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Interesting properties of nested functions 
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#1
Oct1111, 11:46 PM

P: 66

The properties arise from infinitely nested functions such as:
[itex]x=\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}}[/itex] You can solve it algebraically to verify that x is equal to the nested function (all of the following functions can be solved in a similar manner).Simply raise both sides to the n^{th} power: [itex]x^n=x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}[/itex] Divide through by x^{n1}: [itex]x=\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}[/itex] What we will do is explore the properties of finitely iterated nestings. The variable a is used to denote the number of nestings. For this example, a=4: [itex]f(x,n,a)=f(x,n,4)=\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}}}}} [/itex] The interesting properties arise when we subtract a nested function from the number it equals at infinite nestings (x). With this particular variety of nesting: [itex]f(x,n,a) = x\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1...}}}}} [/itex] We end up approaching [itex]n^{a}x\ln{x}[/itex] as a gets larger. It approaches the value quicker for higher n and x. f(x,n,a)/f(x,n,a+1) approaches n as a increases. There are many multiplicative nested type equations we can try, such as: [itex]x=\log_B [ B^x\log_B [B^x \log_B [B^x....]]][/itex] so [itex]f(x,B,a)=x\log_B [ B^x\log_B [B^x \log_B [B^x....]]][/itex] which has the interesting property: [tex]\dfrac{f(x,B,a)}{f(x,B,a+1)}\to x \ln B[/tex] Of course, there are whole other types of nested functions using addition/subtraction, in addition to multiplication (if you mix them). You can do cosine and cosine^{1} together, x^{n} and x^{1/n} and other combinations. This next formulas approach the derivative of the inner functions when taking [itex]\dfrac{f(...,a)}{f(...,a+1)}[/itex] for higher a. For this one, the inner function is x^n: [tex]f(x,n,a)=x\sqrt[n]{x^{n}x+\sqrt[n]{x^{n}x+\sqrt[n]{x^{n}x+\sqrt[n]{x^{n}x+...}}}}[/tex] so [tex]\dfrac{f(x,n,a)}{f(x,n,a+1)}\to nx^{n1}[/tex] For this one, the inner function is B^{x}: [tex]f(x,B,a)=x\log_B [B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [...]]]][/tex] so [tex]\dfrac{f(x,B,a)}{f(x,B,a+1)}\to B^{x}\ln B[/tex] as a increases (or for larger B and x). In fact, all of the basic formulas that use  x + (the repeated formula....) appear to approach the derivative of the inner formula for f(...,a)/f(...,a+1) except in conditions when the functions and inverse functions used have limited well defined domains (such as cosine and cosine^{1}). Combining the functions results in approaching the derivative of the combined inner function: [tex]f(x,B,a)=x\sqrt[n]{\log_B [ B^{x^n}x+ \sqrt[n] {\log_B [B^{x^n}x+ \sqrt[n]{ \log_B [B^{x^n}x+...}}}]]][/tex] Note that it is set up to take x^n first, then take B^(x^n) next (as if it were infinitely iterated so that it is algebraically sound). The "[" symbol doesn't show up to clearly under the radical. Anyways.... As with the other x + ... functions, this one approaches the derivative of the inner function [itex]B^{x^n}[/itex] [tex]\dfrac{f(x,B,a)}{f(x,B,a+1)}\to n\,{x}^{n1}\,{y}^{{x}^{n}}\,log\left( y\right)[/tex] For all of these functions, the exact approached value (so for x^n as the inner function, nx^(n1) ) for f(...,a)/f(...,a+1) can be taken to the a^{th} power (number of iterations) and multiplied by f(....,a) to create a constant. Haven't found a rational one yet. Not a lot of them are listed over at the inverse symbolic calculator, although for the x^nx+.... one, with x and n equal to 2, you end up with pi^2/4. Note that a value more or less than the value that f(...,a)/f(...,a+1) approaches causes the calculated constant to diverge towards 0 or infinity as a increases [UNLESS you use the exact constant (such as the derivatives, or n for the first example, x ln (B) for the second, etc.)]. 


#2
Oct2811, 10:46 PM

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P: 3,252

One way to motivate your method is: For [itex] x \ge 0 [/itex] and [itex] n [/itex] a positive integer [eq. 1] [itex] x = \sqrt[n]{x^n} = \sqrt[n]{x^{n1} x } [/itex] Use eq. 1 to substitute for the term x in the right hand side of eq. 1. We obtain [eq. 2] [itex] x = \sqrt[n]{x^{n1} \sqrt[n]{x^{n1} x} } [/itex] Use eq 1 to substitute for the term x in the right hand side of eq 2. We obtain [eq. 3] [itex] x = \sqrt[n]{x^{n1} \sqrt[n]{x^{n1} } \sqrt[n]{x^{n1} x }} [/itex] Continuing the above process suggests (but does not prove) that x is equal to the "infinitely nested" function given in your first equation. Define a sequence of functions [itex] \{f_i\} [/itex] recursively as follows: [itex] f_1(x) = \sqrt[n]{x^{n1}} [/itex] For [itex] j > 1 [/itex] , [itex] f_j(x) = \sqrt[n]{x^{n1} f_{j1}(x) } [/itex] Your claim is that for each [itex] x \ge 0 [/itex], [itex] \lim_{j \rightarrow \infty} f_j(x) = x [/itex] 


#3
Oct2911, 04:21 PM

P: 66

Incidentally, this isn't the point I was bringing up, and as of yet I have not come up with a valid proof for the derivative conjecture, which is the most interesting property of nested functions. The derivative conjecture can be readily tested (although inductive "validity" is more than a little nonrigorous), and stands up to all tests I've thrown at it (within specific domains for various functions), I'm just drawing a blank (for now) on how to prove it. As to this little gem: [tex]x=\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}}[/tex] Take both sides to the nth power: [tex]x^n=x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}}[/tex] Note that you still have the infinitely nested radical after the [itex]x^{n1}[/itex] part. Once you divide [itex]x^{n1}[/itex] on both sides of the equation, you end up with your original equation of x= infinitely nested radical. I actually wrote out a rough proof for this particular radicals interesting tendency towards [tex] ln{x} =\lim_{a\to\infty} \dfrac{x \sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}} }{x} \times n^a[/tex] with a being the number of iterations of the radical As you probably know, you can "force multiply" (I think that's similar to how McGuffin put it) through radicals. For example: [tex] \sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}} = \sqrt[{n^2}]{x^{n^21}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}[/tex] An easier example: [tex]2\, \sqrt[2]{2} = \sqrt[2]{2^2 \times 2}[/tex] As you can see, to force multiply a number into a radical, you take it to the power of the radical. When you have multiple radicals together, such as [itex]2\, \sqrt[2]{2\sqrt[2]{2}} = \sqrt[2]{8\,\sqrt[2]{2}}= \sqrt[4]{8^2 \times 2}[/itex], as you push the number through the radical, instead of leaving stacked radicals like [itex]\sqrt[2]{\sqrt[2]{x}}[/itex] you can concentrate them under a single radical (square root of a square root is the 4th root): [itex]\sqrt[4]{x}[/itex]. For the above nested radical of a nestings, we end up with the following: [tex] x^{\frac{n^a1}{n^a}} = \sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}\sqrt[n]{x^{n1}...}}}}[/tex] Of course: [tex]x^{\frac{n^a1}{n^a}} =x^{\frac{n^a}{n^a}} \times x^{\frac{1}{n^a}}=x \times x^{\frac{1}{n^a}}[/tex] Therefore dividing [itex]x x^{\frac{n^a1}{n^a}}[/itex] by x will result in: [itex]1x^{\frac{1}{n^a}}[/itex]. Multiplying this quantity by n^{a} results in the following equation: [itex]\left( 1x^{\frac{1}{n^a}} \right) \times n^a[/itex] And if we take the limit as [itex]n^a\to\infty[/itex] we end up with a very familiar looking equation (one of the formulas for natural log of a number). Back to the original problem with lack of proof that x= so and so infinitely nested radical, you can look at [itex]x^{\frac{n^a1}{n^a}}[/itex]. As [itex]\lim_{n^a\to\infty} \dfrac{n^a1}{n^a}=1[/itex] therefore [itex] \lim_{n^a\to\infty} x^{\frac{n^a1}{n^a}} = x^1 = x[/itex] 


#4
Oct2911, 08:12 PM

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P: 3,252

Interesting properties of nested functions
For example, if we assert: 1 = 1  1 + 1  1 + 1...... We can add (1  1) to both sides obtaining 1 + 1  1 = (1 1) + 1  1 + 1  1 + .... 1 = 1  1 + 1  1 + .... Which is the original equation. But that doesn't establish the correctness of the original equation. But before we get to that, how general is the possibility of expressing the identity function as an infinite recursion of other functions? Do you think things could be as general as this: Hypothesis: Let [itex] g(x,y) [/itex] be a real valued function of two real variables whose partial derivatives exist and are continuous. Further suppose that [itex] g(x,x) = x [/itex]. Concluson (?): Then there exists a constant k such that the sequence of functions [itex]\{ f_i\}[/itex] defined recursively by: [itex] f_1(x) = g(x,k) [/itex] For [itex] j > 1[/itex], [itex] f_j (x) = g(f_{j1}(x),k) [/itex] has the property that for all [itex] x, [/itex] [itex] \lim_{j \rightarrow \infty} f_j(x) = x [/itex] Of course, I'm just trying to make a generalization based on the case [itex] g(x,y) = \sqrt[n]{x^{n1} y} [/itex] and [itex] k = 1 [/itex]. 


#5
Oct3111, 03:41 PM

P: 66




#6
Oct3111, 05:10 PM

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P: 3,252

So if I want to begin a recursive definition based on the above thinking, I can't say "Let [itex] f_1(x) = g(x) [/itex]" because I'm missing a variable in [itex] g [/itex]. Looking at your examples, it appears that I can realize them by saying "Let [itex] f_1(x) = g(x,k) [/itex]" if I pick the right value of the constant k. 


#7
Oct3111, 11:05 PM

P: 66

I'm still drawing a complete blank on why you would need an additional constant?
I don't use one in any of the functions, although I do specify a specific nesting depth of a (or call it recursivity depth). Now, all of the functions with the interesting derivative property are of the form: [itex]x= f^{1}(f(x)x + f^{1}(f(x)x+...))[/itex] so that we apply the function to both sides: [itex]f(x)= f\left( f^{1}(f(x)x + f^{1}(f(x)x+...))\right)[/itex] which ends up as: [itex]f(x)= f(x)x+ f^{1}(f(x)x + f^{1}(f(x)x+...))[/itex] so that we can subtract [itex]f(x)x[/itex] from both sides and end up with the original equation. If you are trying to specify a nesting depth, or recursivity depth such that: [tex]f_1(x)=f^{1}(f(x)x)[/tex] [tex]f_2(x)= f^{1}(f(x)x + f^{1}(f(x)x))[/tex] I've been calling the depth a, so the first is: [tex]f(x,a) = f(x,1) = f^{1}(f(x)x)[/tex] [tex]f(x,2) = f^{1}(f(x)x + f^{1}(f(x)x))[/tex] Another way of specifying depth is (with [itex]f_0(x)=0[/itex]): [tex]f_n(x)=f^{1}(f(x)x+f_{n1}(x))[/tex] which should strike you as resembling Fibonacci sequence or Mandelbrot set syntax. Here is a quick example (note that the original post has both an incorrect and correct version of the following formula). Note that [itex]f(x,B)=B^x[/itex] and [itex]f^{1}(x,B)=\log_B(x)[/itex] [tex]x=\log_B [B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [...]]]][/tex] [tex]B^x=B^{\log_B [B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [...]]]]}[/tex] [tex]B^x=B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [...]]]][/tex] subtract B^xx from both sides and you end up with the original equation: [tex]x=\log_B [B^xx+\log_B [B^xx+\log_B [B^xx+\log_B [...]]]][/tex] Another side note, the multiplicative infinite nestings of the form: [itex]x= f^{1}(\frac{f(x)}{x} \times f^{1}(\frac{f(x)}{x} \times f^{1}(...))[/itex] don't appear to display the derivative property (at least for the few I've analyzed there is no rigorous proof against this as of yet). 


#8
Nov111, 12:45 AM

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P: 3,252

There are certainly other attempts to state what your are doing in general terms. Another attempt is this: Write [itex] x = f^{1}(f(x)) [/itex] for some invertible function [itex] f[/itex]. Find a function [itex] g(x,y) [/itex] such that [itex] g(x,0) = f(x) [/itex] Define the sequence of functions [itex] \{f_i\} [/itex] by: [itex] f_1(x) = f^{1}(g(x,x)) [/itex] For [itex] j > 1[/itex], [itex] f_j(x) = f^{1}( g(x,x) + f_{j1}(x)) [/itex] I don't know if that approach works. All I'm saying is that it is one way to generalize your example ( by using [itex] g(x,y) = f(x)  y [/itex]). Can you state the most general procedure for expessing the identity function as the limit of a sequence of recursively defined functions? (And can you do it without using "infinite" symbolic expressions with "..."'s in them?) If I start with the equation [itex] A = B [/itex] and apply [itex] f [/itex] to both sides, I get [itex] f(A) = f(B) [/itex] Since [itex] f(A) = f(B) [/itex] then [itex] A  f(A) = B  f(B) [/itex], so I can subtract [itex] A  f(A) [/itex] from the left and [itex] B  f(B) [/itex] from the right and get the original equation. Instead of that argument, what you are trying to express has something to do with the "algebraic form" of the terms in equation. That's the type of mathematics one sees when people talk about "formal" power series. You're just supposed to treat them as strings of symbols and not worry about convergence. You are demonstrating something about the behavior of symbols. However, if you are trying to prove something about derivatives, I think you must eventually express the ideas in a way that acceptable for doing proofs involving convergence, epsilons and deltas etc. 


#9
Nov111, 01:59 AM

P: 66

[tex]g_n(x) = f^{1}\left(f(x)x+g_{n1}(x)\right)[/tex] [tex]x= \lim_{n\to\infty} g_n(x)[/tex] It's very similar for the multiplication/division identity functions (proof/demo if requested): [tex]g_0(x) = 1[/tex] [tex]g_n(x) = f^{1}\left(\frac{f(x)}{x} \times g_{n1}(x)\right)[/tex] [tex]x= \lim_{n\to\infty} g_n(x)[/tex] Statement: "all of the functions with the interesting derivative property are of the form:" [tex]1.\,x= f^{1}(f(x)x + f^{1}(f(x)x+...))[/tex] Then I simply showed how the equation works, in case someone jumped in at this point. Apply the function to both sides of the equation: [tex]2.\,f(x)= f\left( f^{1}(f(x)x + f^{1}(f(x)x+...))\right)[/tex] [tex]3.\,f(x)= f(x)x+ f^{1}(f(x)x + f^{1}(f(x)x+...))[/tex] Once we subtract f(x)x from both sides of equation 3, we end up with equation 1 again. We could also add f(x)x to both sides of equation 1 and arrive at equation 3, then apply the inverse function to both sides to arrive at equation 1. The wikipedia demonstration which leads to [itex]x=\sqrt{2+x}[/itex] is but one of many possible forms of this type of equation. Specifically [itex]f(x)=x^2[/itex], [itex]f^{1}(x)=\sqrt{x}[/itex] and lastly, with x=2: [tex]x = \sqrt{x^2x+\sqrt{x^2x+...}} = \sqrt {2 +\sqrt{2+...}} = \sqrt{2 +x}[/tex] 


#10
Nov111, 03:28 AM

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P: 3,252

I'll take a shot at it. We start with an equation of the form [itex] x = f^{1}[/itex](some stuff). We apply f to both sides obtaining [itex]f(x) =[/itex] (some stuff) Then we do some operation to both sides of the equation that converts [itex] f(x) [/itex] to [itex] x [/itex] and the (some stuff) to (some other stuff). We find that, as infinite strings of symbols, (some other stuff).is equal to [itex] f^{1}[/itex] (some.stuff). So what we are demonstrating is not something about showing numerical equality. We aren't proving that the first equation is correct. We are showing something about the transformation properties of an infinite string of symbols. (And for purposes of mathematics like calculus that worries about things like convergence, demonstrations like this are not formal proofs. As far as I can see the Wikipedia and the Wolfram page you cited don't give formal proofs. The Wolfram page has references for the results it states. What is acceptable as a formal proof could be determined by what is in those references.) What I find hard to forumulate in precise mathematical terms is my statement that we apply "an operation" to both sides of the equation. If we wanted an operation to change f(x) to x, the natural operation would be to take [itex] f^{1} [/itex] of both sides. But that's not what we do. We do something like divide by [itex] x^{n1} [/itex] or subtract [itex] f(x)  x [/itex]. What is a precise way to express "an operation" in a general way that includes both those examples as special cases? 


#11
Nov211, 01:36 AM

P: 66

[tex] x = f^{1}\left ( 2 \times f(x)  \dfrac{f(x)}{x} \times f^{1} \left ( 2 \times f(x)  \dfrac{f(x)}{x} \times r(x) \right ) \, \right)[/tex] First apply function f to both sides: [tex] f(x) = 2 \times f(x)  \dfrac{f(x)}{x} \times f^{1} \left ( 2 \times f(x)  \dfrac{f(x)}{x} \times r(x) \right ) [/tex] subtract [itex]2 \times f(x)[/itex] from both sides: [tex] f(x) =  \dfrac{f(x)}{x} \times f^{1} \left ( 2 \times f(x)  \dfrac{f(x)}{x} \times r(x) \right ) [/tex] divide both sides by [itex]\dfrac{f(x)}{x}[/itex]: [tex]  \dfrac{f(x) \times x}{f(x)} = x = f^{1} \left ( 2 \times f(x)  \dfrac{f(x)}{x} \times r(x) \right ) [/tex] Remembering that r(x) is the infinitely repeated function sequence. 1) Let's call the infinitely nested function r(x) 2) For x to be equal to r(x), we must be able to apply the same functions to both r(x) and x and arrive back at x= r(x) a. these functions must denest or nest a portion of r(x) or we run the risk of doing something circular (or trivial) such as your "parody" example (trivial or circular manipulation as in: add 1 to both sides, multiply both sides by 2, subtract 2 from both sides, divide both sides by 2) b. when [itex]x=r(x)=\sqrt{x^2x+\sqrt{x^2x+...}}[/itex] we must be able to either add a recursion to r(x), or remove a recursion: i. to add a recursion to this example subtract x from both sides [itex] x  x = 0 = x + \sqrt{x^2x+\sqrt{x^2x+...}}[/itex] ii. add x^2 to both sides [itex] xx+x^2 = x^2 = x^2x + \sqrt{x^2x+\sqrt{x^2x+...}}[/itex] iii. take the square root of both sides [itex]\sqrt{x^2} = x = \sqrt{x^2x+\sqrt{x^2x+...}}[/itex] Do the inverse operations in reverse order to remove a recursion (square both sides, subtract x^2 from both sides, add in x to both sides). Remember x must be equal to one recursion + x (since x is equal to an infinite recursion). Therefore one should be able to remove one recursion and have the same formula. I'll show you 2 examples of why the following infinite recursion does NOT work for non trivial solutions: [tex]x=\sqrt{x^3x+\sqrt{x^3x+...}}[/tex] which should be equal to the following equation if the infinite recursion [itex]\sqrt{x^3x+\sqrt{x^3x+...}}[/itex] is equal to x [tex]x=\sqrt{x^3x+x}[/tex] square both sides: [itex]x^2=x^3x+x[/itex] in other words [itex]x^2=x^3[/itex] which is only valid for the trivial solution of x=0 (not for the invalid solution x=1, which ends up with 1=0, even for certain valid formulas (x=1 is not in the domain for these formulas)): [tex] 1= \sqrt{1^31+\sqrt{1^31+...}} = \sqrt{0+\sqrt{0+...}}[/tex] Also note that there is no way to remove or add a recursion from this formula without altering it, nontrivial manipulation simply leads to a new formula: [tex]x=\sqrt{x^3x+\sqrt{x^3x+...}}[/tex] [tex]x^2=x^3x+\sqrt{x^3x+\sqrt{x^3x+...}}[/tex] notice we end up with x being equal to something else (although it still works for the trivial solution of 0): [tex]x=x^3x^2+\sqrt{x^3x+\sqrt{x^3x+...}}[/tex] 1) assume an algebraically valid non trivial infinite nest x= r(x) within valid domain and range of functions in r(x) !!! 2) adding or removing a nesting from r(x) must result in the original equality x=r(x) For example, the following additive portion: [itex]x^2x[/itex] is not the whole identity function for that particular function. You add that in then take the square root of both sides, so the identity function of this particular function involves more than one step. [itex]x=\sqrt{x^2x+\sqrt{x^2x+...}}[/itex] [itex]x+x^2x=x^2x+\sqrt{x^2x+\sqrt{x^2x+...}}[/itex] [itex]x^2=x^2x+\sqrt{x^2x+\sqrt{x^2x+...}}[/itex] square root: [itex]x=\sqrt{x^2x+\sqrt{x^2x+\sqrt{x^2x+...}}}=\sqrt{x^2x+\sqrt{x^2x+...}}[/itex] Here's a neat fact about the formula right above this sentence. Setting x equal to the golden ratio gives you the nested root formula for the golden ratio, since [itex]\phi^2\phi=1[/itex]. Check equation 14 on the Mathworld Golden Ratio website. Setting x=2, you get part of a formula for pi that you can check out at Mathworld's Pi Formulas website (formula 66*). In fact, many different constants can be made from these various equations. 


#12
Nov211, 10:15 AM

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P: 3,252

For example, you showed that this equation "works": [tex] x = f^{1}( f(x)  x + f^{1}(f(x) x + ....) [/tex] Let [itex] f(x) = x [/itex] Define [itex] g_0(x) = 0 [/itex] [itex] g_{n}(x) = f^{1}( f(x) x + g_{n1}(x) ) [/itex] Then we have: [itex] g_0(x) = 0 [/itex] [itex] g_1(x) = f^{1}(x  x + 0) = f^{1}(0) = 0 [/itex] [itex] g_2(x) = f^{1}(x  x + g_1(x)) = f^{1}(0 + 0) = 0 [/itex] etc. The statement: [itex] x = \lim_{n \rightarrow \infty} g_n(x) [/itex] is false except at [itex] x = 0 [/itex] 


#13
Nov211, 07:54 PM

P: 66

Do you really need me to explain every specific case in which these types of equations do not work? Here are some examples: 1) x has to be within the range of the inverse function f^{1} 2) f(x)x + r(x) must be within the domain of the inverse function f^{1} 3) x must be within the domain of the function f 4) trivial quantities such as zero are trivial (tautologically speaking) 5) f(x) cannot be equal to x (exceptions may exist, none come to mind) When x can not equal r(x), it should be obvious. [tex]x= f^{1}\left(f(x)x+f^{1}(f(x)x+...)\right)[/tex] In this case, y= either side of the equation and x=x: [tex]f(x)=f(x)x+ f^{1}\left(f(x)x+f^{1}(f(x)x+...)\right)[/tex] Now another function, [itex] f^{1}(z)[/itex] is applied to both sides with the result being the original equation. If you can think of examples besides the above list in which x will not equal an infinitely nested function group, we should add them to the list. Of course, there are other things I really want to learn about, such as what is the name of the derivative approximation method using these functions? In addition, specific rules need to be written out for the derivative approximation method, which as far as I can tell requires valid x= infinitely nested functions. 


#14
Nov211, 11:57 PM

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P: 3,252

I'm not trying to function as the mathematical Thought Police. I agree that your methods of manipulating infinite strings of symbols suggest interesting results but it would require more work to prove your assertions and clarify precisely when they apply. The only way that I see, so far, to determine whether a function f(x) "works" in the equation, is test it as a specific case. 


#15
Nov311, 01:30 AM

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P: 3,252

Here's another one that looks like it doesn't work: [itex] f(x) = \frac{x}{2} [/itex] at [itex] x = 2 [/itex]
[itex] g_1(2)= 0 [/itex] [itex] g_2 (2) = 2( \frac{2}{2}  2) = 2 ( 1 2) = 2(1) = 2 [/itex] [itex] g_3(2) = 2( \frac{2}{2}  2 + (2)) = 2( 1 + (2) ) =  6 [/itex] [itex] g_4(2) = 2( \frac{2}{2}  2 + (6) ) = 2( 1 + (6)) =  14 [/itex] 


#16
Nov311, 09:16 PM

P: 66

For example, I've been working with x and n greater than 1 for all equations of the format [itex]\sqrt[n]{x^nx+\sqrt[n]{x^nx+...}}[/itex]. If you set x=2 and n=2, you end up approaching 3 (as 3^23=6 just like (2)^2  2=6). Now I could specify: [itex] x= \sqrt[n]{x^nx+\sqrt[n]{x^nx+...}}[/itex] for all x and n greater than 1, but I don't have a valid proof, as you've shown (induction not being proof). I'm wondering if Ramanajun proved this particular form? Anyways, for this form of the equation: x>1 and n>1 [tex] x^n > x^n  x[/tex] [tex] x > \sqrt[n]{x^nx}[/tex] Because [itex] x > \sqrt[n]{x^nx}[/itex], [itex]g_1(x) = \sqrt[n]{x^nx} [/itex], [itex]g_1(x)< x[/itex] therefore [itex]g_2(x)= \sqrt[n]{x^n x + g_1(x)} < x[/itex]. [tex]g_i(x)=\sqrt[n]{x^nx+g_{i1}(x)}[/tex] You can see that each g_{i} will be larger than the next, although they will never reach x since we require g_{i} to equal x in order for it to reach x (and it's always going to be short). You can also see that g_{i} of x will approach the limit x as [itex]i\to\infty[/itex]. Can you think of a better way to say this? I'm drawing a blank. Therefore.... [tex] x= \sqrt[n]{x^nx+\sqrt[n]{x^nx+...}}[/tex] Interesting: [tex][g_i(x)]^n=x^nx+g_{i1}(x)[/tex] [tex]x=x^n[g_i(x)]^n+g_{i1}(x)[/tex] [tex]x^nx=[g_i(x)]^ng_{i1}(x)[/tex] [tex]x^n[g_i(x)]^n=xg_{i1}(x)[/tex] remembering that we end up with something along the lines of (in some cases, more than one operation is required): [tex]nx^{n1} = \lim_{i\to\infty} \dfrac{xg_{i1}(x)}{xg_{i}(x)}[/tex] 


#17
Nov311, 11:49 PM

P: 66

Here is another quick proof for a range of values (B>1 and x>1).
To be proved: [tex]x=\log_B [B^xx+\log_B [B^xx+...]][/tex] To keep it simple, for this part of the proof assume B>1 and x>1, we can work out how other values work later. [tex]g_0(x)=0[/tex] [tex]g_i(x)= \log_B {\left[B^xx+g_{i1}(x)\right]}[/tex] So for this one, [itex]B^xx[/itex] must be greater than 1. Obviously the log of that will be less than x, and remain so except at the limit [itex]g_{i\to\infty}[/itex]. Once again, a little neat thing popped out at me from the [itex]g_i[/itex] equation (at least I like it): [tex]B^{g_i(x)}= B^xx+g_{i1}(x)[/tex] [tex]xg_{i1}(x)= B^xB^{g_i(x)}[/tex] And once again, applying the inverse function (log base B) to both individual parts of the higher i side of the equation, and dividing out (following the various rules outlined in the other thread keep in mind I haven't clearly defined them as of yet!!) gives us the approximate derivative of B^{x}, B^{x}ln(B) as [itex]g_{i\to\infty}[/itex]. [itex]\dfrac{xg_{i1}(x)}{\log_B [B^x] \log_B [B^{g_i(x)}]}\; = \; \dfrac{xg_{i1}(x)}{ xg_i(x)}[/itex] Anyways, will do a few trig ones after the weekend, won't be able to check in for a few days, so have a good one. 


#18
Nov411, 12:16 AM

Sci Advisor
P: 3,252

I'll have to read that carefully before understanding it.
Today's hazy thoughts on the subject. It simplifies notation to interchange the roles of [itex] f^{1} [/itex] and [itex] f [/itex], which I will do. I'll also write the index of the recursion variable in brackets instead of as a subscript. So I'll define [itex] g[1](x) = 0 [/itex] [itex] g[n](x) = f ( f^{1}(x)  x + g[n1](x)) , n > 1 [/itex] For linear functions of x , [itex] f(x) =cx + d [/itex], the associated sequence [itex] g[i] [/itex] appears to converge to [itex] x [/itex] when [itex] c < 1[/itex] since it is the sequence of partial sums of an infinite geometric series that sums to [itex] x [/itex]. Suppose we are given a nonlinear function [itex] f(x) [/itex] and we can sandwich it between the graphs of two linear functions [itex] A(x) [/itex] and [itex] B(x) [/itex] as long as [itex] x [/itex] is in some interval [itex] I [/itex]. So for [itex] x \in I [/itex], [itex] A(x) \le f(x) \le B(x) [/itex]. Suppose that the associated sequences [itex] g_A[i] [/itex] and[ [itex]g_B[i] [/itex] both converge to the identity function (for any real number x) and that the sequence of [itex] g_f[i] [/itex] associated with [itex] f(x) [/itex] at a given [itex] x = x_0 [/itex] never involves evaluation [itex] f [/itex] at any point outside the interval I. Intuitively, since the recursion process moves the graphs of both linear functions to be the graph of the identity function, it also should move the graph of f to be the identity function. This might be formalized enough to use the squeeze theorem for sequences. If it is true that [itex] g_A[i](x_0) \le g_f[i](x_0) \le g_B[i](x_0) [/itex] and both the extreme terms approach [itex] x_0 [/itex] in the limit, then the middle term should also. I haven't visualized the recursions process carefully enough to know if that inequality must hold when the graph of f is sandwiched. 


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