Math, asked by Anonymous, 2 months ago


\displaystyle \lim_{x \to \infty} \left( 1 + \frac{1}{x} \right)^x = e

Answers

Answered by Anonymous
19

\large{ \underline{\sf{Solution :-}}}

We have,

 \rm \lim \limits_{x \to \infty} \left( 1 + \dfrac{1}{x} \right)^x

Let's assume that,

 \implies \rm y =  \lim \limits_{x \to \infty} \left( 1 + \dfrac{1}{x} \right)^x

Taking natural log both sides.

 \implies \rm \:  \ln y =  \lim \limits_{x \to \infty}  \ln\left( 1 + \dfrac{1}{x} \right)^x

{ \implies \rm \:  \ln y =  \lim \limits_{x \to \infty}  \dfrac{ \ln\left( 1 + \dfrac{1}{x} \right)}{ {x}^{ - 1} }}

Now applying L'Hopital rule.

{ \implies \rm \:  \ln y =  \lim \limits_{x \to \infty}  \dfrac{ \dfrac{d}{dx}  \ln\left( 1 + \dfrac{1}{x} \right)}{ \dfrac{d}{dx}  {x}^{ - 1} }}

{ \implies \rm \:  \ln y =  \lim \limits_{x \to \infty}  \dfrac{ \dfrac1{\left( 1 + \frac{1}{x} \right)} \times ( -  {x}^{ - 2} )}{  { - x}^{ - 2}  }}

{ \implies \rm \:  \ln y =  \lim \limits_{x \to \infty}  \dfrac1{\left( 1 + \dfrac{1}{x} \right)}}

{ \implies \rm \:  \ln y =    \dfrac1{\left( 1 + \dfrac{1}{ \infty} \right)}}

{ \implies \rm \:  \ln y =    \dfrac1{\left( 1 + 0\right)}}

{ \implies \rm \:  \ln y =   1}

Or in terms of exponential,

{ \implies \rm \:   {e}^{\ln y }=    {e}^{1} }

{ \implies \rm \:  y=    {e}^{1}}

{ \implies \rm \:  y=    {e}}

Therefore the required result is proved that,

 \underline{ \boxed{ \rm \lim \limits_{x \to \infty} \left( 1 + \dfrac{1}{x} \right)^x  = e}}

Additional Information :-

\boxed{\begin{array}{c|c} \tt f(x)& \tt f'(x)\\\underline{\qquad\qquad}&\underline{\qquad\qquad}\\ \\ \sf x^n&\sf nx^{n-1}\\\\\sf {ln  \: a}&\sf{\dfrac{1}{x}}\\\\\sf {e^x}&\sf {e^x} \\  \\  \sf log_{a}x & \sf\dfrac{1}{x}\log_ea\\\\ \sf a^x&\sf a^x\log_ea\\\\\sf\sqrt{x}&\sf\dfrac{1}{2\sqrt{x}}\end{array}}

Answered by TrustedAnswerer19
22

[ I will solve this question in another method ]

{\blue{ \boxed{ \boxed{ \begin{array}{cc} \bf \to \: we \: have \: to \: prove \:  :   \\  \\ \sf \hookrightarrow \: \displaystyle \lim_{x \to \infty} \rm \:  {(1 +  \frac{1}{x} })^{x}  = e \end{array}}}}}

{ \boxed{ \boxed{ \begin{array}{cc}  \rm \: L.H.S = \displaystyle \lim_{x \to \infty} \rm {(1 +  \frac{1}{x} })^{x} \\  \\ \orange{{\boxed{\begin{array}{cc}\bf \: we \: know :  \\ \:      {(1+ x)}^{n }  = 1 + n \: x +  \frac{n(n - 1)}{2!}  {x}^{2} +   \frac{n(n - 1)(n - 2)}{3!}. {x}^{3}  + ... \end{array}}}} \\  \\ \small{   =\displaystyle \lim_{x \to \infty} \rm \{1 +  \frac{x}{1!} . \frac{1}{x} +  \frac{x(x - 1)}{2!} . {( \frac{1}{x} })^{2}  +  \frac{x(x - 1)(x - 2)}{3!}. {( \frac{1}{x} })^{3}   +  ... \} }  \\  \\  = \displaystyle \lim_{x \to \infty} \rm \{1 +  \frac{1}{1!}  +  \frac{ {x}^{2}( 1 -  \frac{1}{x}) }{2!}. \frac{1}{ {x}^{2} }  +  \frac{ {x}^{3} (1 -  \frac{1}{x} )(1 -  \frac{2}{x}) }{3!} . \frac{1}{ {x}^{3} }  + ... \} \end{array}}}}

{ \boxed{ \boxed{ \begin{array}{cc} =\displaystyle \lim_{x \to \infty} \rm  \{ 1 +  \frac{1}{1!} +  \frac{(1 -  \frac{1}{x}) }{2!}  +  \frac{(1 -  \frac{1}{x})(1 -  \frac{2}{x})  }{3!}  + ... \} \\  \\ =   \rm1 +  \frac{1}{1!} + \frac{ (1 -  \frac{1}{ \infty} )} {2!}  +  \frac{(1 -  \frac{1}{ \infty} ( 1 -  \frac{2}{ \infty} ) }{3!}  + ... \\  \\  \rm = 1 +  \frac{1}{1!} +  \frac{(1 - 0)}{2!} +  \frac{(1 - 0)(1 - 0)}{3!}   + ... \\  \\  \rm = 1 +  \frac{1}{1!}  +  \frac{1}{2!}   +  \frac{1}{3!} + ... \\  \\  \orange{{\boxed{\begin{array}{cc}\bf \: we \: know \: that: \\  \\  \rm \:  {e}^{x}  = 1 +  \frac{x}{1!}  +  \frac{ {x}^{2} }{2!}   +  \frac{ {x}^{3} }{3!} + ... \\  \\  \therefore \rm \: e = 1 +  \frac{1}{1!}  +  \frac{1}{2!}   +  \frac{1}{3!} + ...\end{array}}}}  \\  \\ \rm = e \\  \\  \rm = R.H.S\end{array}}}}

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