The behavior of a number-theoretic function
for large
is often
difficult to determine because the function values can fluctuate considerably
as
increases. It is more fruitful to study partial sums and seek
asymptotic formulas
of the form
where
is a known function of
, and
represents the
error, a function of smaller order than
for all
in some prescribed
range. For example, Dirichlet (1849) proves that for all
,
where
is Euler’s constant (§5.2(ii)).
Dirichlet’s divisor problem
(unsolved in 2009) is to determine
the least number
such
that the error term in (27.11.2) is
for all
. Kolesnik (1969) proves that
.
Equations (27.11.3)–(27.11.11) list further
asymptotic formulas related to some of the functions listed in
§27.2. They are valid for all
. The error terms given
here are not necessarily the best known.
where
again is Euler’s constant.

where
is a constant.
where
,
, and
is a constant depending on
and
.
where
,
.