Evaluate the limit $\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{\mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt}{{{x}^{2}}-\dfrac{{{\pi }^{2}}}{16}}$
A) $\dfrac{8}{\pi }f(2)$
B) $\dfrac{2}{\pi }f(2)$
C) $\dfrac{2}{\pi }f\left( \dfrac{1}{2} \right)$
D) $2f(2)$
Answer
689.4k+ views
Hint: See that the limit is of the form $\dfrac{0}{0}$ and there is an integral in limit. Use Leibniz Rule and L’Hopital Rule to evaluate the limit.
Let the given limit be equal to \[L\],
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{\mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt}{{{x}^{2}}-\dfrac{{{\pi }^{2}}}{16}}$
If we substitute \[x\] as $\dfrac{\pi }{4}$ we get,
$L=\dfrac{\mathop{\int }_{2}^{{{\sec }^{2}}\dfrac{\pi }{4}}f\left( t \right)dt}{{{\left( \dfrac{\pi }{4} \right)}^{2}}-\dfrac{{{\pi }^{2}}}{16}}$
\[L=\dfrac{\mathop{\int }_{2}^{{{\sqrt{2}}^{2}}}f\left( t \right)dt}{\dfrac{{{\pi }^{2}}}{16}-\dfrac{{{\pi }^{2}}}{16}}\]
\[L=\dfrac{\mathop{\int }_{2}^{2}f\left( t \right)dt}{\dfrac{{{\pi }^{2}}}{16}-\dfrac{{{\pi }^{2}}}{16}}\]
We know that \[\int\limits_{a}^{a}{f(x)dx=0}\]. Therefore, the numerator tends to \[0\].
\[L=\dfrac{0}{0}\]
The numerator and denominator tends to zero as \[x\] tends to $\dfrac{\pi }{4}$, so the limit is of the form $\dfrac{0}{0}$. So we can use L’Hopital’s Rule i.e. differentiating the numerator and denominator separately to evaluate the limit. L’Hopital Rule can only be used when the limit is of the form $\dfrac{0}{0}$ or$\dfrac{\infty }{\infty }$.
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)}{\dfrac{d}{dx}\left( {{x}^{2}}-\dfrac{{{\pi }^{2}}}{16} \right)}$
For evaluating the numerator we use Leibniz’s Rule i.e.
$\dfrac{d}{dx}\left( \mathop{\int }_{b\left( x \right)}^{a\left( x \right)}f\left( x \right)dx \right)=\left\{ f\left( a\left( x \right) \right)~a'\left( x \right) \right\}-\left\{ f\left( b\left( x \right) \right)b'\left( x \right) \right\}$ where\[a'\left( x \right)\]and \[b'\left( x \right)\]are derivatives of functions \[a\left( x \right)\]and \[b\left( x \right)\] with respect to\[x\].
$\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)=f\left( se{{c}^{2}}\left( x \right) \right)~\left( 2se{{c}^{2}}\left( x \right)\tan \left( x \right) \right)-\left( f\left( 2 \right)\left( 0 \right) \right)$
$\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)=2f\left( se{{c}^{2}}\left( x \right) \right)se{{c}^{2}}\left( x \right))\text{tan}\left( x \right)$
So,
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{2f\left( se{{c}^{2}}\left( x \right) \right)se{{c}^{2}}\left( x \right))\text{tan}\left( x \right)}{2x}$
Now we can simply evaluate the limit by substituting \[x\] as$\dfrac{\pi }{4}$.
$\text{L= }\!\!~\!\!\text{ }\dfrac{2f\left( se{{c}^{2}}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right) \right)se{{c}^{2}}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right))\text{tan}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right)}{2~\times ~\text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4}}$
$\text{L= }\!\!~\!\!\text{ }\dfrac{2f\left( 2 \right)\times 2\times 1}{\dfrac{\pi }{2}}$
$\text{L= }\!\!~\!\!\text{ }\dfrac{8}{\pi }f\left( 2 \right)$
So, the answer is Option A) $\dfrac{8}{\pi }f(2)$
Note: Students must be careful while using Leibniz Rule and L'Hopital Rule. They might make mistakes by only differentiating the numerator only the denominator only, or not using Leibniz Rule correctly i.e. they might not differentiate the limits, not put the limits correctly, etc. Do not use L'Hopital's Rule multiple times, it may lead to incorrect answers.
Let the given limit be equal to \[L\],
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{\mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt}{{{x}^{2}}-\dfrac{{{\pi }^{2}}}{16}}$
If we substitute \[x\] as $\dfrac{\pi }{4}$ we get,
$L=\dfrac{\mathop{\int }_{2}^{{{\sec }^{2}}\dfrac{\pi }{4}}f\left( t \right)dt}{{{\left( \dfrac{\pi }{4} \right)}^{2}}-\dfrac{{{\pi }^{2}}}{16}}$
\[L=\dfrac{\mathop{\int }_{2}^{{{\sqrt{2}}^{2}}}f\left( t \right)dt}{\dfrac{{{\pi }^{2}}}{16}-\dfrac{{{\pi }^{2}}}{16}}\]
\[L=\dfrac{\mathop{\int }_{2}^{2}f\left( t \right)dt}{\dfrac{{{\pi }^{2}}}{16}-\dfrac{{{\pi }^{2}}}{16}}\]
We know that \[\int\limits_{a}^{a}{f(x)dx=0}\]. Therefore, the numerator tends to \[0\].
\[L=\dfrac{0}{0}\]
The numerator and denominator tends to zero as \[x\] tends to $\dfrac{\pi }{4}$, so the limit is of the form $\dfrac{0}{0}$. So we can use L’Hopital’s Rule i.e. differentiating the numerator and denominator separately to evaluate the limit. L’Hopital Rule can only be used when the limit is of the form $\dfrac{0}{0}$ or$\dfrac{\infty }{\infty }$.
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)}{\dfrac{d}{dx}\left( {{x}^{2}}-\dfrac{{{\pi }^{2}}}{16} \right)}$
For evaluating the numerator we use Leibniz’s Rule i.e.
$\dfrac{d}{dx}\left( \mathop{\int }_{b\left( x \right)}^{a\left( x \right)}f\left( x \right)dx \right)=\left\{ f\left( a\left( x \right) \right)~a'\left( x \right) \right\}-\left\{ f\left( b\left( x \right) \right)b'\left( x \right) \right\}$ where\[a'\left( x \right)\]and \[b'\left( x \right)\]are derivatives of functions \[a\left( x \right)\]and \[b\left( x \right)\] with respect to\[x\].
$\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)=f\left( se{{c}^{2}}\left( x \right) \right)~\left( 2se{{c}^{2}}\left( x \right)\tan \left( x \right) \right)-\left( f\left( 2 \right)\left( 0 \right) \right)$
$\dfrac{d}{dx}\left( \mathop{\int }_{2}^{{{\sec }^{2}}x}f\left( t \right)dt \right)=2f\left( se{{c}^{2}}\left( x \right) \right)se{{c}^{2}}\left( x \right))\text{tan}\left( x \right)$
So,
$L=\underset{x\to \dfrac{\pi }{4}}{\mathop{\lim }}\,\dfrac{2f\left( se{{c}^{2}}\left( x \right) \right)se{{c}^{2}}\left( x \right))\text{tan}\left( x \right)}{2x}$
Now we can simply evaluate the limit by substituting \[x\] as$\dfrac{\pi }{4}$.
$\text{L= }\!\!~\!\!\text{ }\dfrac{2f\left( se{{c}^{2}}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right) \right)se{{c}^{2}}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right))\text{tan}\left( \text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4} \right)}{2~\times ~\text{ }\!\!~\!\!\text{ }\dfrac{\pi }{4}}$
$\text{L= }\!\!~\!\!\text{ }\dfrac{2f\left( 2 \right)\times 2\times 1}{\dfrac{\pi }{2}}$
$\text{L= }\!\!~\!\!\text{ }\dfrac{8}{\pi }f\left( 2 \right)$
So, the answer is Option A) $\dfrac{8}{\pi }f(2)$
Note: Students must be careful while using Leibniz Rule and L'Hopital Rule. They might make mistakes by only differentiating the numerator only the denominator only, or not using Leibniz Rule correctly i.e. they might not differentiate the limits, not put the limits correctly, etc. Do not use L'Hopital's Rule multiple times, it may lead to incorrect answers.
Recently Updated Pages
If x a + bt + ct2 where x is in meters and t is in class 11 physics CBSE

A car covers the first half distance between two places class 11 physics CBSE

The resultant of two vectors overrightarrow P and overrightarrow class 11 physics CBSE

Find the value of cos 135 class 11 maths CBSE

A mass M is held in place by an applied force F and class 11 physics CBSE

A solution of glucose in water is labelled as 10 dfracwv class 11 chemistry CBSE

Trending doubts
Find the value of the expression given below sin 30circ class 11 maths CBSE

One Metric ton is equal to kg A 10000 B 1000 C 100 class 11 physics CBSE

Draw a diagram of nephron and explain its structur class 11 biology CBSE

10 examples of friction in our daily life

Proton was discovered by A Thomson B Rutherford C Chadwick class 11 chemistry CBSE

Bond order ofO2 O2+ O2 and O22 is in order A O2 langle class 11 chemistry CBSE

