How do you find the taylor series series for #f(x)=lnx# at a=2?

Answer 1

First, we can start with the general definition of the Taylor series expansion, which is:

#sum_(n=0)^N f^((n))(a)/(n!)(x-a)^n#
where #f^((n))(a)# is the #n#th derivative of #f(x)# evaluated at #x -> a#, #n# varies, #a# does not, and #n!# is #1xx2xx3xxcdotsxx(n-1)xxn#. Note that #x->a# does not apply to #(x-a)^n# (yes, I've seen that happen).
Thus you have to take the derivative up to some #n#th order term. Let's say #n = 4#. Then you have:
#f^((0))(x) = f(x) = lnx# #f'(x) = 1/x# #f''(x) = -1/x^2# #f'''(x) = 2/(x^3)# #f''''(x) = -6/(x^4)#

Now you have the final result to simplify:

#sum_(n=0)^(4) = (f(2))/(0!)(x-2)^0 + (f'(2))/(1!)(x-2)^1 + (f''(2))/(2!)(x-2)^2 + (f'''(2))/(3!)(x-2)^3 + (f''''(2))/(4!)(x-2)^4 + ...#
#= (ln2) + (1/2)(x-2) + (-1/4)/(2)(x-2)^2 + (2/8)/(6)(x-2)^3 + (-6/16)/(24)(x-2)^4 + ...#
#= color(blue)(ln2 + 1/2(x-2) - 1/8(x-2)^2 + 1/24(x-2)^3 - 1/64(x-2)^4 + ...)#
Just remember the following: - #x->a# only for #f(a)#, not #(x-a)^n# - #n# varies, but #a# does not - It's probably wise to take the #n#th derivatives first so you aren't doing them as you are writing out the next step from the point you write out the general series formula
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Answer 2

#ln(2)+1/2(x-2)-1/8(x-2)^2+1/24(x-2)^3-1/64(x-2)^4+\cdots#

Use the following expression for the Taylor series of an infinitely differentiable function at #x=a#:
#f(a)+f'(a)(x-a)+(f''(a))/(2!)(x-a)^2+(f'''(a))/(3!)(x-a)^3+(f''''(a))/(4!)(x-a)^4\cdots#
Since #f(x)=ln(x)#, we get #f'(x)=1/x=x^{-1}#, #f''(x)=-x^{-2}#, #f'''(x)=2x^{-3}#, #f''''(x)=-6x^{-4}#, etc...
Since #a=2#, we calculate #f(2)=ln(2)#, #f'(2)=1/2#, #f''(2)=-1/4#, #f'''(2)=2/8=1/4#, #f''''(2)=-6/16=-3/8#, etc...

Therefore, we can write the answer as

#ln(2)+1/2(x-2)-1/8(x-2)^2+1/24(x-2)^3-1/64(x-2)^4+\cdots#
This series happens to equal #ln(x)# for #0 < x < 4# (the "radius of convergence" is 2 and it equals the function for these values as well).
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Answer 3

To find the Taylor series for ( f(x) = \ln(x) ) at ( a = 2 ), we start by finding the derivatives of ( f(x) = \ln(x) ) and evaluating them at ( x = 2 ) to obtain the coefficients of the Taylor series.

  1. First derivative of ( f(x) = \ln(x) ): ( f'(x) = \frac{1}{x} )
  2. Second derivative of ( f(x) = \ln(x) ): ( f''(x) = -\frac{1}{x^2} )
  3. Third derivative of ( f(x) = \ln(x) ): ( f'''(x) = \frac{2}{x^3} )
  4. Fourth derivative of ( f(x) = \ln(x) ): ( f''''(x) = -\frac{6}{x^4} )

Now, we evaluate these derivatives at ( x = 2 ):

  1. ( f'(2) = \frac{1}{2} )
  2. ( f''(2) = -\frac{1}{4} )
  3. ( f'''(2) = \frac{1}{4} )
  4. ( f''''(2) = -\frac{3}{16} )

Since ( f(a) = \ln(2) ) when ( a = 2 ), the first term of the Taylor series is ( \ln(2) ).

Therefore, the Taylor series for ( f(x) = \ln(x) ) at ( a = 2 ) is:

[ \ln(x) = \ln(2) + \frac{1}{2}(x - 2) - \frac{1}{8}(x - 2)^2 + \frac{1}{12}(x - 2)^3 - \frac{1}{32}(x - 2)^4 + \cdots ]

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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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