0 a d x = 0 b 1 2 x a 2 d x = 1 4 x 2 a 2 0 b = 1 4 a 2 b 2 A y 2 d A = 0 b 0 a y 2 d y d x = 0 b 1 3 y 3 0 a d x = 0 b 1 3 a 3 d x = 1 3 a 3 x 0 b = 1 3 a 3 b

Hence

y p = A y 2 d A A y d A = 1 3 a 3 b 1 2 a 2 b = 2 3 a and x p = A x y d A A y d A = 1 4 a 2 b 2 1 2 a 2 b = 1 2 b

The centre of pressure is ( 1 2 b , 2 3 a ) , so is at a depth of 2 3 a .

6.3 Areas and moments

The surface integral A f ( x , y ) d A can represent a number of physical quantities, depending on the function f ( x , y ) that is used.

Properties:

  1. If f ( x , y ) = 1 then the integral represents the area of A .
  2. If f ( x , y ) = x then the integral represents the first moment of A about the y axis.
  3. If f ( x , y ) = y then the integral represents the first moment of A about the x axis.
  4. If f ( x , y ) = x 2 then the integral represents the second moment of A about the y axis.
  5. If f ( x , y ) = y 2 then the integral represents the second moment of A about the x axis.
  6. If f ( x , y ) = x 2 + y 2 then the integral represents the second moment of A about the z axis.
Example 7

Given a rectangular lamina of length , width b , thickness t (small) and density ρ (see Figure 9), find the second moment of area of this lamina (moment of inertia) about the x -axis.

Figure 9

No alt text was set. Please request alt text from the person who provided you with this resource.

Solution

By property (e) above, the moment of inertia is given by

0 b 0 y 2 ρ t d x d y = ρ t ( 0 ) 0 b y 2 d y = ρ t y 3 3 0 b = ρ t b 3 3

As the mass of the lamina is M = b t ρ , the moment of inertia simplifies to 1 3 M b 2 . The t and ρ are included in the integral to make it a moment of inertia rather than simply a second moment.

Task!

By a similar method to that in Example 7, find the moment of inertia of the same lamina about the y -axis.

From property (d) above, the moment of inertia (or second moment of area) is given by the integral

0 l 0 b x 2 ρ t d y d x = ρ t ( b 0 ) 0 l x 2 d x = b ρ t x 3 3 0 l = b ρ t l 3 3

As the mass of the lamina is M = l b ρ t , the moment of inertia simplifies to 1 3 M l 2 . Again, the t and ρ are included in the integral to make it a moment of inertia rather than simple a second moment.

Exercises

By making use of the form of the integrand, evaluate the following double integrals:

  1. I = 0 π 0 1 y cos 2 x d y d x
  2. I = 8 3 1 1 y 2 d y d x
  3. I = 0 1 0 5 s + 1 4 d t d s
  1. π 4
  2. 22 3
  3. 31