Answer on Question #52103 - Math - Integral Calculus
Integrate with respect to x x x : ∫ − 1 3 x 7 + x 2 d x \int_{-1}^{3} \frac{x}{7 + x^2} dx ∫ − 1 3 7 + x 2 x d x
Solution
∫ − 1 3 x 7 + x 2 d x = 1 2 ∫ − 1 3 1 7 + x 2 d ( x 2 + 7 ) = ∣ substitution t = x 2 + 7 , d t t = d ( ln ( t ) ) ∣ = 1 2 ln ( x 2 + 7 ) ∣ − 1 3 = 1 2 ( ln ( 3 2 + 7 ) − ln ( ( − 1 ) 2 + 7 ) ) = 1 2 ln ( 3 2 + 7 ( − 1 ) 2 + 7 ) = ln 2 2 . \begin{aligned}
\int_{-1}^{3} \frac{x}{7 + x^2} dx &= \frac{1}{2} \int_{-1}^{3} \frac{1}{7 + x^2} d(x^2 + 7) = \left| \text{substitution } t = x^2 + 7, \quad \frac{dt}{t} = d(\ln(t)) \right| \\
&= \frac{1}{2} \ln(x^2 + 7) \Big|_{-1}^{3} = \frac{1}{2} \big( \ln(3^2 + 7) - \ln((-1)^2 + 7) \big) = \frac{1}{2} \ln \left( \frac{3^2 + 7}{(-1)^2 + 7} \right) = \frac{\ln 2}{2}.
\end{aligned} ∫ − 1 3 7 + x 2 x d x = 2 1 ∫ − 1 3 7 + x 2 1 d ( x 2 + 7 ) = ∣ ∣ substitution t = x 2 + 7 , t d t = d ( ln ( t )) ∣ ∣ = 2 1 ln ( x 2 + 7 ) ∣ ∣ − 1 3 = 2 1 ( ln ( 3 2 + 7 ) − ln (( − 1 ) 2 + 7 ) ) = 2 1 ln ( ( − 1 ) 2 + 7 3 2 + 7 ) = 2 ln 2 .
Answer: ln 2 2 \frac{\ln 2}{2} 2 l n 2 .
∫ 1 4 ( x + 1 x ) d x \int_{1}^{4} \left( x + \frac{1}{\sqrt{x}} \right) dx ∫ 1 4 ( x + x 1 ) d x Solution
∫ 1 4 ( x + 1 x ) d x = ∫ 1 4 x d x + ∫ 1 4 1 x d x = x 2 2 ∣ 1 4 + 2 ∫ 1 4 1 2 x d x = 4 2 2 − 1 2 2 + 2 ∫ 1 4 d x = 15 2 + 2 x ∣ 1 4 = = 15 2 + 2 ( 4 − 1 ) = 15 2 + 2 ( 2 − 1 ) = 15 2 + 2 = 19 2 = 9.5. \begin{aligned}
\int_{1}^{4} \left( x + \frac{1}{\sqrt{x}} \right) dx &= \int_{1}^{4} x \, dx + \int_{1}^{4} \frac{1}{\sqrt{x}} dx = \frac{x^2}{2} \Big|_{1}^{4} + 2 \int_{1}^{4} \frac{1}{2\sqrt{x}} dx = \frac{4^2}{2} - \frac{1^2}{2} + 2 \int_{1}^{4} d\sqrt{x} = \frac{15}{2} + 2\sqrt{x} \Big|_{1}^{4} = \\
&= \frac{15}{2} + 2(\sqrt{4} - \sqrt{1}) = \frac{15}{2} + 2(2 - 1) = \frac{15}{2} + 2 = \frac{19}{2} = 9.5.
\end{aligned} ∫ 1 4 ( x + x 1 ) d x = ∫ 1 4 x d x + ∫ 1 4 x 1 d x = 2 x 2 ∣ ∣ 1 4 + 2 ∫ 1 4 2 x 1 d x = 2 4 2 − 2 1 2 + 2 ∫ 1 4 d x = 2 15 + 2 x ∣ ∣ 1 4 = = 2 15 + 2 ( 4 − 1 ) = 2 15 + 2 ( 2 − 1 ) = 2 15 + 2 = 2 19 = 9.5.
Answer: 9.5.
Integrate with respect to x x x : ∫ sec x ⋅ tan x d x \int \sec x \cdot \tan x \, dx ∫ sec x ⋅ tan x d x .
Solution
Method 1 (substitution).
∫ sec x ⋅ tan x d x = ∫ sin x cos 2 x d x = ∣ u = sec x , d u = d ( 1 cos x ) = − − sin x cos 2 x d x = sec x ⋅ tan x d x ∣ = ∫ d u = u + C = sec x + C , where C is an arbitrary real constant . \int \sec x \cdot \tan x \, dx = \int \frac{\sin x}{\cos^2 x} dx = \left| u = \sec x, \, du = d\left(\frac{1}{\cos x}\right) = - \frac{-\sin x}{\cos^2 x} dx = \sec x \cdot \tan x \, dx \right| = \int du = u + C = \sec x + C, \text{ where } C \text{ is an arbitrary real constant}. ∫ sec x ⋅ tan x d x = ∫ cos 2 x sin x d x = ∣ ∣ u = sec x , d u = d ( cos x 1 ) = − cos 2 x − sin x d x = sec x ⋅ tan x d x ∣ ∣ = ∫ d u = u + C = sec x + C , where C is an arbitrary real constant . Method 2 (integration by parts).
∫ sec ( x ) ⋅ tan ( x ) d x = ∫ sin ( x ) cos 2 ( x ) d x = ∫ sin ( x ) d ( tan ( x ) ) = ∣ u = sin ( x ) , d v = d ( tan ( x ) ) , d u = cos ( x ) d x , v = tan ( x ) ∣ = sin ( x ) tan ( x ) − ∫ tan ( x ) cos ( x ) d x = sin 2 ( x ) cos ( x ) − ∫ sin ( x ) d x = = sin 2 ( x ) cos ( x ) + cos ( x ) + C = sin 2 ( x ) + cos 2 ( x ) cos ( x ) + C = 1 cos ( x ) + C = sec ( x ) + C , \begin{aligned}
\int \sec(x) \cdot \tan(x) \, dx &= \int \frac{\sin(x)}{\cos^2(x)} dx = \int \sin(x) d(\tan(x)) = |u = \sin(x), \, dv = d(\tan(x)), \, du = \cos(x) \, dx, \, v = \tan(x)| = \sin(x) \tan(x) - \int \tan(x) \cos(x) \, dx = \frac{\sin^2(x)}{\cos(x)} - \int \sin(x) \, dx = \\
&= \frac{\sin^2(x)}{\cos(x)} + \cos(x) + C = \frac{\sin^2(x) + \cos^2(x)}{\cos(x)} + C = \frac{1}{\cos(x)} + C = \sec(x) + C,
\end{aligned} ∫ sec ( x ) ⋅ tan ( x ) d x = ∫ cos 2 ( x ) sin ( x ) d x = ∫ sin ( x ) d ( tan ( x )) = ∣ u = sin ( x ) , d v = d ( tan ( x )) , d u = cos ( x ) d x , v = tan ( x ) ∣ = sin ( x ) tan ( x ) − ∫ tan ( x ) cos ( x ) d x = cos ( x ) sin 2 ( x ) − ∫ sin ( x ) d x = = cos ( x ) sin 2 ( x ) + cos ( x ) + C = cos ( x ) sin 2 ( x ) + cos 2 ( x ) + C = cos ( x ) 1 + C = sec ( x ) + C ,
where C C C is an arbitrary real constant.
Answer: sec x + C \sec x + C sec x + C .
Integrate with respect to x x x : ∫ csc 2 x d x \int \csc 2x \, dx ∫ csc 2 x d x .
Solution
First we use Trigonometric Identity, namely Reciprocal Identity: csc x = 1 sin x \csc x = \frac{1}{\sin x} csc x = s i n x 1 . So, csc 2 x = 1 sin 2 x \csc 2x = \frac{1}{\sin 2x} csc 2 x = s i n 2 x 1 .
∫ csc 2 x d x = ∫ 1 sin 2 x d x . \int \csc 2x \, dx = \int \frac{1}{\sin 2x} \, dx. ∫ csc 2 x d x = ∫ sin 2 x 1 d x . Method 1.
Let's multiply and divine the integrand, i.e. the function that is to be integrated, 1 sin 2 x \frac{1}{\sin 2x} s i n 2 x 1 by sin 2 x \sin 2x sin 2 x :
∫ 1 sin 2 x d x = ∫ sin 2 x sin 2 2 x d x = ∣ Pythadorean identity sin 2 2 x = 1 − cos 2 2 x ∣ = ∫ sin 2 x 1 − cos 2 2 x d x = − 1 2 ∫ d cos 2 x 1 − cos 2 2 x = ∣ t = cos 2 x ∣ = − 1 2 ∫ d t 1 − t 2 = ∣ 1 1 − t 2 = 1 ( 1 − t ) ( 1 + t ) = 1 2 ( 1 1 − t + 1 1 + t ) ∣ = = − 1 4 ∫ d t 1 − t − 1 4 ∫ d t 1 + t = 1 4 ∫ d t t − 1 − 1 4 ∫ d t t + 1 = − 1 4 ln ∣ t + 1 t − 1 ∣ + C = 1 4 ln ∣ 1 − t ∣ − 1 4 ln ∣ 1 + t ∣ + c = 1 4 ln ∣ 1 − t 1 + t ∣ + c . \begin{aligned}
\int \frac{1}{\sin 2x} \, dx &= \int \frac{\sin 2x}{\sin^2 2x} \, dx = \left| \frac{\text{Pythadorean identity}}{\sin^2 2x = 1 - \cos^2 2x} \right| = \int \frac{\sin 2x}{1 - \cos^2 2x} \, dx = -\frac{1}{2} \int \frac{d \cos 2x}{1 - \cos^2 2x} \\
&= |t = \cos 2x| = -\frac{1}{2} \int \frac{dt}{1 - t^2} = \left| \frac{1}{1 - t^2} = \frac{1}{(1 - t)(1 + t)} = \frac{1}{2} \left( \frac{1}{1 - t} + \frac{1}{1 + t} \right) \right| = \\
&= -\frac{1}{4} \int \frac{dt}{1 - t} - \frac{1}{4} \int \frac{dt}{1 + t} = \frac{1}{4} \int \frac{dt}{t - 1} - \frac{1}{4} \int \frac{dt}{t + 1} = -\frac{1}{4} \ln \left| \frac{t + 1}{t - 1} \right| + C = \frac{1}{4} \ln |1 - t| - \frac{1}{4} \ln |1 + t| + c \\
&= \frac{1}{4} \ln \left| \frac{1 - t}{1 + t} \right| + c.
\end{aligned} ∫ sin 2 x 1 d x = ∫ sin 2 2 x sin 2 x d x = ∣ ∣ sin 2 2 x = 1 − cos 2 2 x Pythadorean identity ∣ ∣ = ∫ 1 − cos 2 2 x sin 2 x d x = − 2 1 ∫ 1 − cos 2 2 x d cos 2 x = ∣ t = cos 2 x ∣ = − 2 1 ∫ 1 − t 2 d t = ∣ ∣ 1 − t 2 1 = ( 1 − t ) ( 1 + t ) 1 = 2 1 ( 1 − t 1 + 1 + t 1 ) ∣ ∣ = = − 4 1 ∫ 1 − t d t − 4 1 ∫ 1 + t d t = 4 1 ∫ t − 1 d t − 4 1 ∫ t + 1 d t = − 4 1 ln ∣ ∣ t − 1 t + 1 ∣ ∣ + C = 4 1 ln ∣1 − t ∣ − 4 1 ln ∣1 + t ∣ + c = 4 1 ln ∣ ∣ 1 + t 1 − t ∣ ∣ + c .
Thus,
∫ csc 2 x d x = 1 4 ln ∣ 1 − cos 2 x 1 + cos 2 x ∣ + c = 1 4 ln ∣ 2 sin 2 ( x ) 2 cos 2 ( x ) ∣ + c = 1 4 ln ∣ tan 2 ( x ) ∣ + c = 1 2 ln ∣ tan ( x ) ∣ + c \int \csc 2x \, dx = \frac{1}{4} \ln \left| \frac{1 - \cos 2x}{1 + \cos 2x} \right| + c = \frac{1}{4} \ln \left| \frac{2 \sin^2(x)}{2 \cos^2(x)} \right| + c = \frac{1}{4} \ln |\tan^2(x)| + c = \frac{1}{2} \ln |\tan(x)| + c ∫ csc 2 x d x = 4 1 ln ∣ ∣ 1 + c o s 2 x 1 − c o s 2 x ∣ ∣ + c = 4 1 ln ∣ ∣ 2 c o s 2 ( x ) 2 s i n 2 ( x ) ∣ ∣ + c = 4 1 ln ∣ tan 2 ( x ) ∣ + c = 2 1 ln ∣ tan ( x ) ∣ + c , where c c c is an arbitrary real constant.
Method 2.
∫ 1 sin 2 x d x = ∫ d x 2 sin ( x ) cos ( x ) = ∣ divide the numerator and denominator by cos 2 ( x ) ∣ = ∫ d x cos 2 ( x ) 2 sin ( x ) cos ( x ) cos 2 ( x ) = 1 2 ∫ d ( tan ( x ) ) tan ( x ) = ∣ y = tan ( x ) ∣ = 1 2 ∫ d y y = 1 2 ln ∣ y ∣ + c = 1 2 ln ∣ tan ( x ) ∣ + c , where c is an arbitrary real constant . \begin{aligned}
\int \frac{1}{\sin 2x} \, dx &= \int \frac{dx}{2 \sin(x) \cos(x)} = \left| \text{divide the numerator and denominator by } \cos^2(x) \right| = \int \frac{\frac{dx}{\cos^2(x)}}{\frac{2 \sin(x) \cos(x)}{\cos^2(x)}} = \\
&\frac{1}{2} \int \frac{d(\tan(x))}{\tan(x)} = |y = \tan(x)| = \frac{1}{2} \int \frac{dy}{y} = \frac{1}{2} \ln |y| + c = \frac{1}{2} \ln |\tan(x)| + c, \text{ where } c \text{ is an arbitrary real constant}.
\end{aligned} ∫ sin 2 x 1 d x = ∫ 2 sin ( x ) cos ( x ) d x = ∣ ∣ divide the numerator and denominator by cos 2 ( x ) ∣ ∣ = ∫ c o s 2 ( x ) 2 s i n ( x ) c o s ( x ) c o s 2 ( x ) d x = 2 1 ∫ tan ( x ) d ( tan ( x )) = ∣ y = tan ( x ) ∣ = 2 1 ∫ y d y = 2 1 ln ∣ y ∣ + c = 2 1 ln ∣ tan ( x ) ∣ + c , where c is an arbitrary real constant .
Answer: 1 2 ln ∣ tan ( x ) ∣ + c \frac{1}{2} \ln |\tan(x)| + c 2 1 ln ∣ tan ( x ) ∣ + c
Integrate with respect to x x x : ∫ sin x d x \int \sin x \, dx ∫ sin x d x .
Solution
∫ sin x d x = − cos x + C , C ∈ R . \int \sin x \, dx = -\cos x + C, C \in \mathbb{R}. ∫ sin x d x = − cos x + C , C ∈ R .
Answer: − cos x + C -\cos x + C − cos x + C .
Integrate with respect to Q Q Q : ∫ 0 π ( 2 sin Q − 5 cos Q ) d Q \int_0^\pi (2 \sin Q - 5 \cos Q) \, dQ ∫ 0 π ( 2 sin Q − 5 cos Q ) d Q .
Solution
∫ 0 π 3 ( 2 sin Q − 5 cos Q ) d Q = ( − 2 cos Q − 5 sin Q ) ∣ π 3 0 ∣ = − 2 ⋅ 1 2 − 5 ⋅ 3 2 + 2 − 0 = 1 − 5 3 2 = 2 − 5 3 2 ≈ − 3.33013. \begin{aligned}
\int_0^{\frac{\pi}{3}} (2 \sin Q - 5 \cos Q) \, dQ &= (-2 \cos Q - 5 \sin Q) \left| \begin{array}{c} \frac{\pi}{3} \\ 0 \end{array} \right| = -2 \cdot \frac{1}{2} - 5 \cdot \frac{\sqrt{3}}{2} + 2 - 0 = 1 - \frac{5\sqrt{3}}{2} = \frac{2 - 5\sqrt{3}}{2} \\
&\approx -3.33013.
\end{aligned} ∫ 0 3 π ( 2 sin Q − 5 cos Q ) d Q = ( − 2 cos Q − 5 sin Q ) ∣ ∣ 3 π 0 ∣ ∣ = − 2 ⋅ 2 1 − 5 ⋅ 2 3 + 2 − 0 = 1 − 2 5 3 = 2 2 − 5 3 ≈ − 3.33013.
Answer: 2 − 5 3 2 ≈ − 3.33013 \frac{2 - 5\sqrt{3}}{2} \approx -3.33013 2 2 − 5 3 ≈ − 3.33013 .
Integrate with respect to v v v : ∫ 63 1 ( 4 v − 2 ) d v \int_{63}^{1}(4v - 2) \, dv ∫ 63 1 ( 4 v − 2 ) d v
Solution
Method 1
∫ 63 1 ( 4 v − 2 ) d v = ( 4 v 2 2 − 2 v ) ∣ 63 1 = ( 4 1 2 2 − 2 ⋅ 1 ) − ( 4 6 3 2 2 − 2 ⋅ 63 ) = − 7812. \int_{63}^{1} (4v - 2)dv = \left(4 \frac{v^2}{2} - 2v\right) \Big|_{63}^{1} = \left(4 \frac{1^2}{2} - 2 \cdot 1\right) - \left(4 \frac{63^2}{2} - 2 \cdot 63\right) = -7812. ∫ 63 1 ( 4 v − 2 ) d v = ( 4 2 v 2 − 2 v ) ∣ ∣ 63 1 = ( 4 2 1 2 − 2 ⋅ 1 ) − ( 4 2 6 3 2 − 2 ⋅ 63 ) = − 7812. Method 2
∫ 63 1 ( 4 v − 2 ) d v = 1 4 ∫ 63 1 ( 4 v − 2 ) d ( 4 v − 2 ) = ∣ substitution t = 4 v − 2 , t ( 63 ) = 250 , t ( 1 ) = 2 ∣ = 1 4 ∫ 250 2 t d t = 1 4 t 2 2 ∣ 250 2 = 1 8 ( 2 2 − 25 0 2 ) = − 7812 \begin{aligned}
\int_{63}^{1} (4v - 2)dv &= \frac{1}{4} \int_{63}^{1} (4v - 2) d(4v - 2) = \left| \text{substitution } t = 4v - 2, t(63) = 250, t(1) = 2 \right| \\
&= \frac{1}{4} \int_{250}^{2} t dt = \left. \frac{1}{4} \frac{t^2}{2} \right|_{250}^{2} = \frac{1}{8} (2^2 - 250^2) = -7812
\end{aligned} ∫ 63 1 ( 4 v − 2 ) d v = 4 1 ∫ 63 1 ( 4 v − 2 ) d ( 4 v − 2 ) = ∣ substitution t = 4 v − 2 , t ( 63 ) = 250 , t ( 1 ) = 2 ∣ = 4 1 ∫ 250 2 t d t = 4 1 2 t 2 ∣ ∣ 250 2 = 8 1 ( 2 2 − 25 0 2 ) = − 7812
Answer: -7812.
Integrate with respect to x x x : ∫ 0 1 ( 7 − 4 x ) 2 d x \int_0^1 (7 - 4x)^2 dx ∫ 0 1 ( 7 − 4 x ) 2 d x .
Solution
Method 1.
∫ 0 1 ( 7 − 4 x ) 2 d x = ∫ 0 1 ( 49 − 56 x + 16 x 2 ) d x = 49 x − 28 x 2 + 16 x 3 3 ∣ 0 1 = 79 3 . \int_{0}^{1} (7 - 4x)^2 dx = \int_{0}^{1} (49 - 56x + 16x^2) dx = 49x - 28x^2 + \frac{16x^3}{3} \Big|_{0}^{1} = \frac{79}{3}. ∫ 0 1 ( 7 − 4 x ) 2 d x = ∫ 0 1 ( 49 − 56 x + 16 x 2 ) d x = 49 x − 28 x 2 + 3 16 x 3 ∣ ∣ 0 1 = 3 79 . Method 2.
∫ 0 1 ( 7 − 4 x ) 2 d x = − 1 4 ∫ 0 1 ( 7 − 4 x ) 2 d ( 7 − 4 x ) = ∣ substitution t = 7 − 4 x , t ( 0 ) = 7 , t ( 1 ) = 3 ∣ = − 1 4 ∫ 7 3 t 2 d t = − 1 4 t 3 3 ∣ 7 3 = − 1 12 ( 3 3 − 7 3 ) = 316 12 = 79 3 \begin{aligned}
\int_{0}^{1} (7 - 4x)^2 dx &= - \frac{1}{4} \int_{0}^{1} (7 - 4x)^2 d(7 - 4x) = \left| \text{substitution } t = 7 - 4x, t(0) = 7, t(1) = 3 \right| \\
&= - \frac{1}{4} \int_{7}^{3} t^2 dt = - \left. \frac{1}{4} \frac{t^3}{3} \right|_{7}^{3} = - \frac{1}{12} (3^3 - 7^3) = \frac{316}{12} = \frac{79}{3}
\end{aligned} ∫ 0 1 ( 7 − 4 x ) 2 d x = − 4 1 ∫ 0 1 ( 7 − 4 x ) 2 d ( 7 − 4 x ) = ∣ substitution t = 7 − 4 x , t ( 0 ) = 7 , t ( 1 ) = 3 ∣ = − 4 1 ∫ 7 3 t 2 d t = − 4 1 3 t 3 ∣ ∣ 7 3 = − 12 1 ( 3 3 − 7 3 ) = 12 316 = 3 79
Answer: 79 3 \frac{79}{3} 3 79 .
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