List of limits

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This is a list of limits for common functions such as elementary functions. In this article, the terms a, b and c are constants with respect to x.

${\displaystyle \lim _{x\to c}f(x)=L}${\displaystyle \lim _{x\to c}f(x)=L} if and only if ${\displaystyle \forall \varepsilon >0\ \exists \delta >0:0<|x-c|<\delta \implies |f(x)-L|<\varepsilon }${\displaystyle \forall \varepsilon >0\ \exists \delta >0:0<|x-c|<\delta \implies |f(x)-L|<\varepsilon }. This is the (ε, δ)-definition of limit.

The limit superior and limit inferior of a sequence are defined as ${\displaystyle \limsup _{n\to \infty }x_{n}=\lim _{n\to \infty }\left(\sup _{m\geq n}x_{m}\right)}${\displaystyle \limsup _{n\to \infty }x_{n}=\lim _{n\to \infty }\left(\sup _{m\geq n}x_{m}\right)} and ${\displaystyle \liminf _{n\to \infty }x_{n}=\lim _{n\to \infty }\left(\inf _{m\geq n}x_{m}\right)}${\displaystyle \liminf _{n\to \infty }x_{n}=\lim _{n\to \infty }\left(\inf _{m\geq n}x_{m}\right)}.

A function, ${\displaystyle f(x)}${\displaystyle f(x)}, is said to be continuous at a point, c, if $${\displaystyle \lim _{x\to c}f(x)=f(c).}$${\displaystyle \lim _{x\to c}f(x)=f(c).}

If ${\displaystyle \lim _{x\to c}f(x)=L}${\displaystyle \lim _{x\to c}f(x)=L} then:

• ${\displaystyle \lim _{x\to c},円[f(x)\pm a]=L\pm a}${\displaystyle \lim _{x\to c},円[f(x)\pm a]=L\pm a}
• ${\displaystyle \lim _{x\to c},円af(x)=aL}${\displaystyle \lim _{x\to c},円af(x)=aL}^{[1] [2] [3]}
• ${\displaystyle \lim _{x\to c}{\frac {1}{f(x)}}={\frac {1}{L}}}${\displaystyle \lim _{x\to c}{\frac {1}{f(x)}}={\frac {1}{L}}}^[4] if L is not equal to 0.
• ${\displaystyle \lim _{x\to c},円f(x)^{n}=L^{n}}${\displaystyle \lim _{x\to c},円f(x)^{n}=L^{n}} if n is a positive integer^{[1] [2] [3]}
• ${\displaystyle \lim _{x\to c},円f(x)^{1 \over n}=L^{1 \over n}}${\displaystyle \lim _{x\to c},円f(x)^{1 \over n}=L^{1 \over n}} if n is a positive integer, and if n is even, then L > 0.^{[1] [3]}

In general, if g(x) is continuous at L and ${\displaystyle \lim _{x\to c}f(x)=L}${\displaystyle \lim _{x\to c}f(x)=L} then

• ${\displaystyle \lim _{x\to c}g\left(f(x)\right)=g(L)}${\displaystyle \lim _{x\to c}g\left(f(x)\right)=g(L)}^{[1] [2]}

If ${\displaystyle \lim _{x\to c}f(x)=L_{1}}${\displaystyle \lim _{x\to c}f(x)=L_{1}} and ${\displaystyle \lim _{x\to c}g(x)=L_{2}}${\displaystyle \lim _{x\to c}g(x)=L_{2}} then:

• ${\displaystyle \lim _{x\to c},円[f(x)\pm g(x)]=L_{1}\pm L_{2}}${\displaystyle \lim _{x\to c},円[f(x)\pm g(x)]=L_{1}\pm L_{2}}^{[1] [2] [3]}
• ${\displaystyle \lim _{x\to c},円[f(x)g(x)]=L_{1}\cdot L_{2}}${\displaystyle \lim _{x\to c},円[f(x)g(x)]=L_{1}\cdot L_{2}}^{[1] [2] [3]}
• ${\displaystyle \lim _{x\to c}{\frac {f(x)}{g(x)}}={\frac {L_{1}}{L_{2}}}\qquad {\text{ if }}L_{2}\neq 0}${\displaystyle \lim _{x\to c}{\frac {f(x)}{g(x)}}={\frac {L_{1}}{L_{2}}}\qquad {\text{ if }}L_{2}\neq 0}^{[1] [2] [3]}

In these limits, the infinitesimal change ${\displaystyle h}${\displaystyle h} is often denoted ${\displaystyle \Delta x}${\displaystyle \Delta x} or ${\displaystyle \delta x}${\displaystyle \delta x}. If ${\displaystyle f(x)}${\displaystyle f(x)} is differentiable at ${\displaystyle x}${\displaystyle x},

• ${\displaystyle \lim _{h\to 0}{f(x+h)-f(x) \over h}=f'(x)}${\displaystyle \lim _{h\to 0}{f(x+h)-f(x) \over h}=f'(x)}. This is the definition of the derivative. All differentiation rules can also be reframed as rules involving limits. For example, if g(x) is differentiable at x,
  • ${\displaystyle \lim _{h\to 0}{f\circ g(x+h)-f\circ g(x) \over h}=f'[g(x)]g'(x)}${\displaystyle \lim _{h\to 0}{f\circ g(x+h)-f\circ g(x) \over h}=f'[g(x)]g'(x)}. This is the chain rule.
  • ${\displaystyle \lim _{h\to 0}{f(x+h)g(x+h)-f(x)g(x) \over h}=f'(x)g(x)+f(x)g'(x)}${\displaystyle \lim _{h\to 0}{f(x+h)g(x+h)-f(x)g(x) \over h}=f'(x)g(x)+f(x)g'(x)}. This is the product rule.
• ${\displaystyle \lim _{h\to 0}\left({\frac {f(x+h)}{f(x)}}\right)^{1/h}=\exp \left({\frac {f'(x)}{f(x)}}\right)}${\displaystyle \lim _{h\to 0}\left({\frac {f(x+h)}{f(x)}}\right)^{1/h}=\exp \left({\frac {f'(x)}{f(x)}}\right)}
• ${\displaystyle \lim _{h\to 0}{\left({f(e^{h}x) \over {f(x)}}\right)^{1/h}}=\exp \left({\frac {xf'(x)}{f(x)}}\right)}${\displaystyle \lim _{h\to 0}{\left({f(e^{h}x) \over {f(x)}}\right)^{1/h}}=\exp \left({\frac {xf'(x)}{f(x)}}\right)}

If ${\displaystyle f(x)}${\displaystyle f(x)} and ${\displaystyle g(x)}${\displaystyle g(x)} are differentiable on an open interval containing c, except possibly c itself, and ${\displaystyle \lim _{x\to c}f(x)=\lim _{x\to c}g(x)=0{\text{ or }}\pm \infty }${\displaystyle \lim _{x\to c}f(x)=\lim _{x\to c}g(x)=0{\text{ or }}\pm \infty }, L'Hôpital's rule can be used:

• ${\displaystyle \lim _{x\to c}{\frac {f(x)}{g(x)}}=\lim _{x\to c}{\frac {f'(x)}{g'(x)}}}${\displaystyle \lim _{x\to c}{\frac {f(x)}{g(x)}}=\lim _{x\to c}{\frac {f'(x)}{g'(x)}}}^[2]

If ${\displaystyle f(x)\leq g(x)}${\displaystyle f(x)\leq g(x)} for all x in an interval that contains c, except possibly c itself, and the limit of ${\displaystyle f(x)}${\displaystyle f(x)} and ${\displaystyle g(x)}${\displaystyle g(x)} both exist at c, then^[5] $${\displaystyle \lim _{x\to c}f(x)\leq \lim _{x\to c}g(x)}$${\displaystyle \lim _{x\to c}f(x)\leq \lim _{x\to c}g(x)}

If ${\displaystyle \lim _{x\to c}f(x)=\lim _{x\to c}h(x)=L}${\displaystyle \lim _{x\to c}f(x)=\lim _{x\to c}h(x)=L} and ${\displaystyle f(x)\leq g(x)\leq h(x)}${\displaystyle f(x)\leq g(x)\leq h(x)} for all x in an open interval that contains c, except possibly c itself, $${\displaystyle \lim _{x\to c}g(x)=L.}$${\displaystyle \lim _{x\to c}g(x)=L.} This is known as the squeeze theorem.^{[1] [2]} This applies even in the cases that f(x) and g(x) take on different values at c, or are discontinuous at c.

• ${\displaystyle \lim _{x\to c}a=a}${\displaystyle \lim _{x\to c}a=a}^{[1] [2] [3]}

• ${\displaystyle \lim _{x\to c}x=c}${\displaystyle \lim _{x\to c}x=c}^{[1] [2] [3]}
• ${\displaystyle \lim _{x\to c}(ax+b)=ac+b}${\displaystyle \lim _{x\to c}(ax+b)=ac+b}
• ${\displaystyle \lim _{x\to c}x^{n}=c^{n}}${\displaystyle \lim _{x\to c}x^{n}=c^{n}} if n is a positive integer^[5]
• ${\displaystyle \lim _{x\to \infty }x/a={\begin{cases}\infty ,&a>0\\{\text{does not exist}},&a=0\\-\infty ,&a<0\end{cases}}}${\displaystyle \lim _{x\to \infty }x/a={\begin{cases}\infty ,&a>0\\{\text{does not exist}},&a=0\\-\infty ,&a<0\end{cases}}}

In general, if ${\displaystyle p(x)}${\displaystyle p(x)} is a polynomial then, by the continuity of polynomials,^[5] $${\displaystyle \lim _{x\to c}p(x)=p(c)}$${\displaystyle \lim _{x\to c}p(x)=p(c)} This is also true for rational functions, as they are continuous on their domains.^[5]

• ${\displaystyle \lim _{x\to c}x^{a}=c^{a}.}${\displaystyle \lim _{x\to c}x^{a}=c^{a}.}^[5] In particular,
  • ${\displaystyle \lim _{x\to \infty }x^{a}={\begin{cases}\infty ,&a>0\1,円&a=0\0,円&a<0\end{cases}}}${\displaystyle \lim _{x\to \infty }x^{a}={\begin{cases}\infty ,&a>0\1,円&a=0\0,円&a<0\end{cases}}}
• ${\displaystyle \lim _{x\to c}x^{1/a}=c^{1/a}}${\displaystyle \lim _{x\to c}x^{1/a}=c^{1/a}}.^[5] In particular,
  • ${\displaystyle \lim _{x\to \infty }x^{1/a}=\lim _{x\to \infty }{\sqrt[{a}]{x}}=\infty {\text{ for any }}a>0}${\displaystyle \lim _{x\to \infty }x^{1/a}=\lim _{x\to \infty }{\sqrt[{a}]{x}}=\infty {\text{ for any }}a>0}^[6]
• ${\displaystyle \lim _{x\to 0^{+}}x^{-n}=\lim _{x\to 0^{+}}{\frac {1}{x^{n}}}=+\infty }${\displaystyle \lim _{x\to 0^{+}}x^{-n}=\lim _{x\to 0^{+}}{\frac {1}{x^{n}}}=+\infty }
• ${\displaystyle \lim _{x\to 0^{-}}x^{-n}=\lim _{x\to 0^{-}}{\frac {1}{x^{n}}}={\begin{cases}-\infty ,&{\text{if }}n{\text{ is odd}}\\+\infty ,&{\text{if }}n{\text{ is even}}\end{cases}}}${\displaystyle \lim _{x\to 0^{-}}x^{-n}=\lim _{x\to 0^{-}}{\frac {1}{x^{n}}}={\begin{cases}-\infty ,&{\text{if }}n{\text{ is odd}}\\+\infty ,&{\text{if }}n{\text{ is even}}\end{cases}}}
• ${\displaystyle \lim _{x\to \infty }ax^{-1}=\lim _{x\to \infty }a/x=0{\text{ for any real }}a}${\displaystyle \lim _{x\to \infty }ax^{-1}=\lim _{x\to \infty }a/x=0{\text{ for any real }}a}

• ${\displaystyle \lim _{x\to c}e^{x}=e^{c}}${\displaystyle \lim _{x\to c}e^{x}=e^{c}}, due to the continuity of ${\displaystyle e^{x}}${\displaystyle e^{x}}
• ${\displaystyle \lim _{x\to \infty }a^{x}={\begin{cases}\infty ,&a>1\1,円&a=1\0,円&0<a<1\end{cases}}}${\displaystyle \lim _{x\to \infty }a^{x}={\begin{cases}\infty ,&a>1\1,円&a=1\0,円&0<a<1\end{cases}}}
• ${\displaystyle \lim _{x\to \infty }a^{-x}={\begin{cases}0,&a>1\1,円&a=1\\\infty ,&0<a<1\end{cases}}}${\displaystyle \lim _{x\to \infty }a^{-x}={\begin{cases}0,&a>1\1,円&a=1\\\infty ,&0<a<1\end{cases}}}^[6]
• ${\displaystyle \lim _{x\to \infty }{\sqrt[{x}]{a}}=\lim _{x\to \infty }{a}^{1/x}={\begin{cases}1,&a>0\0,円&a=0\\{\text{does not exist}},&a<0\end{cases}}}${\displaystyle \lim _{x\to \infty }{\sqrt[{x}]{a}}=\lim _{x\to \infty }{a}^{1/x}={\begin{cases}1,&a>0\0,円&a=0\\{\text{does not exist}},&a<0\end{cases}}}

• ${\displaystyle \lim _{x\to \infty }{\sqrt[{x}]{x}}=\lim _{x\to \infty }{x}^{1/x}=1}${\displaystyle \lim _{x\to \infty }{\sqrt[{x}]{x}}=\lim _{x\to \infty }{x}^{1/x}=1}

• ${\displaystyle \lim _{x\to +\infty }\left({\frac {x}{x+k}}\right)^{x}=e^{-k}}${\displaystyle \lim _{x\to +\infty }\left({\frac {x}{x+k}}\right)^{x}=e^{-k}}^[2]
• ${\displaystyle \lim _{x\to 0}\left(1+x\right)^{\frac {1}{x}}=e}${\displaystyle \lim _{x\to 0}\left(1+x\right)^{\frac {1}{x}}=e}^[2]
• ${\displaystyle \lim _{x\to 0}\left(1+kx\right)^{\frac {m}{x}}=e^{mk}}${\displaystyle \lim _{x\to 0}\left(1+kx\right)^{\frac {m}{x}}=e^{mk}}
• ${\displaystyle \lim _{x\to +\infty }\left(1+{\frac {1}{x}}\right)^{x}=e}${\displaystyle \lim _{x\to +\infty }\left(1+{\frac {1}{x}}\right)^{x}=e}^[7]
• ${\displaystyle \lim _{x\to +\infty }\left(1-{\frac {1}{x}}\right)^{x}={\frac {1}{e}}}${\displaystyle \lim _{x\to +\infty }\left(1-{\frac {1}{x}}\right)^{x}={\frac {1}{e}}}
• ${\displaystyle \lim _{x\to +\infty }\left(1+{\frac {k}{x}}\right)^{mx}=e^{mk}}${\displaystyle \lim _{x\to +\infty }\left(1+{\frac {k}{x}}\right)^{mx}=e^{mk}}^[6]
• ${\displaystyle \lim _{x\to 0}\left(1+a\left({e^{-x}-1}\right)\right)^{-{\frac {1}{x}}}=e^{a}}${\displaystyle \lim _{x\to 0}\left(1+a\left({e^{-x}-1}\right)\right)^{-{\frac {1}{x}}}=e^{a}}. This limit can be derived from this limit.

• ${\displaystyle \lim _{x\to 0}xe^{-x}=0}${\displaystyle \lim _{x\to 0}xe^{-x}=0}
• ${\displaystyle \lim _{x\to \infty }xe^{-x}=0}${\displaystyle \lim _{x\to \infty }xe^{-x}=0}
• ${\displaystyle \lim _{x\to 0}\left({\frac {a^{x}-1}{x}}\right)=\ln {a},}${\displaystyle \lim _{x\to 0}\left({\frac {a^{x}-1}{x}}\right)=\ln {a},} for all positive a.^{[4] [7]}
• ${\displaystyle \lim _{x\to 0}\left({\frac {e^{x}-1}{x}}\right)=1}${\displaystyle \lim _{x\to 0}\left({\frac {e^{x}-1}{x}}\right)=1}
• ${\displaystyle \lim _{x\to 0}\left({\frac {e^{ax}-1}{x}}\right)=a}${\displaystyle \lim _{x\to 0}\left({\frac {e^{ax}-1}{x}}\right)=a}

• ${\displaystyle \lim _{x\to c}\ln {x}=\ln c}${\displaystyle \lim _{x\to c}\ln {x}=\ln c}, due to the continuity of ${\displaystyle \ln {x}}${\displaystyle \ln {x}}. In particular,
  • ${\displaystyle \lim _{x\to 0^{+}}\log x=-\infty }${\displaystyle \lim _{x\to 0^{+}}\log x=-\infty }
  • ${\displaystyle \lim _{x\to \infty }\log x=\infty }${\displaystyle \lim _{x\to \infty }\log x=\infty }
• ${\displaystyle \lim _{x\to 1}{\frac {\ln(x)}{x-1}}=1}${\displaystyle \lim _{x\to 1}{\frac {\ln(x)}{x-1}}=1}
• ${\displaystyle \lim _{x\to 0}{\frac {\ln(x+1)}{x}}=1}${\displaystyle \lim _{x\to 0}{\frac {\ln(x+1)}{x}}=1}^[7]
• ${\displaystyle \lim _{x\to 0}{\frac {-\ln \left(1+a\left({e^{-x}-1}\right)\right)}{x}}=a}${\displaystyle \lim _{x\to 0}{\frac {-\ln \left(1+a\left({e^{-x}-1}\right)\right)}{x}}=a}. This limit follows from L'Hôpital's rule.
• ${\displaystyle \lim _{x\to 0}x\ln x=0}${\displaystyle \lim _{x\to 0}x\ln x=0}, hence ${\displaystyle \lim _{x\to 0}x^{x}=1}${\displaystyle \lim _{x\to 0}x^{x}=1}
• ${\displaystyle \lim _{x\to \infty }{\frac {\ln x}{x}}=0}${\displaystyle \lim _{x\to \infty }{\frac {\ln x}{x}}=0}^[6]

For b > 1,

• ${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=-\infty }${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=-\infty }
• ${\displaystyle \lim _{x\to \infty }\log _{b}x=\infty }${\displaystyle \lim _{x\to \infty }\log _{b}x=\infty }

For b < 1,

• ${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=\infty }${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=\infty }
• ${\displaystyle \lim _{x\to \infty }\log _{b}x=-\infty }${\displaystyle \lim _{x\to \infty }\log _{b}x=-\infty }

Both cases can be generalized to:

• ${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=-F(b)\infty }${\displaystyle \lim _{x\to 0^{+}}\log _{b}x=-F(b)\infty }
• ${\displaystyle \lim _{x\to \infty }\log _{b}x=F(b)\infty }${\displaystyle \lim _{x\to \infty }\log _{b}x=F(b)\infty }

where ${\displaystyle F(x)=2H(x-1)-1}${\displaystyle F(x)=2H(x-1)-1} and ${\displaystyle H(x)}${\displaystyle H(x)} is the Heaviside step function

If ${\displaystyle x}${\displaystyle x} is expressed in radians:

• ${\displaystyle \lim _{x\to a}\sin x=\sin a}${\displaystyle \lim _{x\to a}\sin x=\sin a}
• ${\displaystyle \lim _{x\to a}\cos x=\cos a}${\displaystyle \lim _{x\to a}\cos x=\cos a}

These limits both follow from the continuity of sin and cos.

• ${\displaystyle \lim _{x\to 0}{\frac {\sin x}{x}}=1}${\displaystyle \lim _{x\to 0}{\frac {\sin x}{x}}=1}.^{[7] [8]} Or, in general,
  • ${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{ax}}=1}${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{ax}}=1}, for a not equal to 0.
  • ${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{x}}=a}${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{x}}=a}
  • ${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{bx}}={\frac {a}{b}}}${\displaystyle \lim _{x\to 0}{\frac {\sin ax}{bx}}={\frac {a}{b}}}, for b not equal to 0.
• ${\displaystyle \lim _{x\to \infty }x\sin \left({\frac {1}{x}}\right)=1}${\displaystyle \lim _{x\to \infty }x\sin \left({\frac {1}{x}}\right)=1}
• ${\displaystyle \lim _{x\to 0}{\frac {1-\cos x}{x}}=\lim _{x\to 0}{\frac {\cos x-1}{x}}=0}${\displaystyle \lim _{x\to 0}{\frac {1-\cos x}{x}}=\lim _{x\to 0}{\frac {\cos x-1}{x}}=0}^{[4] [8] [9]}
• ${\displaystyle \lim _{x\to 0}{\frac {1-\cos x}{x^{2}}}={\frac {1}{2}}}${\displaystyle \lim _{x\to 0}{\frac {1-\cos x}{x^{2}}}={\frac {1}{2}}}
• ${\displaystyle \lim _{x\to n^{\pm }}\tan \left(\pi x+{\frac {\pi }{2}}\right)=\mp \infty }${\displaystyle \lim _{x\to n^{\pm }}\tan \left(\pi x+{\frac {\pi }{2}}\right)=\mp \infty }, for integer n.
• ${\displaystyle \lim _{x\to 0}{\frac {\tan x}{x}}=1}${\displaystyle \lim _{x\to 0}{\frac {\tan x}{x}}=1}. Or, in general,
  • ${\displaystyle \lim _{x\to 0}{\frac {\tan ax}{ax}}=1}${\displaystyle \lim _{x\to 0}{\frac {\tan ax}{ax}}=1}, for a not equal to 0.
  • ${\displaystyle \lim _{x\to 0}{\frac {\tan ax}{bx}}={\frac {a}{b}}}${\displaystyle \lim _{x\to 0}{\frac {\tan ax}{bx}}={\frac {a}{b}}}, for b not equal to 0.
• ${\displaystyle \lim _{n\to \infty }\ \underbrace {\sin \sin \cdots \sin(x_{0})} _{n}=0}${\displaystyle \lim _{n\to \infty }\ \underbrace {\sin \sin \cdots \sin(x_{0})} _{n}=0}, where x₀ is an arbitrary real number.
• ${\displaystyle \lim _{n\to \infty }\ \underbrace {\cos \cos \cdots \cos(x_{0})} _{n}=d}${\displaystyle \lim _{n\to \infty }\ \underbrace {\cos \cos \cdots \cos(x_{0})} _{n}=d}, where d is the Dottie number. x₀ can be any arbitrary real number.

In general, any infinite series is the limit of its partial sums. For example, an analytic function is the limit of its Taylor series, within its radius of convergence.

• ${\displaystyle \lim _{n\to \infty }\sum _{k=1}^{n}{\frac {1}{k}}=\infty }${\displaystyle \lim _{n\to \infty }\sum _{k=1}^{n}{\frac {1}{k}}=\infty }. This is known as the harmonic series.^[6]
• ${\displaystyle \lim _{n\to \infty }\left(\sum _{k=1}^{n}{\frac {1}{k}}-\log n\right)=\gamma }${\displaystyle \lim _{n\to \infty }\left(\sum _{k=1}^{n}{\frac {1}{k}}-\log n\right)=\gamma }. This is the Euler Mascheroni constant.

• ${\displaystyle \lim _{n\to \infty }{\frac {n}{\sqrt[{n}]{n!}}}=e}${\displaystyle \lim _{n\to \infty }{\frac {n}{\sqrt[{n}]{n!}}}=e}
• ${\displaystyle \lim _{n\to \infty }\left(n!\right)^{1/n}=\infty }${\displaystyle \lim _{n\to \infty }\left(n!\right)^{1/n}=\infty }. This can be proven by considering the inequality ${\displaystyle e^{x}\geq {\frac {x^{n}}{n!}}}${\displaystyle e^{x}\geq {\frac {x^{n}}{n!}}} at ${\displaystyle x=n}${\displaystyle x=n}.
• ${\displaystyle \lim _{n\to \infty },2円^{n}\underbrace {\sqrt {2-{\sqrt {2+{\sqrt {2+\dots +{\sqrt {2}}}}}}}} _{n}=\pi }${\displaystyle \lim _{n\to \infty },2円^{n}\underbrace {\sqrt {2-{\sqrt {2+{\sqrt {2+\dots +{\sqrt {2}}}}}}}} _{n}=\pi }. This can be derived from Viète's formula for π.

Asymptotic equivalences, ${\displaystyle f(x)\sim g(x)}${\displaystyle f(x)\sim g(x)}, are true if ${\displaystyle \lim _{x\to \infty }{\frac {f(x)}{g(x)}}=1}${\displaystyle \lim _{x\to \infty }{\frac {f(x)}{g(x)}}=1}. Therefore, they can also be reframed as limits. Some notable asymptotic equivalences include

• ${\displaystyle \lim _{x\to \infty }{\frac {x/\ln x}{\pi (x)}}=1}${\displaystyle \lim _{x\to \infty }{\frac {x/\ln x}{\pi (x)}}=1}, due to the prime number theorem, ${\displaystyle \pi (x)\sim {\frac {x}{\ln x}}}${\displaystyle \pi (x)\sim {\frac {x}{\ln x}}}, where π(x) is the prime counting function.
• ${\displaystyle \lim _{n\to \infty }{\frac {{\sqrt {2\pi n}}\left({\frac {n}{e}}\right)^{n}}{n!}}=1}${\displaystyle \lim _{n\to \infty }{\frac {{\sqrt {2\pi n}}\left({\frac {n}{e}}\right)^{n}}{n!}}=1}, due to Stirling's approximation, ${\displaystyle n!\sim {\sqrt {2\pi n}}\left({\frac {n}{e}}\right)^{n}}${\displaystyle n!\sim {\sqrt {2\pi n}}\left({\frac {n}{e}}\right)^{n}}.

The behaviour of functions described by Big O notation can also be described by limits. For example

• ${\displaystyle f(x)\in {\mathcal {O}}(g(x))}${\displaystyle f(x)\in {\mathcal {O}}(g(x))} if ${\displaystyle \limsup _{x\to \infty }{\frac {|f(x)|}{g(x)}}<\infty }${\displaystyle \limsup _{x\to \infty }{\frac {|f(x)|}{g(x)}}<\infty }

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