Launching soon

Something brilliant is being computed.

A new kind of science lab for schools is almost ready. Schools already on board: your portal is open as always.

✦The current drifting behind this text is a live fluid simulation — a taste of what's coming.

i\hbar\,\partial_t \psi = \hat{H}\psi

\vec{F} = q(\vec{E} + \vec{v}\times\vec{B})

\ddot{\vec{r}} = -\tfrac{GM}{r^2}\hat{r}

\Delta x\,\Delta p \geq \tfrac{\hbar}{2}

\mathcal{L} = T - V

\oint \vec{B}\cdot d\vec{\ell} = \mu_0 I

\frac{\partial^2 u}{\partial t^2} = c^2 \nabla^2 u

E = \tfrac{1}{2}mv^2 - \tfrac{Gm_1m_2}{r}

T^2 \propto a^3

\|\delta(t)\| \sim e^{\lambda t}

\nabla \cdot \vec{E} = \tfrac{\rho}{\varepsilon_0}

S = \int \mathcal{L}\,dt

i\hbar\,\partial_t \psi = \hat{H}\psi

\vec{F} = q(\vec{E} + \vec{v}\times\vec{B})

\ddot{\vec{r}} = -\tfrac{GM}{r^2}\hat{r}

\Delta x\,\Delta p \geq \tfrac{\hbar}{2}

\mathcal{L} = T - V

\oint \vec{B}\cdot d\vec{\ell} = \mu_0 I

\frac{\partial^2 u}{\partial t^2} = c^2 \nabla^2 u

E = \tfrac{1}{2}mv^2 - \tfrac{Gm_1m_2}{r}

T^2 \propto a^3

\|\delta(t)\| \sim e^{\lambda t}

\nabla \cdot \vec{E} = \tfrac{\rho}{\varepsilon_0}

S = \int \mathcal{L}\,dt