@Astyx i think, if i have the free time i wewrite the first proof. i think you are right. The LHS should be viewed seperate from the RHS. Otherwise it's easy to get errors.
if you do the subtraction in one way, you'll get back your original series; but if you do it another way, you'll get a geometric series plus a constant.
what symbolab tells you is that $\sum_{n=0}^\infty \frac{n+2}{2^n} = \sum_{n=0}^\infty \frac{2}{2^n}+\sum_{n=0}^\infty \frac{n}{2^n}=4+\sum_{n=0}^\infty \frac{n}{2^n}$
, I really confused, so i posted it, please try to explain http://math.stackexchange.com/questions/2009669/find-the-value-of-sum-n-0-infty-left-leftn2-right-2n-right
that title is a bit misleading: you ask about $\sum_{n=0}^\infty (n+2)/2^n$ in the title, but in the post itself you make clear that you're only confused about $\sum_{n=0}^\infty n/2^n=2$
and, well, that's a series that i'm sure has shown up on MSE before.
@AndersonFelipeViveiros This is only to do feebback about your question. A thing important in the live of vikings was the navigation in all climatic conditions. Thus you can search what's about it. I don't know references. Search references in internet also in spanish, or other languages.
what does the Poisson bracket do, geometrically? I don't quite get why it should be a vector field (I can prove it).
by Poisson bracket, I mean Poisson bracket of vector fields, defined by $[X, Y](f) = X(Y(f)) - Y(X(f))$, where $X(f)$ and the like means directional derivative of $f$ along $X$.
In mathematics and classical mechanics, the Poisson bracket is an important binary operation in Hamiltonian mechanics, playing a central role in Hamilton's equations of motion, which govern the time evolution of a Hamiltonian dynamical system. The Poisson bracket also distinguishes a certain class of coordinate transformations, called canonical transformations, which map canonical coordinate systems into canonical coordinate systems. A "canonical coordinate system" consists of canonical position and momentum variables (below symbolized by qi and pi, respectively) that satisfy canonical Poisson...
Could some one help explain how the solution set is worked out from the graph of the inequality x^2 + x - 2 < 0. I got (-inf,-2] U [1, inf). But it seems it is actually (-2,1) i don't understand why
given the line goes on forever why does my book state it is actually closed at those numbers not infinite =/
Is there anyone here that could help explain what I am trying to say to a user? It's a pretty complicated concept and I think they're having a hard time understanding my question.
It seems you have many difficulties explaining what you want. You never talked of "a final operator" — user195200921 mins ago
I wish to rigorously define alternate different integrals where an arbitrary set of functions is what all potential integrals of some kind vary by (by "vary by" I mean that the difference of any two integrals is an element of this function set), and where the alternate integral treats functions o...
In the formula for sum of infinite arithmetico geometric series, $S_n = \frac{a}{(1-r)} + \frac{rd}{(1-r^2)}$ what is $a$? Is the initial value of the series of the initial value of the AP part of the series?
At the end of that page there's a formula for the infinite AGP series. I wanted to know what the variable $a$ represents in that formula. Is it the initial value of the AP part or the initial value of the AGP series. Thanks.
@TheGreatDuck: I'm not going to look on my phone, but offhand you need your function set to consist of solutions of some particular differential equation.
the lack of rigorous notation, terminology and other things makes it difficult to express. I'm trying my hardest but it seems like it won't get answered anytime soon (the only person commenting seems to have trouble understanding), which is quite sad as having a way to express this for other people to understand would be quite beneficial to me.
"I'm not going to" huh? I asked if you had any ideas on how to improve it?
"but offhand you need your function set to consist of solutions of some particular differential equation." how so?
are differential equations a way of altering the integral?