Calculus II - Assignment with Solution Key | MATH 211, Assignments of Calculus

Material Type: Assignment; Class: Calculus 2; Subject: Mathematics; University: Millersville University of Pennsylvania; Term: Summer 1 2009;

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Millersville University
Department of Mathematics
MATH 211, Calculus II
Please evaluate the following improper integrals.
1. Z1
1
1
x2/3dx
This integral is improper since the integrand possesses a discontinuity at x= 0 and
1<0<1.
Z1
1
1
x2/3dx = lim
M0ZM
1
1
x2/3dx + lim
R0+Z1
R
1
x2/3dx
= lim
M0ZM
1
x2/3dx + lim
R0+Z1
R
x2/3dx
= lim
M03x1/3
M
1+ lim
R0+3x1/3
1
R
= lim
M03M1/3+ 3+ lim
R0+33R1/3
= 3 + 3
= 6
2. Z2
−∞
2
x2+ 4 dx
This integral is improper since the lower limit of integration is −∞.
Z2
−∞
2
x2+ 4 dx = lim
R→−∞ Z2
R
2
x2+ 4 dx
= lim
R→−∞ tan1x
2
2
R!
= lim
R→−∞ tan1(1) tan1R
2
= lim
R→−∞ π
4tan1R
2
=π
4lim
R→−∞ tan1R
2
=π
4π
2
=3π
4
3. Z2
0
x+ 1
4x2dx
pf3
pf4
pf5

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Millersville University

Department of Mathematics

MATH 211, Calculus II

Please evaluate the following improper integrals.

∫ (^1)

− 1

x^2 /^3

dx

This integral is improper since the integrand possesses a discontinuity at x = 0 and − 1 < 0 < 1.

∫ (^1)

− 1

x^2 /^3

dx = lim M → 0 −

∫ (^) M

− 1

x^2 /^3

dx + lim R→ 0 +

∫ (^1)

R

x^2 /^3

dx

= lim M → 0 −

∫ (^) M

− 1

x − 2 / 3 dx + lim R→ 0 +

∫ (^1)

R

x − 2 / 3 dx

= lim M → 0 −

( 3 x 1 / 3

∣ ∣ ∣

M

− 1

)

  • lim R→ 0 +

( 3 x 1 / 3

∣ ∣ ∣

1

R

)

= lim M → 0 −

( 3 M 1 / 3

  • 3

)

  • lim R→ 0 +

( 3 − 3 R 1 / 3

)

∫ (^2)

−∞

x^2 + 4

dx

This integral is improper since the lower limit of integration is −∞.

∫ (^2)

−∞

x^2 + 4

dx = lim R→−∞

∫ (^2)

R

x^2 + 4

dx

= lim R→−∞

(

tan − 1 x 2

∣ ∣ ∣ ∣

2

R

)

= lim R→−∞

( tan − 1 (1) − tan

− 1 R

)

= lim R→−∞

( π

4

− tan

− 1 R

)

π

4

− lim R→−∞

( tan

− 1 R

)

π

4

( −

π

2

)

3 π

4

∫ (^2)

0

x + 1 √ 4 − x^2

dx

This integral is improper since the integrand is discontinuous at x = 2.

∫ (^2)

0

x + 1 √ 4 − x^2

dx = lim R→ 2 −

∫ (^) R

0

x + 1 √ 4 − x^2

dx

= lim R→ 2 −

∫ (^) R

0

( x √ 4 − x^2

4 − x^2

)

dx

= lim R→ 2 −

(

4 − x^2 + sin − 1 x 2

∣ ∣ ∣ ∣

R

0

)

= lim R→ 2 −

( −

4 − R^2 + 2 + sin−^1

R

)

∫ (^) ∞

− 1

x^2 + 5x + 6

dx

This integral is improper since the upper limit is integration is infinite.

∫ (^) ∞

− 1

x^2 + 5x + 6

dx = lim R→∞

∫ (^) R

− 1

x^2 + 5x + 6

dx

= lim R→∞

∫ (^) R

− 1

(x + 2)(x + 3)

dx

We must use partial fraction expansion to rewrite the integrand.

(x + 2)(x + 3)

A

x + 2

B

x + 3

A(x + 3) + B(x + 2)

(x + 2)(x + 3)

1 = A(x + 3) + B(x + 2)

When x = −2 we see that A = 1 and when x = −3 we have B = −1.

lim R→∞

∫ (^) R

− 1

(x + 2)(x + 3)

dx = lim R→∞

∫ (^) R

− 1

( 1

x + 2

x + 3

) dx

= lim R→∞

( ln |x + 2| − ln |x + 3||

R − 1

)

= lim R→∞

(ln |R + 2| − ln |R + 3| − ln 1 + ln 2)

= lim R→∞

(

ln

|R + 2|

|R + 3|

  • ln 2

)

= lim R→∞

( ln

∣ ∣ ∣ ∣

R + 2

R + 3

∣ ∣ ∣ ∣ + ln 2

)

= ln 1 + ln 2

= ln 2

= lim R→−∞

( −1 + e −R^2

)

  • lim M →∞

( −e −M 2

  • 1

)

∫ (^) ∞

0

16 tan − 1 x

1 + x^2

dx

This integral is improper since the upper limit of integration is infinite.

∫ (^) ∞

0

16 tan − 1 x

1 + x^2

dx = lim R→∞

∫ (^) R

0

16 tan − 1 x

1 + x^2

dx

We will integrate by substitution using

u = tan − 1 x and du =

1 + x^2

dx.

lim R→∞

∫ (^) R

0

16 tan − 1 x

1 + x^2

dx = lim R→∞

∫ (^) tan− (^1) R

0

16 u du

= lim R→∞

( 8 u^2

∣ ∣ ∣

tan−^1 R 0

)

= lim R→∞

( 8

[ tan − 1 R

] 2 )

[ π

2

] 2

= 2 π 2

∫ (^) ∞

0

2 e −x sin x dx

This integral is improper since the upper limit of integration is infinite. In order to find an antiderivative of the integrand, we must use integration by parts, twice. We make the following assignments.

u = 2 e −x v = − cos x

du = − 2 e −x dx dv = sin x dx

Therefore ∫ 2 e −x sin x dx = − 2 e −x cos x −

∫ 2 e −x cos x dx.

For the second integration by parts step we make the assignments:

u = 2 e −x v = sin x

du = − 2 e −x dx dv = cos x dx.

Now we have ∫ 2 e −x sin x dx = − 2 e −x cos x −

∫ 2 e −x cos x dx

= − 2 e−x^ cos x −

( 2 e−x^ sin x +

∫ 2 e−x^ sin x dx

)

= − 2 e−x^ cos x − 2 e−x^ sin x −

∫ 2 e−x^ sin x dx

∫ 2 e −x sin x dx = − 2 e −x cos x − 2 e −x sin x + C ∫ 2 e −x sin x dx = −e −x cos x − e −x sin x + C

Armed with this antiderivative we may return to the task of evaluating the improper integral.

∫ (^) ∞

0

2 e −x sin x dx = lim R→∞

∫ (^) R

0

2 e −x sin x dx

= lim R→∞

( −e −x cos x − e −x sin x

∣ ∣ ∣

R

0

)

= lim R→∞

( −e −R cos R − e −R sin R + 1

)

= 1 − lim R→∞

( e −R cos R + e −R sin R

)

= 1 − lim R→∞

( cos R

eR^

sin R

eR

)

Note that the last limit was evaluated by use of the Squeeze Theorem.

∫ (^1)

0

(− ln x) dx

This integral is improper since the integrand is discontinuous at x = 0.

∫ (^1)

0

(− ln x) dx = lim R→ 0 +

∫ (^1)

R

(− ln x) dx

= lim R→ 0 +

( −x ln x + x| 1 R

)

= lim R→ 0 +^

(1 − (−R ln R + R))

= lim R→ 0 +^

(1 + R ln R − R))

= 1 + lim R→ 0 +

(R ln R)

= 1 + lim R→ 0 +

ln R 1 R