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Calculus 2nd Edition Rogawski

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414 CHAPTER 8 TECHNIQUES OF INTEGRATION<br />

The key step in Integration by Parts is deciding how to write the integrand as a product<br />

uv ′ . Keep in mind that Integration by Parts expresses ∫ uv ′ dx in terms of uv and ∫ u ′ vdx.<br />

This is useful if u ′ v is easier to integrate than uv ′ . Here are two guidelines:<br />

• Choose u so that u ′ is “simpler” ∫ than u itself.<br />

• Choose v ′ so that v = v ′ dx can be evaluated.<br />

EXAMPLE 2 Good Versus Bad Choices of u and v ′<br />

∫<br />

Evaluate<br />

xe x dx.<br />

Solution Based on our guidelines, it makes sense to write xe x = uv ′ with<br />

• u = x (since u ′ = 1 is simpler) ∫<br />

• v ′ = e x (since we can evaluate v = e x dx = e x + C)<br />

Integration by Parts gives us<br />

∫<br />

∫<br />

xe x dx = u(x)v(x) −<br />

∫<br />

u ′ (x)v(x) dx = xe x −<br />

e x dx = xe x − e x + C<br />

Let’s see what happens if we write xe x = uv ′ with u = e x , v ′ = x. Then<br />

∫<br />

u ′ (x) = e x , v(x) = xdx= 1 2 x2 + C<br />

∫<br />

}{{}<br />

xe x dx = 1 2 x2 e x<br />

uv ′ } {{ }<br />

uv<br />

−<br />

∫ 1<br />

2 x2 e x dx<br />

} {{ }<br />

u ′ v<br />

This is a poor choice of u and v ′ because the integral on the right is more complicated<br />

than our original integral.<br />

∫<br />

EXAMPLE 3 Integrating by Parts More Than Once Evaluate<br />

x 2 cos xdx.<br />

In Example 3, it makes sense to take<br />

u = x 2 because Integration by Parts<br />

reduces the integration of x 2 cos x to the<br />

integration of 2x sin x, which is easier.<br />

Solution Apply Integration by Parts a first time with u = x 2 and v ′ = cos x:<br />

∫<br />

∫<br />

∫<br />

x<br />

} 2 cos<br />

{{<br />

x<br />

}<br />

dx = x<br />

} 2 {{<br />

sin x<br />

}<br />

− 2x<br />

} {{<br />

sin x<br />

}<br />

dx = x 2 sin x − 2 x sin xdx 2<br />

uv ′<br />

uv<br />

u ′ v<br />

Now apply it again to the integral on the right, this time with u = x and v ′ = sin x:<br />

∫<br />

∫<br />

x<br />

}<br />

sin<br />

{{<br />

x<br />

}<br />

dx = −x<br />

} {{<br />

cos x<br />

}<br />

− (− cos x) dx = −x cos x + sin x + C<br />

} {{ }<br />

uv ′<br />

uv<br />

u ′ v<br />

Using this result in Eq. (2), we obtain<br />

∫<br />

∫<br />

x 2 cos xdx= x 2 sin x − 2 x sin xdx= x 2 sin x − 2(−x cos x + sin x) + C<br />

= x 2 sin x + 2x cos x − 2 sin x + C<br />

Integration by Parts applies to definite integrals:<br />

∫ b<br />

a<br />

u(x)v ′ (x) dx = u(x)v(x)<br />

∣<br />

b<br />

a<br />

−<br />

∫ b<br />

a<br />

u ′ (x)v(x) dx

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