suivant: Series expansion : series
monter: Taylor and asymptotic expansions
précédent: Division by increasing power
Table des matières
Index
Taylor expansion : taylor
taylor takes from one to four arguments :
- an expression dependending of a variable (by default x),
- an equality variable=value (e.g. x = a) where to compute
the Taylor expansion, by default x=0,
- an integer n, the order of the series expansion,
by default 5
- a direction -1, 1 (for unidirectional series expansion)
or 0 (for bidirectional series expansion) (by default 0).
Note that the syntax ...,x,n,a,...
(instead of ...,x=a,n,...) is also accepted.
taylor returns a polynomial in x-a, plus a remainder
of the form:
(x-a)^
n*order_size(x-a)
where order_size is a function such that,
For regular series expansion, order_size is a bounded function,
but for non regular series expansion, it might tend slowly to
infinity, for example like a power of ln(x).
Input :
taylor(sin(x),x=1,2)
Or (be carefull with the order of the arguments !) :
taylor(sin(x),x,2,1)
Output :
sin(1)+cos(1)*(x-1)+(-(1/2*sin(1)))*(x-1)^
2+ (x-1)^
3*order_size(x-1)
Remark
The order returned by taylor may be smaller than n if
cancellations between numerator and denominator occur, for example
taylor(
)
Input :
taylor(x^
3+sin(x)^
3/(x-sin(x)))
The output is only a 2nd-order series expansion :
6+-27/10*x^2
+x^
3*order_size(x)
Indeed the numerator and denominator valuation is 3, hence we loose 3
orders. To get order 4, we should ask n = 7, input :
taylor(x^
3+sin(x)^
3/(x-sin(x)),x=0,7)
Output is a 4th-order series expansion :
6+-27/10*x^
2+x^
3+711/1400*x^
4+x^
5*order_size(x)
suivant: Series expansion : series
monter: Taylor and asymptotic expansions
précédent: Division by increasing power
Table des matières
Index
giac documentation written by Renée De Graeve and Bernard Parisse