agentredlum
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Char. Limit said:Also, 1+1+1=111 in base 1.
YOU'RE RIGHT TOO!
Thanks to all posting
I'm not sure the digit 0 would be allowed in base 0.
Char. Limit said:Also, 1+1+1=111 in base 1.
Char. Limit said:Basically, Base 1 only allows one digit: 1. Base 2 allows 1 and 0. That's why 1+1+1=111 in base 1... actually, 1+1+1...+1 = 111...1 in base 1.


Char. Limit said:No digits would be allowed in base 0. After all, the base number shows how many different "numbers" you can allow. Base 1 has one number: 1. Base 2 has two numbers: 0 and 1. The amount of numbers in base 0 is... the empty set!
agentredlum said:Oh, so I can't use 0 in base 1
Too bad the symmetry is broken.![]()
Samuelb88 said:I always admired the fact that \int_{-1}^1 \frac{\mathrm{d}x}{x} = i\pi. By a symmetry argument, intuition would suggest the integral is zero since there is infinite negative area from -1 to 0 and infinite positive area from 0 to 1.
chiro said:You can use whatever symbol you want, but you can only use that symbol.
Guffel said:I love the fact that the number of partitions into odd parts is the same as the number of partitions in distinct parts. Far from intuitive and finding a bijective proof is difficult (easy to prove using generating functions though). Not really a trick, but the discussion also seems to include curiousities. Sorry if OT.
That's it. And I agree, partitions are fascinating!agentredlum said:Is this what you are posting about?
http://demonstrations.wolfram.com/TheNumberOfPartitionsIntoOddPartsEqualsTheNumberOfPartitions/
Heres an explanation of partitions. Personally I find partitions fascinating
http://en.wikipedia.org/wiki/Partition_(number_theory )
Dodo said:An old trick about differentiation from Feynman's book "Tips on Physics":
If f(x) is a function whose rule has the form f = k . u^a . v^b . w^c . ...
where u,v,w,... are also functions of x (you can think of u,v,w,... as "sub-expressions" in the rule for f),
and k,a,b,c,... are constants, then
f' = f . (a u'/u + b v'/v + c w'/w + ...)
It can be proven by induction on the number of factors.
Note that the sum within parenthesis has as many terms as "sub-expression" factors in the original, and a sum of zero terms should be regarded as 0.
Dodo said:(Sorry, elegysix, I was replying to the post before yours. :)
Well, maybe your example (4x^5)*(3x^2) = 12 x^7 is a bit too simple to use this.
But try to differentiate instead something like
f(x) = (3x+1)*sqrt(x^2-2)*(x+3)^3
which would be very lenghty if you have to apply the product rule repeatedly, instead you can write in a moment,
f'(x) = (3x+1)*sqrt(x^2-2)*(x+3)^3 . ( 3/(3x+1) + (1/2)*2x/(x^2-2) + 3*(1/(x+3)) )
and then simplify to your taste. Although for me it's more the elegance of the formula.
elegysix said:sorry for the late reply, here's an image of my post on fractional calculus you asked for.
[PLAIN]http://img835.imageshack.us/img835/5461/fraccalculus.png[/QUOTE]
Thank you so much for the picture. I really appreciate it. PLEASE POST MORE!![]()
TejasB said:Dude x being the root of a quadratic expression two values are expected in your case you took only + when it is +\-. As an expample consider x^2+x-6=0. By your formula roots become complex when they are 2&-3.
Suppose we consider the integral\int\frac{1}{x-i}{dx}TylerH said:\int_0^x darctanx=\int_0^x \frac{dx}{x^2+1}=\int_0^x \frac{i}{2(x-i)} - \frac{i}{2(x+i)} dx = \frac{i}{2} ln \left( \frac{x-i}{x+i} \right) \Rightarrow \forall x \in \Re, \: arctanx = \frac{i}{2}ln \left( \frac{x-i}{x+i} \right)
Anamitra said:{z=}\frac{1}{2i}{ln}\frac{x-i}{x+i}
or,
{z=}\frac{1}{2i}{ln}\frac{{-}{(}{1}{-}{x}^{2}{)}{-}{2xi}}{{x}^{2}{+}{1}}
We substitute,
x=tan[theta]
Now we have,
{z}{=}{-}{\frac{1}{2i}}{ln}{[}{cos}{2}{\theta}{+}{i}{sin}{(}{2}{\theta}[)]{]}
{e}^{-2iz}{=}{cos}{2}{\theta}{+}{i}{sin}{2}{\theta}
{cos}{-2z}{+}{i}{sin}{-2z}{=}{[}{cos}{(}{2}{\theta}{)}{+}{i}{sin}{(}{2}{\theta}{)}
Therefore,
{-2z}{=}{2}{\theta}
z=-theta=-arctanx
The minus sign is causing trouble
Anamitra said:{z=}\frac{1}{2i}{ln}\frac{x-i}{x+i}
or,
{z=}\frac{1}{2i}{ln}\frac{{-}{(}{1}{-}{x}^{2}{)}{-}{2xi}}{{x}^{2}{+}{1}}
We substitute,
x=tan[theta]
Now we have,
{z}{=}{-}{\frac{1}{2i}}{ln}{[}{cos}{2}{\theta}{+}{i}{sin}{(}{2}{\theta}{)}{]}
{e}^{-2iz}{=}{cos}{2}{\theta}{+}{i}{sin}{2}{\theta}
{cos}{(}{-2z}{)}{+}{i}{sin}{(}{-2z}{)}{=}{[}{cos}{(}{2}{\theta}{)}{+}{i}{sin}{(}{2}{\theta}{)}{]}
Therefore,
{-2z}{=}{2}{\theta}
z=-theta=-arctanx
The minus sign is causing trouble
Anamitra said:We start with:
Integral=
{z}{=}\frac{1}{2i}{ln}{\mid}\frac{{-}{(}{1}{-}{x}^{2}{)}{-}{2xi}}{{x}^{2}{+}{1}}{\mid}
{=}\frac{1}{2i}{ln}{\mid}{-}\frac {{1}{-}{x}^{2}}{{1}{+}{x}^{2}}{-}\frac{2xi}{{1}{+}{x}^{2}}{\mid}
{=}\frac{1}{2i}{ln}{[}\frac {{1}{-}{x}^{2}}{{1}{+}{x}^{2}}{+}\frac{2xi}{{1}{+}{x}^{2}}{]}
Now,
\frac{{1}{-}{tan}^{2}{\theta}}{{1}{+}{tan}^{2}{\theta}}{=}{cos}{2}{\theta}
And,
\frac{{2}{tan}{\theta}}{{1}{+}{tan}^{2}{\theta}}{=}{sin}{2}{\theta}
Substituting x=tan[theta] we may proceed.