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Or Entity?
Nov19-08, 06:30 PM
Lets elect World's most beautiful equation!

Two categories:

1.Mathematics
2.Physics

My personal favourites would be:

1. e^{i\pi}+1=0 (Do i need to give an argument?)

2. E=mc^{2} (I know its mainstream.. but i doesent get much more simple and general than this!)

Ed Aboud
Nov19-08, 06:40 PM
i\hbar\frac{\partial\Psi}{\partial t} = \frac{\hbar^2}{2m}\frac{\partial^2\Psi}{\partial x^2} + V\Psi

vanesch
Nov20-08, 03:03 AM
I'd say: 1 = 0. From this one, you can derive everything :biggrin:

saman
Nov20-08, 05:52 PM
Maxwell's equations of EM?

\nabla \cdot D= \rho
\nabla \cdot B=0
\nabla \times E=- \partial B/ \partial t
\nabla \times H=J+ \partial D/ \partial t

andrewm
Nov20-08, 05:56 PM
p = \frac{h}{\lambda}

robphy
Nov21-08, 04:05 AM
i\hbar\frac{\partial\Psi}{\partial t} = \frac{\hbar^2}{2m}\frac{\partial^2\Psi}{\partial x^2} + V\Psi


I think you are missing a minus sign.

joeyar
Nov21-08, 04:25 AM
1/. cos²(x) + sin²(x) = 1
2/. ω² = k/m

Borek
Nov21-08, 04:26 AM
2. E=mc^{2} (I know its mainstream.. but i doesent get much more simple and general than this!)

Isn't it only an approximation? :wink:

redargon
Nov21-08, 04:36 AM
FD=½ρv2ACD

Some engineering fudgeamatics

Binhjuventus™
Nov21-08, 04:40 AM
For me, it's:
i2=-1

joeyar
Nov21-08, 04:58 AM
Isn't it only an approximation? :wink:

It's true http://nz.news.yahoo.com/a/-/world/5160859/einsteins-emc2-proven-103-years/

Borek
Nov21-08, 05:34 AM
As far as I remember mc2 is only a first term of the power series. Next terms are smaller by at least c2 factor (or even c4, my memory fails me here), so they can be safely ignored, but E=mc2 is still only an approximation.

carapauzinho
Nov21-08, 05:50 AM
As far as I remember mc2 is only a first term of the power series. Next terms are smaller by at least c2 factor (or even c4, my memory fails me here), so they can be safely ignored, but E=mc2 is still only an approximation.


I think you refer this equation:

E2=m2c4+p2c2

Borek
Nov21-08, 06:01 AM
No, I refer to the way equation is derived.

http://www.fourmilab.ch/etexts/einstein/E_mc2/e_mc2.pdf

Neglecting magnitudes of fourth and higher orders we may place

robphy
Nov21-08, 06:41 AM
As far as I remember mc2 is only a first term of the power series. Next terms are smaller by at least c2 factor (or even c4, my memory fails me here), so they can be safely ignored, but E=mc2 is still only an approximation.

You may referring to the Taylor expansion (with respect to the velocity) for the relativistic energy:
http://en.wikipedia.org/wiki/Kinetic_energy
expressed as
E_{rel}=m_{rel}c^2=m_0c^2 \frac{1}{\sqrt{1-(v/c)^2}}=m_0c^2\bigg(1+\frac{1}{2}(v/c)^2+\frac{3}{8}(v/c)^4+\ldots\bigg) \approx m_0c^2 \bigg( 1+\frac{1}{2}(v/c)^2 \bigg)\mbox{[for small (v/c)]}

The rest energy E_0=m_0c^2 is a Lorentz invariant, and E_{rel} and m_{rel} are observer-dependent quantities.

From a special-relativistic viewpoint, these are exact relations.

From a Newtonian-physics viewpoint, one often refers to some of these terms as "relativistic corrections".

Naty1
Nov21-08, 07:53 AM
E= ir !

Ed Aboud
Nov22-08, 11:25 AM
My bad

i\hbar\frac{\partial\Psi}{\partial t} = - \frac{\hbar^2}{2m}\frac{\partial^2\Psi}{\partial x^2} + V\Psi

Friesiangirl
Nov22-08, 05:07 PM
Well, it may be hard to say. I am a junior in high school, so my physics knowledge is limited, however, I am fond of

i^2 = -1

Imaginary x Imaginary = Real. Seems silly but awesome.

Hayley

M Grandin
Nov22-08, 06:53 PM
Maxwell`s velocity distribution formula

f(v) = 4 \pi [ m / 2 \pi k T ]^(3/2) v^2 e^(-m v^2 / 2 k T )

The elegance because he derived this formula just by logical reasoning
almost without calculus or any kind of information. Intellectual wizardy.

Loren Booda
Nov22-08, 08:42 PM
zeta(s)=1+(2^-s)+(3^-s)+(4^-s)+...

- the zeta function from which the Riemann hypothesis derives.

optics123
Nov2-10, 10:13 AM
E=mc^2 .

Max™
Nov2-10, 01:33 PM
http://www.math.ucsb.edu/~stopple/contours.jpg
http://primes.utm.edu/gifs/zetafun1.gif

jobyts
Nov2-10, 02:05 PM
0! = 1

I don't know if it is beautiful; but it is pretty weird.

jackmell
Nov2-10, 04:09 PM
The equation relating primes to zeta zeros:

\psi(x)=-\frac{1}{2\pi i}\mathop\int\limits_{c-i\infty}^{c+i\infty} \frac{\zeta'(s)}{\zeta(s)}\frac{x^s}{x}ds

Max™
Nov2-10, 06:13 PM
The equation relating primes to zeta zeros:

\psi(x)=-\frac{1}{2\pi i}\mathop\int\limits_{c-i\infty}^{c+i\infty} \frac{\zeta'(s)}{\zeta(s)}\frac{x^s}{x}ds

Agreed as well.

I favorited this just because it's one of my favorite studies of zeta so far.

http://arxiv.org/PS_cache/math/pdf/0309/0309433v1.pdf

X-RAY OF RIEMANN’S ZETA-FUNCTION
J. ARIAS-DE-REYNA
1. Introduction
This paper is the result of the effort to give the students of the subject
Analytic Number Theory an idea of the complexity of the behaviour of the
Riemann zeta-function. I tried to make them see with their own eyes the
mystery contained in its apparently simple definition.
There are precedents for the figures we are about to present. In the
tables of Jahnke-Emde [9] we can find pictures of the zeta-function and
some other graphs where we can see some of the lines we draw. In the
dissertation of A. Utzinger [21], directed by Speiser, the lines Re (s) = 0
and Im(s) = 0 are drawn on the rectangle (−9, 10) × (0, 29).
Besides, Speiser’s paper contains some very interesting ideas. He proves
that the Riemann Hypothesis is equivalent to the fact that the non trivial
zeros of ′(s) are on the right of the critical line. He proves this claim
using an entirely geometric reasoning that is on the borderline between the
proved and the admissible. Afterwards rigorous proofs of this statement
have been given.

The legend
Nov2-10, 09:54 PM
Both of your choices, Entity, are my favourites!!!! I just love those equations and the first one, i understood only a few days ago!

So for me, they are the best equations! :smile:

DaveC426913
Nov2-10, 11:06 PM
Does the Mandelbrot Set count as an equation? It's really more of an algorithm I suppose.

DR13
Nov2-10, 11:07 PM
2+2=5

Max™
Nov3-10, 12:26 AM
2+2=5

How Orwellian of you.

The legend
Nov3-10, 01:47 AM
2+2=5

:rofl:

Chi Meson
Nov3-10, 05:36 AM
2+2=5

That is only true for large values of 2.

Upisoft
Nov3-10, 05:43 AM
pi=3.0

n.karthick
Nov3-10, 06:05 AM
For me the Fourier transform equation is the most beautiful


F(\omega)=\int_{-\infty}^{\infty} f(t) e^{i \omega t} dt

Max™
Nov3-10, 03:46 PM
That is only true for large values of 2.

As long as the error bars are sufficiently broad it could work as well.

hotvette
Nov3-10, 03:54 PM
I like:

x2+y2=1
y = xx

lisab
Nov3-10, 04:12 PM
pi=3.0

:tongue2:

Pinčiukas
Nov3-10, 04:23 PM
178212+184112=192212
:approve:

Dembadon
Nov3-10, 04:23 PM
pi=3.0

Upisoft hits R for 9000 damage (.14159 Overkill)
R dies

G037H3
Nov3-10, 09:15 PM
Upisoft hits R for 9000 damage (.14159 Overkill)
R dies

not over 9K, notice

Upisoft
Nov4-10, 09:56 AM
Upisoft hits R for 9000 damage (.14159 Overkill)
R dies

They will fix it in the next version...:rofl:

xeniosm
Feb19-11, 06:33 AM
the very simple (and suppressed!) standard model lagrangian

chaoseverlasting
Feb19-11, 06:52 AM
f(x)=\frac{a_0}{2} + \sum_{n=1}^\infty \, [a_n \cos(nx) + b_n \sin(nx)]

I'm surprised no one has put this one up yet!

elfboy
Feb19-11, 07:07 PM
http://upload.wikimedia.org/math/f/c/c/fccd2367982ea085e0d801aa2cfbc5e1.png

my identity

a single equation? i dunno too many to think of

micromass
Feb19-11, 09:54 PM
The most beautiful "equation" is

\langle a,b~\vert~o(a)=2, o(b)=3, o(ab)=29, o((ab)^4(abb)^2)=50, o(a((ab)^4(abb)^2)^{25})=5, o(ab^{abababababb})=34\rangle

Extra points for anybody who says what I've written down here :biggrin:

Containment
Feb19-11, 10:30 PM
Ohm's law gets my vote.

Pengwuino
Feb19-11, 10:44 PM
G_{\mu \nu} = 8T_{\mu \nu}

Where I have set c = G = \pi = 1

FtlIsAwesome
Feb20-11, 09:48 PM
I'd say: 1 = 0. From this one, you can derive everything :biggrin:
:rofl:


What about i>u ?
:tongue2: :tongue2: :tongue2:

Pattonias
Feb20-11, 09:58 PM
I find derivatives beautiful even though I also hate them.

Pythagorean
Feb22-11, 09:31 AM
Math:

Euler's Equation
e^{\pm i \theta} = \cos(\theta) + i \sin(\theta)

because it demonstrates the meaning of i as a transform/operator, rather than sqrt(-1)

Physics:

Continuity Equation (for conserved \phi):
\frac{\delta \phi}{\delta t} + \nabla \cdot f = 0

because it relates the physical meaning of the partial derivative to that of the total derivative.

Biology:

\Delta G = -n F \Delta E

Energy for work is the number of moles of stored energy from electric charge.