How about Why does the Landau notation for division work when h approaches 0?

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SUMMARY

The discussion focuses on the behavior of the Landau notation for division as the variable h approaches 0. Specifically, it establishes that the expression frac{a+\mathcal{O}(h^2)}{b+\mathcal{O}(h^2)} = \frac{a}{b}+\mathcal{O}(h^2) holds true, clarifying that the \mathcal{O}(h^2) term does not simplify to \mathcal{O}(1). The analysis includes a power series expansion of the fraction c = \frac{a + k1h^2}{b + k2h^2}, demonstrating that the leading term remains \frac{a}{b} with the error term being \mathcal{O}(h^2).

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IniquiTrance
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Why is it that,

##
\frac{a+\mathcal{O}(h^2)}{b+\mathcal{O}(h^2)} = \frac{a}{b}+\mathcal{O}(h^2)
##

as ##h\rightarrow 0##? It seems like the ##\mathcal{O}(h^2)## term should become ##\mathcal{O}(1)##.
 
IniquiTrance said:
Why is it that,

a+(h2)b+(h2)=ab+(h2) \frac{a+\mathcal{O}(h^2)}{b+\mathcal{O}(h^2)} = \frac{a}{b}+\mathcal{O}(h^2)

as h→0h\rightarrow 0? It seems like the (h2)\mathcal{O}(h^2) term should become (1)\mathcal{O}(1).


Think about this very simple illustration. Consider the specific case

<br /> c = \frac{a + k1h^2}{b + k2h^2}<br />

with k1, k2 positive (specific choices for the second terms in numerator and denominator, but since h-squared is the key term it's find. Bear with me.)

Suppose that fraction is expanded into a power series in h. The first few terms are

<br /> \frac a b −\frac{((ak2−bk1)h^2)}{b^2}+\frac{((ak2^2−bk1k2)h^4)}{b^3}−\frac{((ak2^3−bk1k2^2)h^6)}{b^4}+\frac{((ak2^4−bk1k2^3)h^8)}{b^5}+... = \frac a b + O(h^2)<br />
 

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