Solutions to Problems in 10.3© 2000 by Karl Hahn |
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a) First use the table to find the area function (and hence also the indefinite integral) of f(x) = x1/2. We see that the indefinite integral is
2
F(x) = x3/2 + C
3
where C is an undetermined constant. Now remember that we use the indefinite integral
without the undetermined constant to form the bracket-expression:
121 |
x1/2 dx = |
2 |
121 |
2662 - 16 2646which is the answer.== 882 3 3
Solutions to Problems in 10.3© 2000 by Karl Hahn |
|
b) First use the table to find the area function (and hence also the indefinite integral) of f(x) = 2x. We see that the indefinite integral is
F(x) = |
1
|
Notice that the - 1 in the expression in the table (which is itself a constant) has been absorbed here into the undetermined constant, C. Now set up the bracket-expression using the indefinite integral (without the constant, C) together with the limits of integration:
3 |
2x dx = |
1
|
2x |
3 |
1 _
(8 - √2)
ln(2)
which is the answer.
Solutions to Problems in 10.3© 2000 by Karl Hahn |
|
c) This one is a little easier than the last. Again use the table to find the expression for the indefinite integral. In this case you come up with
1
F(x) = x3 + C
3
where C again is the undetermined constant. Now write the bracket expression in which you bracket
the indefinite integral, posting the limits of integration above and below the right-hand bracket, and dropping
the undetermined constant:
2 |
x2 dx = |
1 |
2 |
1
= |
x3 |
2 |
2 |
x2 dx = |
1 |
117 |
Solutions to Problems in 10.3© 2000 by Karl Hahn |
|
d) This is one is also pretty easy, and you might be able to guess at what the indefinite integral is without looking at the table. But don't be shy about looking if you need to. You would have found that
3
F(x) = x2 + 4x + C
2
where again C is that undetermined constant. Now make the bracket equation:
5 |
3x + 4 dx = |
3 |
5 |
Solutions to Problems in 10.3© 2000 by Karl Hahn |
|
e) Again the table will give you the indefinite integral.
1
F(x) = x2 + C
2
Making the bracket equation you get
b |
mx dx = |
1 |
b |
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