How do you use the Taylor Remainder term to estimate the error in approximating a function #y=f(x)# on a given interval #(c-r,c+r)#?

Answer 1
Assume that there exists a finite #M>0# such that
#|f^{(n+1)}(x)| le M#
for all #x# in #(c-r,c+r)#.
The error of approximating #f(x)# by the Taylor polynomial #p_n(x;c)# can be estimated by
#|f(x)-p_n(x;c)|#
#=|R_n(x;c)|#
#=|{f^{(n+1)}(z)}/{(n+1)!}(x-c)^{n+1}|#, where #z# is between #x# and #c#
#le M/{(n+1)!}r^{n+1}#

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Answer 2

To estimate the error in approximating a function ( y = f(x) ) on an interval ( (c - r, c + r) ) using the Taylor Remainder term, you would typically follow these steps:

  1. Find the Taylor series expansion of ( f(x) ) centered at ( x = c ). This involves finding the function's derivatives at ( x = c ).

  2. Write down the ( n )-th degree Taylor polynomial ( P_n(x) ) using the Taylor series expansion up to the ( n )-th term.

  3. The Taylor Remainder term, denoted by ( R_n(x) ), represents the error between the actual function ( f(x) ) and the Taylor polynomial ( P_n(x) ). It is given by the formula:

[ R_n(x) = f(x) - P_n(x) ]

  1. To estimate the error on the interval ( (c - r, c + r) ), evaluate the Taylor Remainder term ( R_n(x) ) at the endpoints of the interval, i.e., ( c - r ) and ( c + r ). This gives you the maximum possible error within the interval.
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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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