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CBSE - Class 12 Mathematics Integrals Worksheet
EXERCISE 7.8
Worksheet Answers
Solution:
To evaluate the definite integral $I = \int_{0}^{\frac{\pi}{2}} \cos 2x \, dx$, we employ the Fundamental Theorem of Calculus (Part II). This theorem states that if $F(x)$ is the antiderivative of $f(x)$, then $\int_{a}^{b} f(x) \, dx = F(b) - F(a)$. [Fundamental Theorem of Calculus].
We identify the integrand $f(x) = \cos 2x$. To find the antiderivative $F(x)$, we apply the method of integration by substitution or the reverse chain rule for trigonometric functions. Since $\frac{d}{dx}(\sin(kx)) = k \cos(kx)$, it follows that $\int \cos(kx) \, dx = \frac{1}{k} \sin(kx) + C$.
Setting $k = 2$: $F(x) = \int \cos 2x \, dx = \frac{\sin 2x}{2}$
Substituting the upper limit $b = \frac{\pi}{2}$ and the lower limit $a = 0$ into the antiderivative:
$I = \left[ \frac{\sin 2x}{2} \right]_{0}^{\frac{\pi}{2}}$
$I = \frac{1}{2} \left[ \sin\left(2 \cdot \frac{\pi}{2}\right) - \sin(2 \cdot 0) \right]$
Evaluate the trigonometric terms:
$I = \frac{1}{2} [0 - 0] = 0$
The integral represents the net signed area between the curve $y = \cos 2x$ and the $x$-axis from $0$ to $\frac{\pi}{2}$. Because the area from $0$ to $\frac{\pi}{4}$ (positive) exactly cancels the area from $\frac{\pi}{4}$ to $\frac{\pi}{2}$ (negative), the result is zero.
Final Solution: $\int_{0}^{\frac{\pi}{2}} \cos 2x \, dx = 0$
Solution:
Given the definite integral: $I = \int_{0}^{\frac{\pi}{4}} (2\sec^2 x + x^3 + 2) \, dx$.
By the Linearity Property of Integration [$\int_{a}^{b} [f(x) + g(x)] dx = \int_{a}^{b} f(x) dx + \int_{a}^{b} g(x) dx$], we decompose the expression into three distinct integrable terms:
$I = 2 \int_{0}^{\frac{\pi}{4}} \sec^2 x \, dx + \int_{0}^{\frac{\pi}{4}} x^3 \, dx + 2 \int_{0}^{\frac{\pi}{4}} 1 \, dx$
We apply the Fundamental Theorem of Calculus Part II: $\int_{a}^{b} f(x) dx = F(b) - F(a)$, where $F'(x) = f(x)$.
Applying the limits $[0, \frac{\pi}{4}]$ to each term:
$I = 2[\tan x]_{0}^{\frac{\pi}{4}} + \left[ \frac{x^4}{4} \right]_{0}^{\frac{\pi}{4}} + 2[x]_{0}^{\frac{\pi}{4}}$
Calculating the values:
Summing the results obtained in Step 3:
$I = 2 + \frac{\pi^4}{1024} + \frac{\pi}{2}$
Final Solution: $2 + \frac{\pi}{2} + \frac{\pi^4}{1024}$
Solution:
To evaluate the definite integral $\int_{\frac{\pi}{6}}^{\frac{\pi}{4}} \csc x \, dx$, we utilize the standard integral formula for the cosecant function. The antiderivative of $\csc x$ is given by:
$\int \csc x \, dx = \ln |\csc x - \cot x| + C$ [Standard Integral Calculus Identity]
By the Fundamental Theorem of Calculus, Part II, if $F(x)$ is the antiderivative of $f(x)$, then:
$\int_{a}^{b} f(x) \, dx = F(b) - F(a)$
Substituting our limits $a = \frac{\pi}{6}$ and $b = \frac{\pi}{4}$:
$\int_{\frac{\pi}{6}}^{\frac{\pi}{4}} \csc x \, dx = \left[ \ln |\csc x - \cot x| \right]_{\frac{\pi}{6}}^{\frac{\pi}{4}}$
Substitute the upper limit $x = \frac{\pi}{4}$:
$F(\frac{\pi}{4}) = \ln |\csc(\frac{\pi}{4}) - \cot(\frac{\pi}{4})| = \ln |\sqrt{2} - 1|$
[Using trigonometric ratios: $\csc(\frac{\pi}{4}) = \sqrt{2}$, $\cot(\frac{\pi}{4}) = 1$]
Substitute the lower limit $x = \frac{\pi}{6}$:
$F(\frac{\pi}{6}) = \ln |\csc(\frac{\pi}{6}) - \cot(\frac{\pi}{6})| = \ln |2 - \sqrt{3}|$
[Using trigonometric ratios: $\csc(\frac{\pi}{6}) = 2$, $\cot(\frac{\pi}{6}) = \sqrt{3}$]
Subtracting the values:
Result $= \ln |\sqrt{2} - 1| - \ln |2 - \sqrt{3}|$
Using the logarithmic quotient rule $\ln(a) - \ln(b) = \ln(\frac{a}{b})$:
Result $= \ln \left| \frac{\sqrt{2} - 1}{2 - \sqrt{3}} \right|$
Rationalize the denominator to simplify the expression:
$\frac{\sqrt{2} - 1}{2 - \sqrt{3}} \times \frac{2 + \sqrt{3}}{2 + \sqrt{3}} = \frac{2\sqrt{2} + \sqrt{6} - 2 - \sqrt{3}}{4 - 3} = 2\sqrt{2} + \sqrt{6} - 2 - \sqrt{3}$
Final Solution: \ln \left| \frac{\sqrt{2} - 1}{2 - \sqrt{3}} \right| \text{ or } \ln(2\sqrt{2} + \sqrt{6} - 2 - \sqrt{3})
Solution:
To evaluate the integral $I = \int_{0}^{\pi} (\sin^2 \frac{x}{2} - \cos^2 \frac{x}{2}) \, dx$, we first simplify the integrand using the double-angle identity for cosine: $\cos(2\theta) = \cos^2 \theta - \sin^2 \theta$.
By rearranging the given integrand:
$\sin^2 \frac{x}{2} - \cos^2 \frac{x}{2} = -(\cos^2 \frac{x}{2} - \sin^2 \frac{x}{2})$
Applying the identity with $\theta = \frac{x}{2}$:
$-(\cos(2 \cdot \frac{x}{2})) = -\cos(x)$
[By Trigonometric Identity: $\cos(2A) = \cos^2 A - \sin^2 A$]
Substitute the simplified expression back into the definite integral:
$I = \int_{0}^{\pi} -\cos(x) \, dx$
$I = -\int_{0}^{\pi} \cos(x) \, dx$
The integral of $\cos(x)$ with respect to $x$ is $\sin(x)$. [Per the Fundamental Theorem of Calculus Part II, if $F'(x) = f(x)$, then $\int_{a}^{b} f(x)dx = F(b) - F(a)$].
$I = -[\sin(x)]_{0}^{\pi}$
Apply the limits of integration ($0$ and $\pi$):
$I = -(\sin(\pi) - \sin(0))$
Evaluating the trigonometric values:
$\sin(\pi) = 0$
$\sin(0) = 0$
$I = -(0 - 0) = 0$
Final Solution: $0$
Solution:
The integral of the trigonometric function $\tan x$ is a fundamental antiderivative derived from the logarithmic form of the natural logarithm of the secant function. [Per the Fundamental Theorem of Calculus, $\int_{a}^{b} f(x) dx = F(b) - F(a)$ where $F'(x) = f(x)$].
The indefinite integral is defined as:
$\int \tan x \, dx = \int \frac{\sin x}{\cos x} \, dx$
By applying the substitution method, let $u = \cos x$, then $du = -\sin x \, dx$, which implies $\sin x \, dx = -du$.
$\int \frac{-du}{u} = -\ln|u| + C = -\ln|\cos x| + C = \ln|\sec x| + C$ [Using the logarithmic property $-\ln(a) = \ln(a^{-1})$].
Applying the limits $[0, \frac{\pi}{4}]$ to the antiderivative $\ln|\sec x|$:
$I = \left[ \ln|\sec x| \right]_{0}^{\frac{\pi}{4}}$
$I = \ln|\sec(\frac{\pi}{4})| - \ln|\sec(0)|$
Given the standard trigonometric ratios:
$I = \ln|\sqrt{2}| - \ln|1|$
Since $\ln(1) = 0$ [Per the logarithmic identity $\ln(1) = 0$]:
$I = \ln(2^{1/2}) - 0$
$I = \frac{1}{2} \ln(2)$
Final Solution: $\frac{1}{2} \ln 2$
Solution:
The given definite integral is:
$I = \int_{0}^{2} \frac{6x+3}{x^2+4} dx$
By the additive property of integrals [Linearity of the integral operator], we can split the integrand into two distinct parts to simplify the integration process:
$I = \int_{0}^{2} \frac{6x}{x^2+4} dx + \int_{0}^{2} \frac{3}{x^2+4} dx$
Let $I_1 = \int_{0}^{2} \frac{6x}{x^2+4} dx$.
Use the method of $u$-substitution. Let $u = x^2 + 4$.
Then, the derivative is $\frac{du}{dx} = 2x$, which implies $du = 2x dx$.
Since the numerator is $6x dx = 3(2x dx) = 3 du$, we perform the change of limits:
$I_1 = \int_{4}^{8} \frac{3}{u} du = 3 [\ln|u|]_{4}^{8}$
$I_1 = 3 (\ln 8 - \ln 4) = 3 \ln\left(\frac{8}{4}\right) = 3 \ln 2$
Let $I_2 = \int_{0}^{2} \frac{3}{x^2+4} dx$.
We use the standard integral formula: $\int \frac{1}{x^2 + a^2} dx = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right) + C$ [Integration of rational functions].
Here, $a^2 = 4$, so $a = 2$.
$I_2 = 3 \int_{0}^{2} \frac{1}{x^2 + 2^2} dx = 3 \left[ \frac{1}{2} \tan^{-1}\left(\frac{x}{2}\right) \right]_{0}^{2}$
$I_2 = \frac{3}{2} \left[ \tan^{-1}\left(\frac{2}{2}\right) - \tan^{-1}\left(\frac{0}{2}\right) \right]$
$I_2 = \frac{3}{2} (\tan^{-1}(1) - \tan^{-1}(0)) = \frac{3}{2} \left( \frac{\pi}{4} - 0 \right) = \frac{3\pi}{8}$
The total integral is the sum of $I_1$ and $I_2$:
$I = 3 \ln 2 + \frac{3\pi}{8}$
Final Solution: $3 \ln 2 + \frac{3\pi}{8}$
Solution:
By the linearity property of definite integrals, we can split the given integral into two distinct parts [Per the Linearity Property of Integrals]:
$\int_{0}^{1} (x e^x + \sin \frac{\pi x}{4}) \, dx = \int_{0}^{1} x e^x \, dx + \int_{0}^{1} \sin \frac{\pi x}{4} \, dx$
To evaluate this integral, we employ the Integration by Parts formula: $\int u \, dv = uv - \int v \, du$ [Per the Integration by Parts Theorem].
Applying the formula:
$I_1 = [x e^x]_{0}^{1} - \int_{0}^{1} e^x \, dx$
$I_1 = (1 \cdot e^1 - 0 \cdot e^0) - [e^x]_{0}^{1}$
$I_1 = e - (e^1 - e^0) = e - e + 1 = 1$
We use the standard integral formula $\int \sin(ax) \, dx = -\frac{1}{a} \cos(ax) + C$ [Per the Integration of Trigonometric Functions].
$I_2 = \left[ -\frac{1}{\pi/4} \cos \frac{\pi x}{4} \right]_{0}^{1}$
$I_2 = -\frac{4}{\pi} \left[ \cos \frac{\pi(1)}{4} - \cos \frac{\pi(0)}{4} \right]$
$I_2 = -\frac{4}{\pi} \left( \cos \frac{\pi}{4} - \cos 0 \right)$
Since $\cos \frac{\pi}{4} = \frac{1}{\sqrt{2}}$ and $\cos 0 = 1$:
$I_2 = -\frac{4}{\pi} \left( \frac{1}{\sqrt{2}} - 1 \right) = \frac{4}{\pi} \left( 1 - \frac{1}{\sqrt{2}} \right)$
Combining $I_1$ and $I_2$:
Result = $1 + \frac{4}{\pi} \left( 1 - \frac{1}{\sqrt{2}} \right)$
Simplifying the expression within the parenthesis:
Result = $1 + \frac{4}{\pi} - \frac{4}{\pi\sqrt{2}} = 1 + \frac{4}{\pi} - \frac{2\sqrt{2}}{\pi}$
Final Solution: $1 + \frac{4 - 2\sqrt{2}}{\pi}$
Solution:
According to the Fundamental Theorem of Calculus, the definite integral $\int_{a}^{b} f(x) dx$ can be evaluated using the limit of a Riemann sum as $n \to \infty$:
$\int_{a}^{b} f(x) dx = \lim_{n \to \infty} h \sum_{r=0}^{n-1} f(a + rh)$
Where:
Given $f(x) = x + 1$. We evaluate $f(a + rh)$:
$f(-1 + rh) = (-1 + rh) + 1 = rh$
Substituting this into the summation formula:
$\int_{-1}^{1} (x+1) dx = \lim_{n \to \infty} \left( \frac{2}{n} \right) \sum_{r=0}^{n-1} \left( r \cdot \frac{2}{n} \right)$
Factoring out constants from the summation [Per the Summation Property $\sum c \cdot a_r = c \sum a_r$]:
$= \lim_{n \to \infty} \left( \frac{2}{n} \right) \left( \frac{2}{n} \right) \sum_{r=0}^{n-1} r$
Using the identity for the sum of the first $(n-1)$ natural numbers, $\sum_{r=0}^{n-1} r = \frac{(n-1)n}{2}$ [By Arithmetic Progression Sum formula]:
$= \lim_{n \to \infty} \frac{4}{n^2} \cdot \frac{(n-1)n}{2}$
Simplifying the expression within the limit:
$= \lim_{n \to \infty} \frac{4n(n-1)}{2n^2} = \lim_{n \to \infty} 2 \left( \frac{n^2 - n}{n^2} \right)$
$= \lim_{n \to \infty} 2 \left( 1 - \frac{1}{n} \right)$
As $n \to \infty$, $\frac{1}{n} \to 0$. Thus:
$= 2(1 - 0) = 2$
The integral represents the area of a right-angled triangle with base $b = 2$ and height $h = 2$. Area $= \frac{1}{2} \times 2 \times 2 = 2$.
Final Solution: 2
Solution:
The integral to be evaluated is $I = \int_{0}^{1} \frac{2x+3}{5x^2+1} dx$. We begin by splitting the integral into two distinct parts to handle the linear term and the constant term separately [By the Additivity Property of Integrals]:
$I = \int_{0}^{1} \frac{2x}{5x^2+1} dx + \int_{0}^{1} \frac{3}{5x^2+1} dx$
Let $I_1 = \int_{0}^{1} \frac{2x}{5x^2+1} dx$. We apply the method of substitution [By Integration by Substitution]:
Let $u = 5x^2 + 1$. Then, the derivative is $\frac{du}{dx} = 10x$, which implies $2x dx = \frac{1}{5} du$.
Adjusting the limits: When $x=0$, $u=1$. When $x=1$, $u=6$.
$I_1 = \frac{1}{5} \int_{1}^{6} \frac{1}{u} du = \frac{1}{5} [\ln|u|]_{1}^{6}$
$I_1 = \frac{1}{5} (\ln 6 - \ln 1) = \frac{\ln 6}{5}$
Let $I_2 = \int_{0}^{1} \frac{3}{5x^2+1} dx$. We factor out the constant 5 from the denominator to match the standard form $\int \frac{1}{x^2 + a^2} dx = \frac{1}{a} \tan^{-1}(\frac{x}{a})$:
$I_2 = 3 \int_{0}^{1} \frac{1}{5(x^2 + \frac{1}{5})} dx = \frac{3}{5} \int_{0}^{1} \frac{1}{x^2 + (\frac{1}{\sqrt{5}})^2} dx$
Using the standard integral formula [By the Integral of $1/(x^2+a^2)$]:
$I_2 = \frac{3}{5} \left[ \frac{1}{1/\sqrt{5}} \tan^{-1} \left( \frac{x}{1/\sqrt{5}} \right) \right]_{0}^{1}$
$I_2 = \frac{3\sqrt{5}}{5} \left[ \tan^{-1}(\sqrt{5}x) \right]_{0}^{1} = \frac{3}{\sqrt{5}} \tan^{-1}(\sqrt{5})$
Summing the two components $I = I_1 + I_2$:
$I = \frac{\ln 6}{5} + \frac{3}{\sqrt{5}} \tan^{-1}(\sqrt{5})$
Final Solution: $\frac{1}{5} \ln 6 + \frac{3}{\sqrt{5}} \tan^{-1}(\sqrt{5})$
Solution:
The given definite integral is defined as:
$I = \int_{0}^{\frac{\pi}{4}} \sin(2x) \, dx$
To evaluate the integral, we identify the antiderivative of the function $f(x) = \sin(2x)$. [Per the Fundamental Theorem of Calculus Part II].
We use the substitution method or the direct formula for linear arguments: $\int \sin(ax) \, dx = -\frac{\cos(ax)}{a} + C$.
Here, $a = 2$, therefore:
$\int \sin(2x) \, dx = -\frac{\cos(2x)}{2}$
Applying the limits of integration from $0$ to $\frac{\pi}{4}$:
$I = \left[ -\frac{\cos(2x)}{2} \right]_{0}^{\frac{\pi}{4}}$
$I = -\frac{1}{2} \left[ \cos(2x) \right]_{0}^{\frac{\pi}{4}}$
Substitute the upper and lower limits into the expression:
$I = -\frac{1}{2} \left[ \cos\left(2 \cdot \frac{\pi}{4}\right) - \cos(2 \cdot 0) \right]$
$I = -\frac{1}{2} \left[ \cos\left(\frac{\pi}{2}\right) - \cos(0) \right]$
Recall the standard trigonometric values: $\cos\left(\frac{\pi}{2}\right) = 0$ and $\cos(0) = 1$. [By definition of unit circle coordinates].
$I = -\frac{1}{2} \left[ 0 - 1 \right]$
$I = -\frac{1}{2} \left[ -1 \right]$
$I = \frac{1}{2}$
Final Solution: \frac{1}{2}
Solution:
Given the definite integral:
$$I = \int_{2}^{3} \frac{x}{x^2+1} dx$$
To evaluate this, we identify a function $f(x) = x^2 + 1$ such that its derivative $f'(x) = 2x$ is proportional to the numerator. We utilize the method of integration by substitution. [Per the Integration by Substitution Rule].
Let $u = x^2 + 1$. Then, differentiating both sides with respect to $x$ yields:
$$\frac{du}{dx} = 2x \implies du = 2x dx \implies x dx = \frac{1}{2} du$$
Since the variable of integration changes from $x$ to $u$, we must transform the limits of integration accordingly [Fundamental Theorem of Calculus]:
Substituting the variables into the integral expression:
$$I = \int_{5}^{10} \frac{1}{2} \cdot \frac{1}{u} du$$
Extracting the constant factor and applying the standard integral formula $\int \frac{1}{u} du = \ln|u| + C$:
$$I = \frac{1}{2} [\ln|u|]_{5}^{10}$$
Applying the limits [Fundamental Theorem of Calculus, Part II]:
$$I = \frac{1}{2} (\ln 10 - \ln 5)$$
Using the property $\ln a - \ln b = \ln(\frac{a}{b})$:
$$I = \frac{1}{2} \ln\left(\frac{10}{5}\right)$$
$$I = \frac{1}{2} \ln(2)$$
Final Solution: \frac{1}{2} \ln 2
Solution:
To evaluate the definite integral $\int_{a}^{b} f(x) dx$, we utilize the Fundamental Theorem of Calculus (Part II), which states:
$\int_{a}^{b} f(x) dx = F(b) - F(a)$
where $F(x)$ is the anti-derivative of the function $f(x)$ [Per the Fundamental Theorem of Calculus].
The integrand is $f(x) = \frac{1}{x}$. The standard integral for the reciprocal function is given by:
$\int \frac{1}{x} dx = \ln|x| + C$
Thus, our anti-derivative function is $F(x) = \ln|x|$.
Given the definite integral with limits $a = 2$ and $b = 3$:
$\int_{2}^{3} \frac{1}{x} dx = \left[ \ln|x| \right]_{2}^{3}$
Applying the upper and lower limits [By the definition of definite integrals]:
$= \ln|3| - \ln|2|$
Using the quotient rule for logarithms, which states $\ln(m) - \ln(n) = \ln\left(\frac{m}{n}\right)$ for $m, n > 0$ [Per Logarithmic Identity Laws]:
$= \ln\left(\frac{3}{2}\right)$
The numerical value is the natural logarithm of $1.5$.
Final Solution: $\ln\left(\frac{3}{2}\right)$ or $\ln(1.5)$
Solution:
Given the integral $I = \int_{1}^{2} \frac{5x^2}{x^2+4x+3} dx$. Since the degree of the numerator is equal to the degree of the denominator, we perform long division [Polynomial Division Theorem].
Divide $5x^2$ by $x^2 + 4x + 3$:
| $5x^2 = 5(x^2 + 4x + 3) - 20x - 15$ |
Thus, the integrand is expressed as:
$\frac{5x^2}{x^2+4x+3} = 5 - \frac{20x + 15}{x^2 + 4x + 3}$
Factorize the denominator: $x^2 + 4x + 3 = (x+1)(x+3)$. We set up the partial fractions for the remainder term:
$\frac{20x + 15}{(x+1)(x+3)} = \frac{A}{x+1} + \frac{B}{x+3}$
Multiply by $(x+1)(x+3)$: $20x + 15 = A(x+3) + B(x+1)$.
Substitute back into the integral expression:
$I = \int_{1}^{2} 5 \, dx - \int_{1}^{2} \left( \frac{-5/2}{x+1} + \frac{45/2}{x+3} \right) \, dx$
$I = \int_{1}^{2} 5 \, dx + \frac{5}{2} \int_{1}^{2} \frac{1}{x+1} \, dx - \frac{45}{2} \int_{1}^{2} \frac{1}{x+3} \, dx$
Apply the Fundamental Theorem of Calculus [$\int \frac{1}{x} dx = \ln|x|$]:
$I = [5x]_{1}^{2} + \frac{5}{2} [\ln|x+1|]_{1}^{2} - \frac{45}{2} [\ln|x+3|]_{1}^{2}$
$I = 5(2 - 1) + \frac{5}{2} (\ln 3 - \ln 2) - \frac{45}{2} (\ln 5 - \ln 4)$
$I = 5 + \frac{5}{2} \ln(\frac{3}{2}) - \frac{45}{2} \ln(\frac{5}{4})$
Using logarithm properties [$\ln a - \ln b = \ln(a/b)$ and $n \ln a = \ln a^n$]:
$I = 5 + \ln \left( \left(\frac{3}{2}\right)^{5/2} \right) - \ln \left( \left(\frac{5}{4}\right)^{45/2} \right)$
$I = 5 + \frac{5}{2} \ln 3 - \frac{5}{2} \ln 2 - \frac{45}{2} \ln 5 + \frac{45}{2} \ln 4$
Since $\ln 4 = 2 \ln 2$:
$I = 5 + \frac{5}{2} \ln 3 - \frac{5}{2} \ln 2 - \frac{45}{2} \ln 5 + 45 \ln 2$
$I = 5 + \frac{5}{2} \ln 3 + \frac{85}{2} \ln 2 - \frac{45}{2} \ln 5$
Final Solution: $5 + \frac{5}{2} \ln 3 + \frac{85}{2} \ln 2 - \frac{45}{2} \ln 5$ or $5 + \frac{5}{2} \ln\left( \frac{3 \cdot 2^{17}}{5^9} \right)$
Solution:
To evaluate the definite integral of the polynomial function $f(x) = 4x^3 - 5x^2 + 6x + 9$ over the interval $[1, 2]$, we utilize the Second Fundamental Theorem of Calculus, which states that if $F(x)$ is the antiderivative of $f(x)$, then:
$\int_{a}^{b} f(x) \, dx = F(b) - F(a)$ [Per the Fundamental Theorem of Calculus, Part II]
We apply the power rule for integration, $\int x^n \, dx = \frac{x^{n+1}}{n+1} + C$, to each term of the integrand individually:
Thus, the antiderivative is $F(x) = x^4 - \frac{5}{3}x^3 + 3x^2 + 9x$.
We evaluate $F(x)$ at the upper bound ($x=2$) and lower bound ($x=1$):
For $x = 2$:
$F(2) = (2)^4 - \frac{5}{3}(2)^3 + 3(2)^2 + 9(2)$
$F(2) = 16 - \frac{5}{3}(8) + 3(4) + 18$
$F(2) = 16 - \frac{40}{3} + 12 + 18 = 46 - \frac{40}{3}$
$F(2) = \frac{138 - 40}{3} = \frac{98}{3}$
For $x = 1$:
$F(1) = (1)^4 - \frac{5}{3}(1)^3 + 3(1)^2 + 9(1)$
$F(1) = 1 - \frac{5}{3} + 3 + 9 = 13 - \frac{5}{3}$
$F(1) = \frac{39 - 5}{3} = \frac{34}{3}$
Subtracting $F(1)$ from $F(2)$:
$\int_{1}^{2} f(x) \, dx = \frac{98}{3} - \frac{34}{3}$
$\int_{1}^{2} f(x) \, dx = \frac{64}{3}$
Final Solution: \frac{64}{3}
Solution:
We are tasked with evaluating the definite integral:
$I = \int_{0}^{1} x e^{x^2} dx$
Given the integrand is a composition of functions where the derivative of the exponent ($x^2$) is proportional to the multiplier ($x$), we employ the Method of Substitution [Per the substitution rule for definite integrals].
Let $u = x^2$.
Differentiating both sides with respect to $x$:
$\frac{du}{dx} = 2x \implies du = 2x dx \implies x dx = \frac{1}{2} du$
We must adjust the limits of integration from the variable $x$ to the variable $u$ using the relation $u = x^2$:
[By the Fundamental Theorem of Calculus, the transformation of bounds is required when performing change of variables].
Substituting $u$ and $du$ into the original integral:
$I = \int_{0}^{1} e^u \left( \frac{1}{2} du \right)$
$I = \frac{1}{2} \int_{0}^{1} e^u du$
Evaluating the antiderivative [Per the integration rule $\int e^u du = e^u + C$]:
$I = \frac{1}{2} [e^u]_{0}^{1}$
$I = \frac{1}{2} (e^1 - e^0)$
Since $e^0 = 1$ [By the zero exponent rule in algebra]:
$I = \frac{1}{2} (e - 1)$
Final Solution: \frac{e-1}{2}
Solution:
The given definite integral is:
$I = \int_{0}^{1} \frac{dx}{\sqrt{1-x^2}}$
This integral corresponds to the standard derivative form of the inverse trigonometric function $\arcsin(x)$. [Per the Fundamental Theorem of Calculus and standard integration tables, $\int \frac{1}{\sqrt{a^2-x^2}} dx = \sin^{-1}\left(\frac{x}{a}\right) + C$.]
In this specific case, $a = 1$. Therefore, the antiderivative of $f(x) = \frac{1}{\sqrt{1-x^2}}$ is:
$F(x) = \sin^{-1}(x)$
By the Second Fundamental Theorem of Calculus, if $f$ is continuous on $[a, b]$ and $F$ is an antiderivative of $f$, then:
$\int_{a}^{b} f(x) dx = F(b) - F(a)$
Substituting the limits $0$ and $1$ into the antiderivative $F(x) = \sin^{-1}(x)$:
$I = [\sin^{-1}(x)]_{0}^{1}$
$I = \sin^{-1}(1) - \sin^{-1}(0)$
We evaluate the inverse sine values based on the unit circle definitions:
$I = \frac{\pi}{2} - 0 = \frac{\pi}{2}$
Final Solution: \frac{\pi}{2}
Solution:
The given definite integral is:
$I = \int_{1}^{\sqrt{3}} \frac{dx}{1+x^2}$
We observe that the integrand is of the standard form $\frac{1}{a^2 + x^2}$, where $a = 1$. [Per the standard integral table for inverse trigonometric functions]
We recall the standard result for the antiderivative:
$\int \frac{dx}{1+x^2} = \tan^{-1}(x) + C$
Applying the Fundamental Theorem of Calculus, Part II, which states that if $F$ is the antiderivative of $f$, then $\int_{a}^{b} f(x) dx = F(b) - F(a)$:
$I = [\tan^{-1}(x)]_{1}^{\sqrt{3}}$
Substitute the upper and lower limits into the evaluated antiderivative:
$I = \tan^{-1}(\sqrt{3}) - \tan^{-1}(1)$
Using the principal values of the inverse tangent function:
Therefore:
$I = \frac{\pi}{3} - \frac{\pi}{4}$
To subtract the fractions, find the least common denominator (LCD), which is $12$:
$I = \frac{4\pi}{12} - \frac{3\pi}{12} = \frac{\pi}{12}$
Final Solution: \frac{\pi}{12}
Solution:
The given integral is $\int_{2}^{3} \frac{dx}{x^2 - 1}$. We recognize that the denominator is a difference of squares, $x^2 - 1 = (x - 1)(x + 1)$. This indicates the application of the method of Partial Fraction Decomposition [Per the algebraic identity for integration of rational functions].
We decompose the integrand into simpler fractions:
$\frac{1}{x^2 - 1} = \frac{1}{(x - 1)(x + 1)} = \frac{A}{x - 1} + \frac{B}{x + 1}$
Multiplying both sides by $(x-1)(x+1)$ yields:
$1 = A(x + 1) + B(x - 1)$
Thus, the integral becomes: $\int_{2}^{3} \left( \frac{1/2}{x-1} - \frac{1/2}{x+1} \right) dx$.
Using the linearity property of integration [Per the Linearity Property of Definite Integrals]:
$\frac{1}{2} \int_{2}^{3} \frac{1}{x-1} dx - \frac{1}{2} \int_{2}^{3} \frac{1}{x+1} dx$
Evaluating the antiderivatives [Per $\int \frac{1}{u} du = \ln|u| + C$]:
$= \frac{1}{2} \left[ \ln|x-1| - \ln|x+1| \right]_{2}^{3}$
$= \frac{1}{2} \left[ \ln \left| \frac{x-1}{x+1} \right| \right]_{2}^{3}$
Applying the limits of integration [Per the Fundamental Theorem of Calculus Part II]:
$= \frac{1}{2} \left( \ln \left| \frac{3-1}{3+1} \right| - \ln \left| \frac{2-1}{2+1} \right| \right)$
$= \frac{1}{2} \left( \ln \left| \frac{2}{4} \right| - \ln \left| \frac{1}{3} \right| \right)$
$= \frac{1}{2} \left( \ln \left( \frac{1}{2} \right) - \ln \left( \frac{1}{3} \right) \right)$
Applying the quotient rule for logarithms [Per $\ln(a) - \ln(b) = \ln(a/b)$]:
$= \frac{1}{2} \ln \left( \frac{1/2}{1/3} \right) = \frac{1}{2} \ln \left( \frac{3}{2} \right)$
Final Solution: $\frac{1}{2} \ln \left( \frac{3}{2} \right)$
Solution:
The integral to be evaluated is defined as $I = \int_{0}^{1} \frac{dx}{1+x^2}$. This integral follows the standard form of the derivative of the inverse trigonometric function, specifically the arctangent function [Per the Fundamental Theorem of Calculus and standard integration tables].
The antiderivative of $\frac{1}{1+x^2}$ with respect to $x$ is defined as:
$\int \frac{dx}{1+x^2} = \tan^{-1}(x) + C$
The Fundamental Theorem of Calculus states that if $f$ is a continuous function on $[a, b]$ and $F$ is an antiderivative of $f$, then:
$\int_{a}^{b} f(x) \, dx = F(b) - F(a)$
In this specific case, $a = 0$, $b = 1$, and $F(x) = \tan^{-1}(x)$.
Substituting the upper and lower limits into the antiderivative:
$I = \left[ \tan^{-1}(x) \right]_{0}^{1}$
$I = \tan^{-1}(1) - \tan^{-1}(0)$
Evaluating the inverse tangent values based on unit circle properties:
Substituting these values:
$I = \frac{\pi}{4} - 0 = \frac{\pi}{4}$
| Component | Value |
|---|---|
| Lower Limit ($a$) | $0$ |
| Upper Limit ($b$) | $1$ |
| Integral Result | $\frac{\pi}{4}$ |
Final Solution: \frac{\pi}{4}
Solution:
The given integral is of the form $\int \frac{dx}{a^2 + f(x)^2}$. To solve this, we utilize the standard integration formula:
$\int \frac{dx}{a^2 + x^2} = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right) + C$
Given the expression $\int_{0}^{\frac{2}{3}} \frac{dx}{4+9x^2}$, we observe that the denominator is not in the form $a^2 + x^2$. We must manipulate the denominator to isolate the $x^2$ term.
Factor out the constant coefficient of $x^2$ from the denominator:
$4 + 9x^2 = 9\left(\frac{4}{9} + x^2\right)$
Substituting this back into the integral:
$I = \int_{0}^{\frac{2}{3}} \frac{dx}{9\left(\left(\frac{2}{3}\right)^2 + x^2\right)} = \frac{1}{9} \int_{0}^{\frac{2}{3}} \frac{dx}{\left(\frac{2}{3}\right)^2 + x^2}$
Using the identity $\int \frac{dx}{a^2 + x^2} = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right)$, where $a = \frac{2}{3}$:
$I = \frac{1}{9} \left[ \frac{1}{2/3} \tan^{-1}\left(\frac{x}{2/3}\right) \right]_{0}^{\frac{2}{3}}$
[By the Fundamental Theorem of Calculus, $\int_{a}^{b} f(x)dx = F(b) - F(a)$]
Simplify the coefficient: $\frac{1}{9} \times \frac{3}{2} = \frac{3}{18} = \frac{1}{6}$
$I = \frac{1}{6} \left[ \tan^{-1}\left(\frac{3x}{2}\right) \right]_{0}^{\frac{2}{3}}$
Substitute the upper and lower limits:
$I = \frac{1}{6} \left[ \tan^{-1}\left(\frac{3}{2} \cdot \frac{2}{3}\right) - \tan^{-1}\left(\frac{3}{2} \cdot 0\right) \right]$
$I = \frac{1}{6} \left[ \tan^{-1}(1) - \tan^{-1}(0) \right]$
Given the standard values of inverse trigonometric functions:
$I = \frac{1}{6} \left( \frac{\pi}{4} - 0 \right) = \frac{\pi}{24}$
Final Solution: \frac{\pi}{24}