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Differential calculus - derivatives
 Applications of differentiation
 Taylor's theorem (Taylor's formula) - The extended mean value theorem

Suppose  f  is continuous on the closed interval [x0, x0 + h] with continuous derivatives to (n - 1)th order on the interval and its nth derivative defined on (x0, x0 + h) then,

is called Taylor's theorem. To prove Taylor's theorem we substitute  x0 = ax0 + h = b  and introduce the function

where Q is still undetermined and  p > 0. Since j (b) = 0 we can define Q by setting j (a) = 0 too,
then we compute j ' (x) to apply Rolle's theorem. Note that successive terms cancel (by the product rule) when differentiating j (x), so we get
  By Rolle's theorem there is some intermediate point c inside the interval [a, b] such that  j' (c) = 0,
which gives
By plugging the Q back into above equation j (a) = 0 while returning substitutions,
a = x0b = x0 + hb - a = h  and where
we obtain Taylor's theorem to be proved. The last term in Taylor's formula
is called the remainder and denoted Rn since it follows after n terms.
By plugging,  a)   p = n  into Rn  we get
the Lagrange form of the remainder,
     while if     b)   p = 1    we get
the Cauchy form of the remainder.
Thus, by substituting x0 + h = x  obtained is 
Taylor's formula with Lagrange form of the remainder.

Therefore, Taylor's formula gives values of a function f inside the interval [x0, x0 + h] using its value and the values of its derivatives to (n - 1)th order at the point x0 in the form

f (x) = Pn - 1(x - x0) + R n

where, Pn - 1(x - x0) is (n - 1)th order Taylor polynomial for f given by the first n terms in the above formula and Rn is one of the given remainders.

 Maclaurin's formula or Maclaurin's theorem
The formula obtained from Taylor's formula by setting x0 = 0
that holds in an open neighborhood of the origin, is called Maclaurin's formula or Maclaurin's theorem.
Consider the polynomial   fn(x) = anxn + an - 1xn - - - 1 + · · · a3x3 + a2x2 + a1x + a0,
let evaluate the polynomial and its successive derivatives at the origin,
f (0) = a0,     f '(0) = 1· a1,     f ''(0) = 1· 2a2,     f '''(0) = 1· 2· 3a3,  . . .  ,  f (n)(0) = n!an  
we get the coefficients,
Therefore, the Taylor polynomial of a function f centered at x0 is the polynomial of degree n which has the same derivatives as f at x0, up to order n.
If a function f is infinitely differentiable on an interval about a point x0  or the origin, as are for example  ex   and  sin x then,   P0 (x) = f (x0),
                          P1 (x) = f (x0) + (x - x0) f ' (x0),
 where  P0, P1, P2, . . . is a sequence of increasingly approximating polynomials for  f.
 
 
 
 
 
 
 
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