
Find the value of
\[\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\]
Answer
483.9k+ views
Hint: We start solving the problem by using the property \[\int\limits_{-a}^{a}{f(x)dx=}\int\limits_{0}^{a}{\left( f(x)+f(-x) \right)}dx\] in the given definite integral. We make subsequent calculations required and use the property \[{{\sin }^{2}}\theta =\dfrac{\left( 1-\cos 2\theta \right)}{2}\] to proceed further through the problem. We then use the property \[\int\limits_{b}^{a}{\left( mf(x)+ng(x) \right)dx=}\int\limits_{b}^{a}{mf(x)dx+\int\limits_{b}^{a}{ng(x)dx}}\] and integrate the functions. We then substitute the limits of the definite integral in the obtained functions to get the required answer.
Complete step-by-step answer:
As mentioned in the question, we have to evaluate the following expression \[I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
Let us assume the value of the given definite integral be I. So, we get \[I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
Using the property of definite integration in the above definite integral, we can write as the following expression
\[\Rightarrow I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
By using the following property of definite integration \[\int\limits_{-a}^{a}{f(x)dx=}\int\limits_{0}^{a}{\left( f(x)+f(-x) \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\sin }^{2}}\left( -x \right)}{1+{{\left( 2017 \right)}^{\left( -x \right)}}} \right)}dx\] ---(1).
We know that ${{a}^{-x}}=\dfrac{1}{{{a}^{x}}}$. We use this result in equation (1).
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\left( -\sin \left( x \right) \right)}^{2}}}{1+\dfrac{1}{{{\left( 2017 \right)}^{x}}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\sin }^{2}}x}{\dfrac{{{\left( 2017 \right)}^{x}}+1}{{{\left( 2017 \right)}^{x}}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{\left( {{\sin }^{2}}x \right)\times {{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
We now take ${{\sin }^{2}}x$ common in both terms present in integrand.
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)\left( \dfrac{1}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)\left( \dfrac{1+{{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)}dx\].
Now, we will use the relation between cos \[2\theta \] and \[{{\sin }^{2}}\theta \] as mentioned in the hint above as
\[{{\sin }^{2}}\theta =\dfrac{\left( 1-\cos 2\theta \right)}{2}\].
Hence, now we can simplify the definite integral as
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{1-\cos 2x}{2} \right)}dx\].
Now, we use another property $\int\limits_{a}^{b}{\left( mf\left( x \right)+ng\left( x \right) \right)dx=\int\limits_{a}^{b}{mf\left( x \right)dx+\int\limits_{a}^{b}{ng\left( x \right)dx}}}$.
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{1}{2} \right)}dx-\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{\cos 2x}{2} \right)}dx\ \ \ \ ...(a)\]
We know that $\int{adx=ax+C}$ and $\int{\cos axdx=\dfrac{\sin ax}{a}+C}$. We also know that $\int\limits_{a}^{b}{{{f}^{'}}\left( x \right)dx=\left[ f\left( x \right) \right]_{a}^{b}=f\left( b \right)-f\left( a \right)}$. We use this results in equation (a).
\[\Rightarrow I=\dfrac{1}{2}\left[ x \right]_{0}^{\dfrac{\pi }{2}}-\dfrac{1}{4}\left[ \sin 2x \right]_{0}^{\dfrac{\pi }{2}}\].
\[\Rightarrow I=\dfrac{1}{2}\left[ \dfrac{\pi }{2}-0 \right]-\dfrac{1}{4}\left[ \sin \pi -\sin 0 \right]\].
\[\Rightarrow I=\dfrac{1}{2}\left[ \dfrac{\pi }{2} \right]-\dfrac{1}{4}\left[ 0-0 \right]\].
\[\Rightarrow I=\dfrac{\pi }{4}-0\].
\[\Rightarrow I=\dfrac{\pi }{4}\].
Hence, the solution of the definite integral is \[\dfrac{\pi }{4}\].
Note: We should not make an error while using the properties mentioned in the solution. The property of definite integration that would be useful in solving this question would be
\[\int\limits_{-a}^{a}{f(x)dx=}\int\limits_{0}^{a}{\left( f(x)+f(-x) \right)}dx\]. This property is usually used when the upper limit and lower limit have the same absolute values with opposite signs. Without the use of these properties the solution would entangle and the student might get a wrong solution.
Complete step-by-step answer:
As mentioned in the question, we have to evaluate the following expression \[I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
Let us assume the value of the given definite integral be I. So, we get \[I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
Using the property of definite integration in the above definite integral, we can write as the following expression
\[\Rightarrow I=\int\limits_{-\dfrac{\pi }{2}}^{\dfrac{\pi }{2}}{\dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}}dx\].
By using the following property of definite integration \[\int\limits_{-a}^{a}{f(x)dx=}\int\limits_{0}^{a}{\left( f(x)+f(-x) \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\sin }^{2}}\left( -x \right)}{1+{{\left( 2017 \right)}^{\left( -x \right)}}} \right)}dx\] ---(1).
We know that ${{a}^{-x}}=\dfrac{1}{{{a}^{x}}}$. We use this result in equation (1).
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\left( -\sin \left( x \right) \right)}^{2}}}{1+\dfrac{1}{{{\left( 2017 \right)}^{x}}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\sin }^{2}}x}{\dfrac{{{\left( 2017 \right)}^{x}}+1}{{{\left( 2017 \right)}^{x}}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{{{\sin }^{2}}x}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{\left( {{\sin }^{2}}x \right)\times {{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
We now take ${{\sin }^{2}}x$ common in both terms present in integrand.
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)\left( \dfrac{1}{1+{{\left( 2017 \right)}^{x}}}+\dfrac{{{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)\left( \dfrac{1+{{\left( 2017 \right)}^{x}}}{1+{{\left( 2017 \right)}^{x}}} \right)}dx\].
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( {{\sin }^{2}}x \right)}dx\].
Now, we will use the relation between cos \[2\theta \] and \[{{\sin }^{2}}\theta \] as mentioned in the hint above as
\[{{\sin }^{2}}\theta =\dfrac{\left( 1-\cos 2\theta \right)}{2}\].
Hence, now we can simplify the definite integral as
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{1-\cos 2x}{2} \right)}dx\].
Now, we use another property $\int\limits_{a}^{b}{\left( mf\left( x \right)+ng\left( x \right) \right)dx=\int\limits_{a}^{b}{mf\left( x \right)dx+\int\limits_{a}^{b}{ng\left( x \right)dx}}}$.
\[\Rightarrow I=\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{1}{2} \right)}dx-\int\limits_{0}^{\dfrac{\pi }{2}}{\left( \dfrac{\cos 2x}{2} \right)}dx\ \ \ \ ...(a)\]
We know that $\int{adx=ax+C}$ and $\int{\cos axdx=\dfrac{\sin ax}{a}+C}$. We also know that $\int\limits_{a}^{b}{{{f}^{'}}\left( x \right)dx=\left[ f\left( x \right) \right]_{a}^{b}=f\left( b \right)-f\left( a \right)}$. We use this results in equation (a).
\[\Rightarrow I=\dfrac{1}{2}\left[ x \right]_{0}^{\dfrac{\pi }{2}}-\dfrac{1}{4}\left[ \sin 2x \right]_{0}^{\dfrac{\pi }{2}}\].
\[\Rightarrow I=\dfrac{1}{2}\left[ \dfrac{\pi }{2}-0 \right]-\dfrac{1}{4}\left[ \sin \pi -\sin 0 \right]\].
\[\Rightarrow I=\dfrac{1}{2}\left[ \dfrac{\pi }{2} \right]-\dfrac{1}{4}\left[ 0-0 \right]\].
\[\Rightarrow I=\dfrac{\pi }{4}-0\].
\[\Rightarrow I=\dfrac{\pi }{4}\].
Hence, the solution of the definite integral is \[\dfrac{\pi }{4}\].
Note: We should not make an error while using the properties mentioned in the solution. The property of definite integration that would be useful in solving this question would be
\[\int\limits_{-a}^{a}{f(x)dx=}\int\limits_{0}^{a}{\left( f(x)+f(-x) \right)}dx\]. This property is usually used when the upper limit and lower limit have the same absolute values with opposite signs. Without the use of these properties the solution would entangle and the student might get a wrong solution.
Recently Updated Pages
Master Class 12 Economics: Engaging Questions & Answers for Success

Master Class 12 Maths: Engaging Questions & Answers for Success

Master Class 12 Biology: Engaging Questions & Answers for Success

Master Class 12 Physics: Engaging Questions & Answers for Success

Master Class 12 Business Studies: Engaging Questions & Answers for Success

Master Class 12 English: Engaging Questions & Answers for Success

Trending doubts
The probability that a leap year will have only 52 class 12 maths CBSE

The final image formed by a compound microscope is class 12 physics CBSE

Which of the following properties of a proton can change class 12 physics CBSE

Sum of two skew symmetric matrices is always matri class 12 maths CBSE

What is the difference between at least one head and class 12 maths CBSE

What is the energy band gap of silicon and germanium class 12 physics CBSE
