Casual chatting thread

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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.
 
Dex-chan lover
Joined
Nov 18, 2018
Messages
13,285
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 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. :aquadrink:
 
Joined
Nov 24, 2024
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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 :
ql_595e6dabd7a1613c0aac68232acf17bd_l3.png
ql_7a8bd6a8519e4cd6f66a707d71f824d2_l3.png

\[ \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} \]
 
Last edited:
Dex-chan lover
Joined
May 29, 2023
Messages
888
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 :
ql_595e6dabd7a1613c0aac68232acf17bd_l3.png
ql_7a8bd6a8519e4cd6f66a707d71f824d2_l3.png

\[ \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} \]
were-gonna-kill-you.png
 
Dex-chan lover
Joined
Feb 5, 2025
Messages
214
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 :wowee:
What are you, AO3 author?
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 :
ql_595e6dabd7a1613c0aac68232acf17bd_l3.png
ql_7a8bd6a8519e4cd6f66a707d71f824d2_l3.png

\[ \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} \]
Dayem. What you rambling about dude?
 
Dex-chan lover
Joined
Jan 17, 2020
Messages
1,760
what did You write since tge Last time I checked ?
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.
The gist is that there exists a portal to the dream dimension (tentatively named Somnium Library). Halcyon and her crew is tasked with investigating it and what effects it could bring to the world. The crew then found out you can extract dreams and make it into your own power. However, overdoing it will turn it into "Nightmares" and it will force the user to indiscriminately attack everyone.


...More or less. Don't want to confuse other forum regulars with my WIPs
 
Supporter
Joined
Apr 26, 2020
Messages
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That said, good afternoon, American forum friends. Hope your day is going smoothly
r7qjwq.png

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.
Sorry to hear that. Day is day-ing right along here.
 
Dex-chan lover
Joined
May 29, 2023
Messages
888
That said, good afternoon, American forum friends. Hope your day is going smoothly
r7qjwq.png

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.
 

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