Supporter
- Joined
- Apr 26, 2020
- Messages
- 4,546
JUST KEPT HAMMERING THAT REFRESH BUTTON.... 
I always forget MangaDex did come back just as a reading site at first, I did the same, though it didn't feel the same without the comments.I remember they posted a timetable about phases such as "in two months MangaDex will be back just to read the stuff it had before the 'Hombre!' incident" and once it was up I read some chapters everyday from the pending manga list I had. From that, I could see how they implemented everything and all the announcements they did as time passed.
I know this comment isn't aimed at me, but I remember that MD twitter had some kind of April Fools plan and pranked their users into thinking MD is backFor people returning back to MangaDex from V3, how did you rediscover MangaDex after the 2021 shutdown?
"The only thing that doesn't change is change itself"started talking with a friend i haven't talked to in 2 years and that i have (cumulatively) been friends with for 8 years.
she is now a transgender male.
and she is completely different.
why can't things just stay the way they are
\[ \begin{aligned} &\textbf{Full Field-definition :} \\[1ex] \mathcal{M}(x^\mu) &= A \cdot \exp\left( -\frac{(x^\mu - X^\mu(\tau))(x_\mu - X_\mu(\tau))}{R^2} \right) \cdot \cos\left( k_\mu (x^\mu - X^\mu(\tau)) \right) \\[2ex] X^\mu(\tau) &= x_0^\mu + u^\mu \tau, \quad u^\mu u_\mu = c^2 \\[2ex] k^\mu &= \left( \frac{\omega}{c}, -\vec{k} \right) \\[2ex] &\textbf{Field equation :} \\[1ex] \Box \mathcal{M} + \frac{dV}{d\mathcal{M}} = S(x), \qquad \Box = \partial^\mu \partial_\mu \\[2ex] V(\mathcal{M}) &= \frac{1}{2} m^2 \mathcal{M}^2 + \frac{\lambda}{4} \mathcal{M}^4 \\[2ex] &\textbf{Lagrangian \& energy :} \\[1ex] \mathcal{L}[I]{\mathcal{M}} = \frac{1}{2} \partial^\mu \mathcal{M} \, \partial[/I]\mu \mathcal{M} - V(\mathcal{M}) + \mathcal{M} \cdot S(x) \\[2ex] \mathcal{E}(x) = \frac{1}{2} (\partial_t \mathcal{M})^2 + \frac{1}{2} (\nabla \mathcal{M})^2 + V(\mathcal{M}) \\[2ex] &\textbf{Source term :} \\[1ex] S(x) = \epsilon \cdot \left[\mathcal{F}(x) - \mathcal{F}[I]{\text{local avg}}(x)\right] \cdot \tanh\left( \frac{\mathcal{C}(x) - \Lambda}{\sigma} \right) \\[2ex] &\textbf{Source-activation function :} \\[1ex] \mathcal{F}(x) = \left|\frac{\vec{E} \cdot \vec{B}}{B_0^2}\right| + \alpha \left|\frac{\partial_t \rho}{\rho_0 \omega_0}\right| + \beta \left|\frac{\nabla \cdot \vec{E}}{E_0 / \ell_0}\right| \\[2ex] \mathcal{F}[/I]{\text{local avg}}(x) = \frac{1}{V_{\delta}} \int_{|x - x'| < \delta} \mathcal{F}(x') \, d^3x' \\[2ex] \mathcal{C}(x) = \mathcal{I}(x) + \gamma \mathcal{T}(x) + \delta \mathcal{K}(x) \\[1ex] \mathcal{I}(x) = T^{00}(x), \quad \mathcal{T}(x) = \epsilon^{ijk} A_i \partial_j A_k, \quad \mathcal{K}(x) = \text{Tr}\left( R^\mu_{\ \nu\rho\sigma} R_\mu^{\ \nu\rho\sigma} \right) \\[2ex] &\textbf{Cꜷsality constraint :} \\[1ex] \left| \frac{\partial \mathcal{M}}{\partial t} \right| \leq c \left| \nabla \mathcal{M} \right| \\[2ex] &\textbf{E.-m. Energy coupling :} \\[1ex] \frac{\partial}{\partial t} \left( \frac{|\vec{E}|^2 + |\vec{B}|^2}{8\pi} \right) = -\mathcal{M}(x) \cdot S_{\text{E.-m.}}(x) \\[2ex] S_{\text{E.-m.}}(x) = \chi \cdot \left[ \frac{\vec{E} \cdot \vec{B}}{B_0^2} + \eta \cdot \frac{\nabla \cdot \vec{E}}{E_0 / \ell_0} + \xi \cdot \frac{\partial_t \rho}{\rho_0 \omega_0} \right] \\[2ex] &\textbf{Constants :} \\[1ex] \alpha, \beta, \gamma, \delta, \epsilon, \eta, \xi, \chi \in \mathbb{R}^+ \quad B_0, E_0, \ell_0, \rho_0, \omega_0 \in \mathbb{R}^+ \quad \Lambda, \sigma, \delta \in \mathbb{R}^+ \end{aligned} \]
I’ve scrabbled an Improv Magic‑system and upon trying It… Well , let Us acknowledge the fact that We — magicians in This universe — won’t need Grease cleaners Any‑more since Any‑thing that’s — practically — More Energy‑extensive than changing Local properties of ʃome fat , We are out of luck , as in ; No explosions that can move mountains.
Haah…
Other than that : We need to kiſs the rails , forget about Other types of magic , & find solace in Floating objects & ʃelf‑cleaning Kitchen‑ware.
.
It mꜽ be the case that limiting It : by speed of light ( \(\left| \frac{\partial \mathcal{M}}{\partial t} \right| \leq c \left| \nabla \mathcal{M} \right|\) ) & to the Local E.-m. field ( \(\frac{\partial}{\partial t} \left( \frac{|\vec{E}|^2 + |\vec{B}|^2}{8\pi} \right) = -\mathcal{M}(x) \cdot S_{\text{E.-m.}}(x)\) ) was a Big mistake… I wonder if I can By‑paß the \(c\) by , well , sꜽing : « ‘tis Actually not transmiſsion of information , but rather ; It’s absence of information reaching information about absence of information. » , or ʃome other Bull‑shit.
Eh.
If , mꜽbe if , I Re‑fine It more , then — mꜽ be ; I will be able to fix some Obvious ißuͤs in the equations but ʃo far I can Only sꜽ that knowing I can only L.-a.R.-p. as a ghost breaks My spirit.
Why dealing with magic has to be ʃo hard ?
…
Does Any‑one know a Nice manga with more than , let’s sꜽ , 50 chapters that has :
1. a girl who doesn’t care about what ʃhe does to others ,
& 2. magic that is — ontologically — more than « I practiced , I became better ! » system.
The math of Mine for those who are interested :
![]()
![]()
\[ \begin{aligned} &\textbf{Full Field-definition :} \\[1ex] \mathcal{M}(x^\mu) &= A \cdot \exp\left( -\frac{(x^\mu - X^\mu(\tau))(x_\mu - X_\mu(\tau))}{R^2} \right) \cdot \cos\left( k_\mu (x^\mu - X^\mu(\tau)) \right) \\[2ex] X^\mu(\tau) &= x_0^\mu + u^\mu \tau, \quad u^\mu u_\mu = c^2 \\[2ex] k^\mu &= \left( \frac{\omega}{c}, -\vec{k} \right) \\[2ex] &\textbf{Field equation :} \\[1ex] \Box \mathcal{M} + \frac{dV}{d\mathcal{M}} = S(x), \qquad \Box = \partial^\mu \partial_\mu \\[2ex] V(\mathcal{M}) &= \frac{1}{2} m^2 \mathcal{M}^2 + \frac{\lambda}{4} \mathcal{M}^4 \\[2ex] &\textbf{Lagrangian \& energy :} \\[1ex] \mathcal{L}[I]{\mathcal{M}} = \frac{1}{2} \partial^\mu \mathcal{M} \, \partial[/I]\mu \mathcal{M} - V(\mathcal{M}) + \mathcal{M} \cdot S(x) \\[2ex] \mathcal{E}(x) = \frac{1}{2} (\partial_t \mathcal{M})^2 + \frac{1}{2} (\nabla \mathcal{M})^2 + V(\mathcal{M}) \\[2ex] &\textbf{Source term :} \\[1ex] S(x) = \epsilon \cdot \left[\mathcal{F}(x) - \mathcal{F}[I]{\text{local avg}}(x)\right] \cdot \tanh\left( \frac{\mathcal{C}(x) - \Lambda}{\sigma} \right) \\[2ex] &\textbf{Source-activation function :} \\[1ex] \mathcal{F}(x) = \left|\frac{\vec{E} \cdot \vec{B}}{B_0^2}\right| + \alpha \left|\frac{\partial_t \rho}{\rho_0 \omega_0}\right| + \beta \left|\frac{\nabla \cdot \vec{E}}{E_0 / \ell_0}\right| \\[2ex] \mathcal{F}[/I]{\text{local avg}}(x) = \frac{1}{V_{\delta}} \int_{|x - x'| < \delta} \mathcal{F}(x') \, d^3x' \\[2ex] \mathcal{C}(x) = \mathcal{I}(x) + \gamma \mathcal{T}(x) + \delta \mathcal{K}(x) \\[1ex] \mathcal{I}(x) = T^{00}(x), \quad \mathcal{T}(x) = \epsilon^{ijk} A_i \partial_j A_k, \quad \mathcal{K}(x) = \text{Tr}\left( R^\mu_{\ \nu\rho\sigma} R_\mu^{\ \nu\rho\sigma} \right) \\[2ex] &\textbf{Cꜷsality constraint :} \\[1ex] \left| \frac{\partial \mathcal{M}}{\partial t} \right| \leq c \left| \nabla \mathcal{M} \right| \\[2ex] &\textbf{E.-m. Energy coupling :} \\[1ex] \frac{\partial}{\partial t} \left( \frac{|\vec{E}|^2 + |\vec{B}|^2}{8\pi} \right) = -\mathcal{M}(x) \cdot S_{\text{E.-m.}}(x) \\[2ex] S_{\text{E.-m.}}(x) = \chi \cdot \left[ \frac{\vec{E} \cdot \vec{B}}{B_0^2} + \eta \cdot \frac{\nabla \cdot \vec{E}}{E_0 / \ell_0} + \xi \cdot \frac{\partial_t \rho}{\rho_0 \omega_0} \right] \\[2ex] &\textbf{Constants :} \\[1ex] \alpha, \beta, \gamma, \delta, \epsilon, \eta, \xi, \chi \in \mathbb{R}^+ \quad B_0, E_0, \ell_0, \rho_0, \omega_0 \in \mathbb{R}^+ \quad \Lambda, \sigma, \delta \in \mathbb{R}^+ \end{aligned} \]
What are you, AO3 author?Doing well so far. Not long ago I fell off my bike because there was a car oncoming. And then I caught a fever. It's all good though, just minor injuries and now I'm completely healed. Thank you for asking![]()
Dayem. What you rambling about dude?I’ve scrabbled an Improv Magic‑system and upon trying It… Well , let Us acknowledge the fact that We — magicians in This universe — won’t need Grease cleaners Any‑more since Any‑thing that’s — practically — More Energy‑extensive than changing Local properties of ʃome fat , We are out of luck , as in ; No explosions that can move mountains.
Haah…
Other than that : We need to kiſs the rails , forget about Other types of magic , & find solace in Floating objects & ʃelf‑cleaning Kitchen‑ware.
.
It mꜽ be the case that limiting It : by speed of light ( \(\left| \frac{\partial \mathcal{M}}{\partial t} \right| \leq c \left| \nabla \mathcal{M} \right|\) ) & to the Local E.-m. field ( \(\frac{\partial}{\partial t} \left( \frac{|\vec{E}|^2 + |\vec{B}|^2}{8\pi} \right) = -\mathcal{M}(x) \cdot S_{\text{E.-m.}}(x)\) ) was a Big mistake… I wonder if I can By‑paß the \(c\) by , well , sꜽing : « ‘tis Actually not transmiſsion of information , but rather ; It’s absence of information reaching information about absence of information. » , or ʃome other Bull‑shit.
Eh.
If , mꜽbe if , I Re‑fine It more , then — mꜽ be ; I will be able to fix some Obvious ißuͤs in the equations but ʃo far I can Only sꜽ that knowing I can only L.-a.R.-p. as a ghost breaks My spirit.
Why dealing with magic has to be ʃo hard ?
…
Does Any‑one know a Nice manga with more than , let’s sꜽ , 50 chapters that has :
1. a girl who doesn’t care about what ʃhe does to others ,
& 2. magic that is — ontologically — more than « I practiced , I became better ! » system.
The math of Mine for those who are interested :
![]()
![]()
\[ \begin{aligned} &\textbf{Full Field-definition :} \\[1ex] \mathcal{M}(x^\mu) &= A \cdot \exp\left( -\frac{(x^\mu - X^\mu(\tau))(x_\mu - X_\mu(\tau))}{R^2} \right) \cdot \cos\left( k_\mu (x^\mu - X^\mu(\tau)) \right) \\[2ex] X^\mu(\tau) &= x_0^\mu + u^\mu \tau, \quad u^\mu u_\mu = c^2 \\[2ex] k^\mu &= \left( \frac{\omega}{c}, -\vec{k} \right) \\[2ex] &\textbf{Field equation :} \\[1ex] \Box \mathcal{M} + \frac{dV}{d\mathcal{M}} = S(x), \qquad \Box = \partial^\mu \partial_\mu \\[2ex] V(\mathcal{M}) &= \frac{1}{2} m^2 \mathcal{M}^2 + \frac{\lambda}{4} \mathcal{M}^4 \\[2ex] &\textbf{Lagrangian \& energy :} \\[1ex] \mathcal{L}[I]{\mathcal{M}} = \frac{1}{2} \partial^\mu \mathcal{M} \, \partial[/I]\mu \mathcal{M} - V(\mathcal{M}) + \mathcal{M} \cdot S(x) \\[2ex] \mathcal{E}(x) = \frac{1}{2} (\partial_t \mathcal{M})^2 + \frac{1}{2} (\nabla \mathcal{M})^2 + V(\mathcal{M}) \\[2ex] &\textbf{Source term :} \\[1ex] S(x) = \epsilon \cdot \left[\mathcal{F}(x) - \mathcal{F}[I]{\text{local avg}}(x)\right] \cdot \tanh\left( \frac{\mathcal{C}(x) - \Lambda}{\sigma} \right) \\[2ex] &\textbf{Source-activation function :} \\[1ex] \mathcal{F}(x) = \left|\frac{\vec{E} \cdot \vec{B}}{B_0^2}\right| + \alpha \left|\frac{\partial_t \rho}{\rho_0 \omega_0}\right| + \beta \left|\frac{\nabla \cdot \vec{E}}{E_0 / \ell_0}\right| \\[2ex] \mathcal{F}[/I]{\text{local avg}}(x) = \frac{1}{V_{\delta}} \int_{|x - x'| < \delta} \mathcal{F}(x') \, d^3x' \\[2ex] \mathcal{C}(x) = \mathcal{I}(x) + \gamma \mathcal{T}(x) + \delta \mathcal{K}(x) \\[1ex] \mathcal{I}(x) = T^{00}(x), \quad \mathcal{T}(x) = \epsilon^{ijk} A_i \partial_j A_k, \quad \mathcal{K}(x) = \text{Tr}\left( R^\mu_{\ \nu\rho\sigma} R_\mu^{\ \nu\rho\sigma} \right) \\[2ex] &\textbf{Cꜷsality constraint :} \\[1ex] \left| \frac{\partial \mathcal{M}}{\partial t} \right| \leq c \left| \nabla \mathcal{M} \right| \\[2ex] &\textbf{E.-m. Energy coupling :} \\[1ex] \frac{\partial}{\partial t} \left( \frac{|\vec{E}|^2 + |\vec{B}|^2}{8\pi} \right) = -\mathcal{M}(x) \cdot S_{\text{E.-m.}}(x) \\[2ex] S_{\text{E.-m.}}(x) = \chi \cdot \left[ \frac{\vec{E} \cdot \vec{B}}{B_0^2} + \eta \cdot \frac{\nabla \cdot \vec{E}}{E_0 / \ell_0} + \xi \cdot \frac{\partial_t \rho}{\rho_0 \omega_0} \right] \\[2ex] &\textbf{Constants :} \\[1ex] \alpha, \beta, \gamma, \delta, \epsilon, \eta, \xi, \chi \in \mathbb{R}^+ \quad B_0, E_0, \ell_0, \rho_0, \omega_0 \in \mathbb{R}^+ \quad \Lambda, \sigma, \delta \in \mathbb{R}^+ \end{aligned} \]
Magic…Dayem. What you rambling about dude?
I feel you, man. Every time I try to think of the magic system for my story, I get headache and fear of contradicting elementsWhy dealing with magic has to be ʃo hard ?
what did You write since tge Last time I checked ?I feel you, man. Every time I try to think of the magic system for my story, I get headache and fear of contradicting elements
Not much, unfortunately, but I do have some good ideas that I keep repeating on my daydreams. I'd like to write some examples but I'll save it for later, when I can properly write them out.what did You write since tge Last time I checked ?
Sorry to hear that. Day is day-ing right along here.That said, good afternoon, American forum friends. Hope your day is going smoothly
![]()
Sorry for using the same image three times now. My two year of reaction image collection was wiped out when I moved it into a MicroSD card. I guess it got corrupted.
Good afternoon, fellow living organism. Watching a movie before I go to work. I will be twerking later.That said, good afternoon, American forum friends. Hope your day is going smoothly
![]()
Sorry for using the same image three times now. My two year of reaction image collection was wiped out when I moved it into a MicroSD card. I guess it got corrupted.
My word, such a baller move.Watching a movie before I go to work.