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Common Limit Patterns

The following patterns are useful after checking the expression's domain and the direction of approach.

ExpressionLimit
lim⁡x→∞ex\displaystyle\lim_{x\to\infty} e^x∞\infty
lim⁡x→−∞ex\displaystyle\lim_{x\to-\infty} e^x00
lim⁡x→∞ln⁡x\displaystyle\lim_{x\to\infty}\ln x∞\infty
lim⁡x→0+ln⁡x\displaystyle\lim_{x\to0^+}\ln x−∞-\infty
lim⁡x→±∞bxr\displaystyle\lim_{x\to\pm\infty}\frac{b}{x^r}, r>0r>0 where defined00
lim⁡x→0sin⁡xx\displaystyle\lim_{x\to0}\frac{\sin x}{x}11
lim⁡x→01−cos⁡xx\displaystyle\lim_{x\to0}\frac{1-\cos x}{x}00
lim⁡x→0ex−1x\displaystyle\lim_{x\to0}\frac{e^x-1}{x}11

For a polynomial

p(x)=anxn+an−1xn−1+⋯+a0,p(x)=a_nx^n+a_{n-1}x^{n-1}+\cdots+a_0,

the leading term determines its end behavior. As x→∞x\to\infty, the sign is the sign of ana_n. As x→−∞x\to-\infty, an even degree preserves that sign and an odd degree reverses it.

For a rational function p(x)/q(x)p(x)/q(x), compare the polynomial degrees:

Degree comparisonLimit as x→±∞x\to\pm\infty
deg⁡p<deg⁡q\deg p<\deg q00
deg⁡p=deg⁡q\deg p=\deg qratio of leading coefficients
deg⁡p>deg⁡q\deg p>\deg qanalyze leading powers; the value is generally unbounded or has no finite limit

These are patterns, not replacements for hypotheses. One-sided behavior and domain restrictions still matter.

Using the patterns​

Trigonometric arguments must be in radians. For a constant k≠0k\ne0, set u=kxu=kx:

lim⁡x→0sin⁡(kx)x=klim⁡u→0sin⁡uu=k.\lim_{x\to0}\frac{\sin(kx)}{x} =k\lim_{u\to0}\frac{\sin u}{u}=k.

For k=0k=0, the quotient is identically zero for x≠0x\ne0. If angles are measured in degrees instead, the basic sine quotient has limit π/180\pi/180, not 11.

In the polynomial discussion, take an≠0a_n\ne0; growth to infinity requires n≥1n\ge1. A constant polynomial keeps its constant value. Degree comparisons assume nonzero polynomials p,qp,q; a zero numerator gives zero wherever the quotient is defined. The negative-infinity power pattern applies only when the chosen real power is defined arbitrarily far to the left (not, for example, x1/2x^{1/2}).

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