Hey guys, I'm trying to work through and understand this: aoengr.com/Dynamics/LagrangianMechanicsPendulum.pdf . The part that's tripping me up is the first half of the third page, where apparently $\frac{\partial{L}}{\partial{\theta}} \left( \frac{1}{2} m l^2 \dot{\theta}^2 \right) = 0$ and $\frac{\partial{L}}{\partial{\dot{\theta}}} \left( m \cdot g \cdot l \cdot (1 - \cos{\theta}) \right) = 0$. I don't understand why you can do that.
$\int_{0}^{ln(2)} \frac{1}{(1+e^{-x}}$ using the substituion $y = e^{-x}$, apparently transforms to $\int{0.5}{1} \frac{1}{y(1+y)}$, but I end up with $\int{0.5}{1} \frac{-1}{y(1+y)}$
huh. i seem to have forgotten formatting too lmao.
Why is the font so unreadable when its being edited
Faust is the protagonist of a classic German legend, based on the historical Johann Georg Faust (c. 1480–1540).
Faust is a scholar who is highly successful yet dissatisfied with his life, which leads him to make a pact with the Devil, exchanging his soul for unlimited knowledge and worldly pleasures. The Faust legend has been the basis for many literary, artistic, cinematic, and musical works that have reinterpreted it through the ages. "Faust" and the adjective "Faustian" imply a situation in which an ambitious person surrenders moral integrity in order to achieve power and success for a delimited...
@El'endiaStarman Maybe a simpler question will fetch an answer: what is $$\frac{\partial{}}{\partial{\theta}} \dot{\theta}$$ and why? Where $\dot{\theta} = \frac{d\theta}{dt}$.
In combinatorics, the binomial transform is a sequence transformation (i.e., a transform of a sequence) that computes its forward differences. It is closely related to the Euler transform, which is the result of applying the binomial transform to the sequence associated with its ordinary generating function.
== Definition ==
The binomial transform, T, of a sequence, {an}, is the sequence {sn} defined by
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In mathematical analysis, Cesàro summation assigns values to some sequences without a sum in the usual sense. The Cesàro sum of a sequence is defined as the limit of the arithmetic means of the partial sums of that sequence.
Cesàro summation is named for the Italian analyst Ernesto Cesàro (1859–1906).
The term summation can be misleading, as some statements and proofs regarding Cesàro summation can be said to implicate the Eilenberg–Mazur swindle. For example, it is commonly applied to Grandi's series with the conclusion that its sum is 1/2.
== Definitions ==
A sequence {ai} is called Ces...
Are you doing Lagrangian mechanics or something like that? It's normal to treat $\theta$ and $\dot\theta$ as different variables in that case @El'endiaStarman
Hello, i was comparing the definition of functional limits and continuity (real analysis), I noticed the definition of functional limits includes Limit Points and does not require the real variable $x$ to be in Domain of $f$.
Whereelse the definition of continuity does not include Limit Points and require $x$ to be in Domain of $f$.
The idea is that to do Lagrangian mechanics you work on the tangent bundle of the configuration space (and sometimes on the tangent bundle of that), this doubles the dimension of the manifold so instead of just having free coordinates for the position you also have them for the velocities and you effectively treat them as separate coordinates, you write $L(r_1,\cdots,r_n,\dot{r_1},\cdots,\dot{r_n})$ for the Lagrangian etc.
But I forgot the details, let's hope Semi arrives soon :P
@AlessandroCodenotti Wait, that might have actually cleared it up for me. Lemme see if I understand. When doing Lagrangian mechanics, to make the math easier, you treat the position and velocity of each particle as independent? So then, what ties them together is the.....Lagrangian itself?
I've seen this things in a mathematical physics course that was very heavy on the maths, I'm not sure about the physical interpretation of why this is correct
Given be the area of a 2-dimensional elephant is $A$. Shrinking the elephant now by its width, will also half its area. (at least if one considers the elephant area to be lebesque or riemann integrable) However how does this change for 2-dimensional animals, one may consider "weird shaped"? Is there a quick example to see, when linearity is not preserved, but measuring area still makes sense?
If you shrink just one dimension, I think it will be halved.
For example if you look at the function $f(x) = \cos(x) +1$ from $0$ to $2pi$, the area does not change if you instead look at $g(x) = \cos(2x) + 1 $ from $0$ to $2 \pi$