Equation xy = yx

{{Short description|In general, exponentiation fails to be commutative}}

{{DISPLAYTITLE:Equation xy = yx}}

File:Plot of x^y = y^x.svg, e).]]

In general, exponentiation fails to be commutative. However, the equation x^y = y^x has an infinity of solutions, consisting of the line {{tmath|1=x=y}} and a smooth curve intersecting the line at {{tmath|(e,e)}}, where {{tmath|e}} is Euler's number. The only integer solution that is on the curve is {{tmath|1=2^4=4^2}}.

History

The equation x^y=y^x is mentioned in a letter of Bernoulli to Goldbach (29 June 1728). The letter contains a statement that when x\ne y, the only solutions in natural numbers are (2, 4) and (4, 2), although there are infinitely many solutions in rational numbers, such as (\tfrac{27}{8}, \tfrac{9}{4}) and (\tfrac{9}{4}, \tfrac{27}{8}).

The reply by Goldbach (31 January 1729) contains a general solution of the equation, obtained by substituting y=vx. A similar solution was found by Euler.

J. van Hengel pointed out that if r, n are positive integers with r \geq 3, then r^{r+n} > (r+n)^r; therefore it is enough to consider possibilities x = 1 and x = 2 in order to find solutions in natural numbers.

The problem was discussed in a number of publications. In 1960, the equation was among the questions on the William Lowell Putnam Competition,{{cite web |url=http://www.kalva.demon.co.uk/putnam/putn60.html |title=21st Putnam 1960. Problem B1 |date=20 Oct 1999 |url-status=bot: unknown |archive-url=https://web.archive.org/web/20080330183949/http://www.kalva.demon.co.uk/putnam/putn60.html |archive-date=2008-03-30 }} which prompted Alvin Hausner to extend results to algebraic number fields.{{Cite journal |last=Hausner |first=Alvin |date=November 1961 |title=Algebraic Number Fields and the Diophantine Equation mn = nm |journal=The American Mathematical Monthly |volume=68 |issue=9 |pages=856–861 |doi=10.1080/00029890.1961.11989781 |issn=0002-9890}}

Positive real solutions

:Main source:

=Explicit form=

An infinite set of trivial solutions in positive real numbers is given by x = y. Nontrivial solutions can be written explicitly using the Lambert W function. The idea is to write the equation as ae^b = c and try to match a and b by multiplying and raising both sides by the same value. Then apply the definition of the Lambert W function a'e^{a'} = c' \Rightarrow a' = W(c') to isolate the desired variable.

:\begin{align}

y^x &= x^y = \exp\left(y\ln x\right) & \\

y^x \exp\left(-y\ln x\right) &= 1 & \left(\mbox{multiply by } \exp\left(-y\ln x\right)\right) \\

y\exp\left(-y\frac{\ln x}{x}\right) &= 1 & \left(\mbox{raise by } 1/x\right) \\

-y\frac{\ln x}{x}\exp\left(-y\frac{\ln x}{x}\right) &= \frac{-\ln x}{x} & \left(\mbox{multiply by } \frac{-\ln x}{x}\right)

\end{align}

:\Rightarrow -y\frac{\ln x}{x} = W\left(\frac{-\ln x}{x}\right)

:\Rightarrow y = \frac{-x}{\ln x}\cdot W\left(\frac{-\ln x}{x}\right) = \exp\left(-W\left(\frac{-\ln x}{x}\right)\right)

Where in the last step we used the identity W(x)/x = \exp(-W(x)).

Here we split the solution into the two branches of the Lambert W function and focus on each interval of interest, applying the identities:

:\begin{align}

W_0\left(\frac{-\ln x}{x}\right) &= -\ln x \quad&\text{for } &0 < x \le e, \\

W_{-1}\left(\frac{-\ln x}{x}\right) &= -\ln x \quad&\text{for } &x \ge e.

\end{align}

  • 0 < x \le 1:

:\Rightarrow \frac{-\ln x}{x} \ge 0

:\begin{align}\Rightarrow y &= \exp\left(-W_0\left(\frac{-\ln x}{x}\right)\right) \\

&= \exp\left(-(-\ln x)\right) \\

&= x \end{align}

  • 1 < x < e:

:\Rightarrow \frac{-1}{e} < \frac{-\ln x}{x} < 0

:\Rightarrow y = \begin{cases}

\exp\left(-W_0\left(\frac{-\ln x}{x}\right)\right) = x \\

\exp\left(-W_{-1}\left(\frac{-\ln x}{x}\right)\right)

\end{cases}

  • x = e:

:\Rightarrow \frac{-\ln x}{x} = \frac{-1}{e}

:\Rightarrow y = \begin{cases}

\exp\left(-W_0\left(\frac{-\ln x}{x}\right)\right) = x \\

\exp\left(-W_{-1}\left(\frac{-\ln x}{x}\right)\right) = x

\end{cases}

  • x > e:

:\Rightarrow \frac{-1}{e} < \frac{-\ln x}{x} < 0

:\Rightarrow y = \begin{cases}

\exp\left(-W_0\left(\frac{-\ln x}{x}\right)\right) \\

\exp\left(-W_{-1}\left(\frac{-\ln x}{x}\right)\right) = x

\end{cases}

Hence the non-trivial solutions are:

{{Equation box 1

|indent=:

|equation=y = \begin{cases}

\exp\left(-W_0\left(\frac{-\ln(x)}{x}\right)\right) \quad &\text{for } x > e,\\

\exp\left(-W_{-1}\left(\frac{-\ln x}{x}\right)\right) \quad &\text{for } 1 < x < e.

\end{cases}

}}

=Parametric form=

Nontrivial solutions can be more easily found by assuming x \ne y and letting y = vx.

Then

: (vx)^x = x^{vx} = (x^v)^x.

Raising both sides to the power \tfrac{1}{x} and dividing by x, we get

: v = x^{v-1}.

Then nontrivial solutions in positive real numbers are expressed as the parametric equation

{{Equation box 1

|indent=:

|equation=\begin{align}x &= v^{1/(v-1)}, \\ y &= v^{v/(v-1)}.\end{align}

}}

The full solution thus is (y=x) \cup \left(v^{1/(v-1)},v^{v/(v-1)}\right) \text{ for } v > 0, v \neq 1 .

Based on the above solution, the derivative dy/dx is 1 for the (x,y) pairs on the line y=x, and for the other (x,y) pairs can be found by (dy/dv)/(dx/dv), which straightforward calculus gives as:

:\frac{dy}{dx} = v^2\left(\frac{v-1-\ln v}{v-1-v\ln v}\right)

for v > 0 and v \neq 1.

Setting v=2 or v=\tfrac{1}{2} generates the nontrivial solution in positive integers, 4^2=2^4.

Other pairs consisting of algebraic numbers exist, such as \sqrt 3 and 3\sqrt 3, as well as \sqrt[3]4 and 4\sqrt[3]4.

The parameterization above leads to a geometric property of this curve. It can be shown that x^y = y^x describes the isocline curve where power functions of the form x^v have slope v^2 for some positive real choice of v\neq 1. For example, x^8=y has a slope of 8^2 at (\sqrt[7]{8}, \sqrt[7]{8}^8), which is also a point on the curve x^y=y^x.

The trivial and non-trivial solutions intersect when v = 1. The equations above cannot be evaluated directly at v = 1, but we can take the limit as v\to 1. This is most conveniently done by substituting v = 1 + 1/n and letting n\to\infty, so

: x = \lim_{v\to 1}v^{1/(v-1)} = \lim_{n\to\infty}\left(1+\frac 1n\right)^n = e.

Thus, the line y = x and the curve for x^y-y^x = 0,\,\, y \ne x intersect at {{math|1=x = y = e}}.

As x \to \infty, the nontrivial solution asymptotes to the line y = 1. A more complete asymptotic form is

: y = 1 + \frac{\ln x}{x} + \frac{3}{2} \frac{(\ln x)^2}{x^2} + \cdots.

Other real solutions

An infinite set of discrete real solutions with at least one of x and y negative also exist. These are provided by the above parameterization when the values generated are real. For example, x=\frac{1}{\sqrt[3]{-2}}, y=\frac{-2}{\sqrt[3]{-2}} is a solution (using the real cube root of -2). Similarly an infinite set of discrete solutions is given by the trivial solution y=x for x<0 when x^x is real; for example x=y=-1.

Similar graphs

= Equation {{math|1={{radic|''y''|''x''}} = {{radic|''x''|''y''}}}} =

The equation \sqrt[x]y = \sqrt[y]x produces a graph where the line and curve intersect at 1/e. The curve also terminates at (0, 1) and (1, 0), instead of continuing on to infinity.

The curved section can be written explicitly as

y=e^{W_0(\ln(x^x))} \quad \mathrm{for} \quad 0

y=e^{W_{-1}(\ln(x^x))} \quad \mathrm{for} \quad 1/e

This equation describes the isocline curve where power functions have slope 1, analogous to the geometric property of x^y = y^x described above.

The equation is equivalent to y^y=x^x, as can be seen by raising both sides to the power xy. Equivalently, this can also be shown to demonstrate that the equation \sqrt[y]{y}=\sqrt[x]{x} is equivalent to x^y = y^x.

= Equation {{math|1=log<sub>''x''</sub>(''y'') = log<sub>''y''</sub>(''x'')}} =

The equation \log_x(y) = \log_y(x) produces a graph where the curve and line intersect at (1, 1). The curve becomes asymptotic to 0, as opposed to 1; it is, in fact, the positive section of y = 1/x.

References

{{reflist|refs =

{{citation

|authorlink = Leonard Eugene Dickson|first=Leonard Eugene |last=Dickson

|title = History of the Theory of Numbers

|volume = II

|location = Washington

|year = 1920

|contribution = Rational solutions of xy {{=}} yx

|contribution-url = https://books.google.com/books?id=dO7C02z4LlcC&pg=PA687

|pages = 687

}}

{{cite web|url=http://www.gotham-corp.com/sources.htm#_Toc69534169 |title=Sources in recreational mathematics: an annotated bibliography. 8th preliminary edition |authorlink=David Singmaster|first=David |last=Singmaster |url-status=unfit |archive-url=https://web.archive.org/web/20040416081838/http://www.gotham-corp.com/sources.htm#_Toc69534169 |archive-date=April 16, 2004 }}

{{cite journal

|first = Marta | last = Sved | authorlink = Márta Svéd

|title = On the Rational Solutions of xy {{=}} yx

|year = 1990

|journal = Mathematics Magazine

| volume = 63 | pages = 30–33 | doi = 10.1080/0025570X.1990.11977480 |url = http://www.maa.org/sites/default/files/Sved50816668.pdf

|archive-url = https://web.archive.org/web/20160304191325/http://www.maa.org/sites/default/files/Sved50816668.pdf

|archive-date = 2016-03-04

}}

{{citation

|title = The William Lowell Putnam mathematical competition problems and solutions: 1938-1964

|authorlink = Andrew M. Gleason|first1=A. M. |last1=Gleason|first2= R. E. |last2=Greenwood|authorlink3=Leroy Milton Kelly|first3=L. M.|last3= Kelly

|publisher = MAA

|year = 1980

|isbn = 0-88385-428-7

|contribution = The twenty-first William Lowell Putnam mathematical competition (December 3, 1960), afternoon session, problem 1

|contribution-url = https://books.google.com/books?id=7D0PAQAAMAAJ&q=%22prove+that+you+have+obtained+all+of+them%22

|pages = 59

}}

{{cite journal

|title = Beweis des Satzes, dass unter allen reellen positiven ganzen Zahlen nur das Zahlenpaar 4 und 2 für a und b der Gleichung ab {{=}} ba genügt

|url = http://digital.ub.uni-duesseldorf.de/ulbdsp/periodical/titleinfo/4315444

| journal = Pr. Gymn. Emmerich | jfm = 20.0164.05

|last = van Hengel|first= Johann

|year = 1888

}}

{{cite journal

|url = http://www.komal.hu/cikkek/loczy/powers/commpower.e.shtml

|title = On commutative and associative powers

|first = Lajos |last=Lóczi

|journal = KöMaL

|archive-url = https://web.archive.org/web/20021015103129/http://www.komal.hu/cikkek/loczy/powers/commpower.e.shtml

|archive-date = 2002-10-15

}} Translation of: {{cite web

|url = http://db.komal.hu/KomalHU/cikk.phtml?id=200047

|title = Mikor kommutatív, illetve asszociatív a hatványozás?

|language = hu

|archive-url = https://web.archive.org/web/20160506183127/http://db.komal.hu/KomalHU/cikk.phtml?id=200047

|archive-date = 2016-05-06

}}

}}