[PDF] Chapter 0706 Integrating Discrete Functions - MATH FOR COLLEGE





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Chapter 0706 Integrating Discrete Functions - MATH FOR COLLEGE

Dec 23 2009 · 07 06 4 Chapter 07 06 and applying the trapezoidal rule over each of the above integrals gives

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07.06.1

Chapter 07.06

Integrating Discrete Functions

After reading this chapter, you should be able to: 1. integrate discrete functions by several methods, 2. derive the formula for trapezoidal rule with unequal segments, and 3. solve examples of finding integrals of discrete functions.

What is integration?

Integration is the process of m

easuring the area under a function plotted on a graph. Why would we want to integrate a function? Among the most common examples are finding the velocity of a body from an acceleration function, and displacement of a body from a velocity function. Throughout many engineering fields, there are (what sometimes seems like) countless applications for integral calculus. You can read about a few of these applications in different engineering majors in Chapters 07.00A-07.00G. Sometimes, the function to be integrated is given at discrete data points, and the area under the curve is needed to be approximated. Here, we will discuss the integration of such discrete functions, b a dxxfI where )(xf is called the integrand and is given at discrete value of x, a lower limit of integration b upper limit of integration

07.06.2 Chapter 07.06

Figure 1 Integration of a function

Integrating discrete functions

Multiple methods of integrating discrete functions are shown below using an example.

Example 1

The upward velocity of a rocket is given as a function of tim e in Table 1.

Table 1 Velocity as a function of time.

(s)t )m/s()(tv 0 0

10 227.04

15 362.78

20 517.35

22.5 602.97

30 901.67

Determine the distance,

,s covered by the rocket from 11t to 16t using the velocity data provided and use any applicable numerical technique.

Solution

Method 1: Average Velocity Method

The velocity of the rocket is not provided at

11t and ,16t so we will have to use an

interval that includes

16,11 to find the average velocity of the rocket within that range. In

this case, the interval

20,10 will suffice.

04.227)10(v

78.362)15(v

35.517)20(v

Integrating Discrete Functions 07.06.3

3)20()15()10(vvvVelocityAverage

335.51778.36204.227

m/s06.369 Figure 1 Velocity vs. time data for the rocket example Using ,tvs we get m3.1845)1116)(06.369(s

Method 2: Trapezoidal Rule

If we were finding the distance traveled between times in the data table, we would simply find the area of the trapezoids with the corner points given as the velocity and time data points. For example 20 10 )(dttv 20 1515
10 )()(dttvdttv and applying the trapezoidal rule over each of the above integrals gives 20 10 )(dttv )]20()15([21520)]15()10([21015vvvv The values of )10(v, )15(v and )20(v are given in Table 1.

However, we are interested in finding

16 11 )(dttv 16 1515
11 )()(dttvdttv

07.06.4 Chapter 07.06

and applying the trapezoidal rule over each of the above integrals gives 16 11 )(dttv)]16()15([21516)]15()11([21115vvvv ))16(78.362(21516)78.362)11((21115vv How do we find )11(v and )16(v? We use linear interpolation. To find )11(v, ,10148.2704.227)(ttv 1510t

1011148.2704.227)11(v

m/s19.254 and to find )16(v ,15913.3078.362)(ttv 2015t

1516913.3078.362)16(v

m/s69.393 Then 16 11 )69.39378.362(21516)78.36219.254(21115 m2.1612 Method 3: Polynomial interpolation to find the velocity profile Because we are finding the area under the curve from ,20,10 we must use three points, ,10 t ,15t and ,20t to fit a quadratic polynomial through the data. Using polynomial interpolation, our resulting velocity function is (refer to notes on direct method of interpolation) .2010,3766.0733.1705.12 2 ttttv Now, we simply take the integral of the quadratic within our limits, giving us 16 11 2

3766.0733.1705.12dttts

16 1132

33766.0

2733.1705.12

ttt 3322

111633766.011162733.17111605.12

m3.1604 Method 4: Spline interpolation to find the velocity profile Fitting quadratic splines (refer to notes on spline method of interpolation) through the data results in the following set of quadratics ,704.22)(ttv 100t
,88.88928.48888.0 2 tt 1510t

Integrating Discrete Functions 07.06.5

,61.14166.351356.0 2 tt 2015t ,55.554956.336048.1 2 tt 5.2220t ,13.15286.2820889.0 2 tt 305.22t

The value of the integral would then simply be

16 1515
11 )()(dttvdttvs 16 15 2 15 11 2 16

1523151123

61.141266.35

31356.088.882928.4

38888.0

tttttt

111588.8811152928.4111538888.0

2233

151661.1411516266.35151631356.0

23
2233
m9.1595

Example 2

What is the absolute relative true error for each of the four methods used in Example 1 if the data in Table 1 was actually obtained from the velocity profile of tttv8.92100140000140000ln2000)(, where v is given in m/s and t in s.

Solution

The distance covered between 11tand 16t is

16 11

8.92100140000140000ln2000dttts

m9.1604

Method 1

The approximate value obtained using average velocity method was m3.1845. Hence, the absolute relative true error, t , is %1009.16043.18459.1604 t %976.14

Method 2:

The approximate value obtained using the trapezoidal rule was m2.1612. Hence, the absolute relative true error, t , is

07.06.6 Chapter 07.06

%1009.16042.16129.1604 t %451.0

Method 3:

The approximate value obtained using the direct polynomial was 1604.3 m. Hence, the absolute relative true error, t , is %1009.16043.16049.1604 t %037.0

Method 4:

The approximate value obtained using the spline interpolation was 1595.9 m, hence, the absolute relative true error, t , is %1009.16049.15959.1604 t %564.0 Table 2 Comparison of discrete function methods of numerical integration

Method

Approximate

Value t

Average Velocity 1845.3 14.976%

Trapezoidal Rule 1612.2 0.451%

Polynomial Interpolation 1604.3 0.037%

Spline Interpolation 1595.9 0.564%

Trapezoidal Rule for Discrete Functions with Unequal Segments For a general case of a function given at ndata points 11 ,xfx,quotesdbs_dbs16.pdfusesText_22
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