Sequences, series, and function approximation
Maclaurin series and Euler's identity
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Cosine Taylor series at 0 (Maclaurin)
Approximating f(x)=cos x using a Maclauren Series (special case of a Taylor series at x=0)
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At 5:31, how is the moon large enough to block the sun? Isn't the sun way larger?

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I could understand the steps, end result, but a question as to how some function determined at 0 is valid over the full range. What I feel is since cosine is periodic function this holds true. Someone correct me if I am wrong.
Two points.
1. If you look at the pattern of your derivatives, you'll see that after 4 derivatives, it goes back to it's original derivative, which means that it will just continue to repeat this pattern no matter how far you go out.
2. It then has to do with the series representation. If you look at the series representation, you'll see that it's E ((1)^k)*x^2k)/(2k!). This is for all k's. You'll notice that the x is just x^2k. If it were (x^2k)3, then it would be centered at 3. The formula for "power" series is E an(xc)^n. If there is no "c" in the series representation, then the function is centered at 0.
Hope this made some sense.
1. If you look at the pattern of your derivatives, you'll see that after 4 derivatives, it goes back to it's original derivative, which means that it will just continue to repeat this pattern no matter how far you go out.
2. It then has to do with the series representation. If you look at the series representation, you'll see that it's E ((1)^k)*x^2k)/(2k!). This is for all k's. You'll notice that the x is just x^2k. If it were (x^2k)3, then it would be centered at 3. The formula for "power" series is E an(xc)^n. If there is no "c" in the series representation, then the function is centered at 0.
Hope this made some sense.
You have to remember that we are not just taking the value of the FUNCTION at 0, but also of all its derivatives, which basically means that you are given the slope of the function at 0, (and plotting the values of the slopes at a bunch of different points in the graph, you would end up with a derived function, which you could then take the first derivative of (i.e. the second derivative of the original function), and a derived function out of all the points you get from that, then take the slope of lots of points in THAT derived function, and you would get another derived function (i.e. the THIRD derivative of the original function.)) Anyway, you are given the function AND all these derivatives, so although a function value at a certain point may not, alone, be a valid representation for the entire function, the value AND ALL ITS DERIVATIVES will be a valid representation for the entire function.
I'm sorry if I confused you.
I'm sorry if I confused you.
So... the Taylor Series is a way to represent a function? :S
With Taylor and Maclaurin series you can approximate a function with a polynomial. This is useful because you can turn a complicated function (defined by a limit, for example) into simple multiplication and exponentiation of numbers. That's how your calculator gets the sine and cosine of angles almost immediately: It doesn't have a table of sines and cosines for all possible values, it approximates them using Taylor/Maclaurin series
it is a way to approximate a function, the more terms you have the better the approximation
This is supposed to approximate the function cos(x). Does it approximate the entire function all the way to infinity, or only near x=0?
There are methods for determining the maximum size of the error produced by an approximation like this, so you can figure out how many terms you need to have in order to get an approximation within the tolerance you desire. Hopefully Sal will cover those in an upcoming video. Also, cos x is periodic, so if you can get within your desired tolerance on, say, the interval from 0 <= x <= 2 pi, then you can just shift over any multiple of 2 pi to get your approximation if your x lies outside that int
How is Maclaurin and Taylor Series related to Complex Number's Polar Form, given that they share the same playlist?
I'm honestly not getting what the relation between these two might be.
I'm honestly not getting what the relation between these two might be.
Very cool concept but I'm wondering if you can do it in reverse, take an infinite polynomial and turn it into a simple function?
Why exactly does taking derivatives at a point give you the function of the polynomial? I don't get the part of how the 3rd,4th,5th etc. derivative will attempt to match the slope at any point other than at zero, is it because the slope of the slope at zero approximates the points around it?
Here's the basic idea: Hm, I wonder if I can make a polynomial that has all of the same derivatives at a point as a particular function? Look at that, now we can.
And here's a bonus: it even looks like the function! In fact, for certain functions, I can "tailor" (pun intended) an infinite polynomial that exactly equals the function at all values of x just by this process of creating a polynomial with the same derivatives as my function.
And here's a bonus: it even looks like the function! In fact, for certain functions, I can "tailor" (pun intended) an infinite polynomial that exactly equals the function at all values of x just by this process of creating a polynomial with the same derivatives as my function.
Think about how the first derivative gives you the slope at a point, and then the second derivative gives you the concavity of the function, and the third derivative will give you the concavity of the first derivative, and so on. Also, remember from the first video that we assume the function is infinitely differentiable.
Another video in this series will probably help more: https://www.khanacademy.org/math/calculus/sequences_series_approx_calc/maclaurin_taylor/v/visualizingtaylorseriesapproximations
Another video in this series will probably help more: https://www.khanacademy.org/math/calculus/sequences_series_approx_calc/maclaurin_taylor/v/visualizingtaylorseriesapproximations
I transformed that last polynomial equation ( produced after the Mac Lauren series was applied ) and transformed it into a power series summation ( like Sal taught us on his last playlist), and I got :
Summation from n=0 to infinity of  ( x^2 / 2n! )^n , which is 1 / [ 1 + ( x^2/2n! )] with radius of convergence x < sqrt( 2n! ).
So my question is, is that correct? Can we represent cos(x) three different ways (MacLaurin polynomial, power series(sigma notation), power series summation after applying the formula 1 / 1r ) ??
Summation from n=0 to infinity of  ( x^2 / 2n! )^n , which is 1 / [ 1 + ( x^2/2n! )] with radius of convergence x < sqrt( 2n! ).
So my question is, is that correct? Can we represent cos(x) three different ways (MacLaurin polynomial, power series(sigma notation), power series summation after applying the formula 1 / 1r ) ??
At around 2:15 he states that the steps work whether you are using radians or degrees, but it doesn't seem reasonable that the polynomial will give you the same answer whether you use x = pi/2 or x=90. Is there some reason that you makes this approximation work specifically with radians?
That is only because you are dealing with an angle of 0, which is the same in radians and degrees. For any other angle, you need to use radians. At this level of study, degrees should not be used at all.
If calculators use a MacLauren series to approximate trig functions, how come when I graph cos x it takes a couple seconds, but when I graph the first 10 terms of it's MacLauren series it takes around half a minute? Does it have to do with the fact that trig functions are periodic, and hence the series only needs to be accurate between pi and pi and then can be horizontally translated to find the cosine of angles outside that domain?
Calculators use a method called CORDIC to compute the trig functions. While this method is quite good for the way that computers process numbers, it isn't really very good for the way that humans do computations by hand. So, that is why it is not routinely taught in math classes.
So, no, calculators do not use Maclaurin series for the trig functions.
So, no, calculators do not use Maclaurin series for the trig functions.
Why would I want to approximate the value of sin(x) or e^x when I can find an exact values?
"when I can find an exact value"
You can? How?
You can? How?
These functions are simple enough. But more complex functions are better approximated as polynomials.
Why when we approximate the cosine function with polynomials it works so much better than approximating the sine function? (I can send my approximations in the graph I made, email me if possible)
It also depends on what order term you use for an approximation. At order 1 (linear approximation), you get a better approximation for sine than cosine (y = x works better for sine than y = 1 works for cosine). But if you include second order terms (quadratic approximation) you do better with cosine because sine doesn't have a second order term.
How fast any particular Taylor series converges depends on the value of x. Thus, the number of terms you need to get the series to converge to an acceptable number of number of decimal places, depends on what value the x is.
But, the Taylor series for both cosine and sine converge very quickly, so I am not sure what you mean.
But, the Taylor series for both cosine and sine converge very quickly, so I am not sure what you mean.
please i could not solve these questions , to expand the function f(x)= Cos2 3x at x0=0
sum of cos (2kpi/(2n+1))= 1/2 from [k=1, n]
How can cos(x) in degrees and cos(x) in radians have the same serie if one finish its cycle at 2 pi and the other in 360. That would mean that if you plug pi to the serie it will give the same result as 180!!
MADNESS I SAY!
MADNESS I SAY!
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