BC Calculus : MC Integration Practice
Class: 5H: BC Calculus
Author: Peter Atlas
Text:
Calculus
Finney, Demana, Waits, Kennedy
\( \displaystyle \int_{-1}^{1} (x^2 - x - 1) \, dx = \)
\(\frac{2}{3}\)
0
\(-\frac{4}{3}\)
-2
-1
Solution
C
\( \displaystyle \int_{1}^{2} \frac{3x - 1}{3x} \, dx = \)
\(\frac{3}{4}\)
\( 1 - \frac{1}{3}\ln{2} \)
\(1 - \ln{ 2}\)
-\(\frac{1}{3}\ln{ 2}\)
1
Solution
B
\( \displaystyle \int_{0}^{3} \frac{dt}{\sqrt{4 - t}} = \)
1
-2
4
-1
2
Solution
E
\( \displaystyle \int_{-1}^{0} \sqrt{3u + 4} \, du = \)
2
\(\frac{14}{9}\)
\(\frac{4}{3}\)
6
\(\frac{7}{2}\)
Solution
B
\( \displaystyle \int_{2}^{3} \frac{dy}{2y - 3} = \)
\( \ln{ 3}\)
\(\frac{1}{2} \ln{ \left( \frac{3}{2} \right) } \)
\(\frac{16}{9}\)
\(\frac{1}{2}\ln{3}\)
\(\sqrt{3} - 1\)
Solution
D
\( \displaystyle \int_{0}^{\sqrt{3}} \frac{x dx}{ \sqrt{4 - x^2}} = \)
1
\( \frac{\pi }{6}\)
\( \frac{ \pi}{3} \)
-1
2
Solution
A
\( \displaystyle \int_{0}^{1} (2t - 1)^3 \, dt = \)
\frac{1}{4}
6
\(\frac{1}{2}\)
0
4
Solution
D
\( \displaystyle \int_{0}^{1} \frac{dx}{\sqrt{4 - x^2}} = \)
\(\frac{ \pi}{3}\)
\(2 -\sqrt{3}\)
\( \frac{ \pi}{12}\)
\(2( \sqrt{3} - 2)\)
\( \frac{\pi }{6}\)
Solution
E
\( \displaystyle \int_{4}^{9} \frac{(2 + x) dx}{2 \sqrt{x}} = \)
\(\frac{25}{3}\)
\(\frac{41}{3}\)
\(\frac{100}{3}\)
\(\frac{5}{3}\)
\(\frac{1}{3}\)
Solution
A
\( \displaystyle \int_{-3}^{3} \frac{dx}{9 + x^2} = \)
\(\frac{ \pi}{2}\)
0
\( \frac{\pi }{6}\)
\(- \frac{ \pi}{2} \)
\(\frac{ \pi}{3}\)
Solution
C
\( \displaystyle \int_{0}^{1}e^{-x} \, dx = \)
\( \frac{1}{e} - 1\)
\(1 - e\)
\(- \frac{1}{e}\)
\(1 - \frac{1}{e} \)
\( \frac{1}{e}\)
Solution
D
\( \displaystyle \int_{0}^{1} xe^{x^2} \, dx = \)
\(e - 1\)
\(\frac{1}{2}(e - 1)\)
\(2(e - 1)\)
\(\frac{e}{2}\)
\(\frac{e}{2} - 1\)
Solution
B
\( \displaystyle \int_{0}^{ \frac{ \pi}{4} }\sin{(2\theta )} \, d\theta = \)
2
\(\frac{1}{2}\)
-1
\(-\frac{1}{2}\)
-2
Solution
B
\( \displaystyle \int_{1}^{2} \frac{dz}{3 - z} = \)
\(-\ln{2} \)
\(\frac{3}{4} \)
\(2(\sqrt{2} - 1) \)
\(\frac{1}{2}\ln{ 2} \)
\(\ln{ 2} \)
Solution
E
\( \displaystyle \int_{1}^{e} \ln{ y} \, dy = \)
\(2e + 1\)
\(\frac{1}{2}\)
1
\(e - 1\)
-1
Solution
C
\( \displaystyle \int_{-4}^{4} \sqrt{16 - x^2} \, dx = \)
\(8 \pi \)
\(4 \pi \)
4
8
none of these
Solution
A
\( \displaystyle \int_{0}^{ \pi } \cos^2{\theta }\sin{ \theta } \, d\theta = \)
\(-\frac{2}{3}\)
\(\frac{1}{3}\)
1
\(\frac{2}{3}\)
0
Solution
D
\( \displaystyle \int_{1}^{e} \frac{\ln{ x}}{ x} \, dx = \)
\(\frac{1}{2}\)
\(\frac{1}{2}(e^2 - 1)\)
0
1
\(e - 1\)
Solution
A
\( \displaystyle \int_{0}^{1} xe^x \, dx = \)
-1
\(e + 1 \)
1
\(e - 1 \)
\(\frac{1}{2}(e - 1) \)
Solution
C
\( \displaystyle \int_{0}^{ \frac{\pi }{6}} \frac{\cos {\theta } }{1 + 2 \sin {\theta}} \, d\theta = \)
\(\ln{ 2}\)
\(\frac{3}{8}\)
\(-\frac{1}{2}\ln{ 2}\)
\(\frac{3}{2}\)
\(\ln{ \sqrt{2}}\)
Solution
E
\( \displaystyle \int_{\sqrt{2}}^{2} \frac{u}{u^2 - 1} \, du = \)
\(\ln{ \sqrt{3}}\)
\(\frac{8}{9}\)
\(\ln{ \frac{3}{2}}\)
\(\ln{ 3}\)
\(1 - \sqrt{3}\)
Solution
A
\( \displaystyle \int_{\sqrt{2}}^{2} \frac{u}{(u^2 - 1)^2} \, du = \)
\(-\frac{1}{3}\)
\(-\frac{2}{3}\)
\(\frac{2}{3}\)
-1
\(\frac{1}{3}\)
Solution
E
\( \displaystyle \int_{ \frac{ \pi}{12}}^{ \frac{ \pi}{4}} \frac{\cos {(2x)} }{\sin^2 {(2x)}} = \)
\(-\frac{1}{4}\)
1
\(\frac{1}{2}\)
\(-\frac{1}{2}\)
-1
Solution
C
\( \displaystyle \int_{0}^{1} \frac{e^{-x} + 1}{ e^{-x}} \, dx = \)
\(e\)
\(2 + e\)
\( \frac{1}{e}\)
\(1 + e\)
\(e - 1\)
Solution
A
\( \displaystyle \int_{0}^{1} \frac{ e^x dx}{e^x + 1} = \)
\(\ln{ 2}\)
\(e\)
\(1 + e\)
\(-\ln{ 2|}\)
\(\ln{ \left( \frac{e + 1}{2} \right) }\)
Solution
E
If the substitution \( u = \sqrt{x + 1}\) is used, then \( \displaystyle \int_{0}^{3} \frac{dx}{x\sqrt{x + 1}}\) is equivalent to
\( \displaystyle \int_{1}^{2} \frac{du}{u^2 - 1}\)
\( \displaystyle \int_{1}^{2} \frac{2du}{u^2 - 1}\)
\(2 \displaystyle \int_{0}^{3} \frac{du}{(u - 1)(u + 1)}\)
\(2 \displaystyle \int_{1}^{2} \frac{du}{u(u^2 - 1)}\)
\(2 \displaystyle \int_{0}^{3} \frac{du}{u(u - 1)}\)
Solution
B