
A metric on the sphere
At a chosen latitude, the metric is an ordinary matrix. Its symbolic curvature remains a separate calculation.
theta=pi/3 g=[1,0;0,sin(theta)^2] det(g) inv(g)
Mathematics from differential geometry, engineering, physics, information theory, and original manuscript sources, with concise inputs and honest scope notes.

At a chosen latitude, the metric is an ordinary matrix. Its symbolic curvature remains a separate calculation.
theta=pi/3 g=[1,0;0,sin(theta)^2] det(g) inv(g)

Vectorized arrays let you compare a dynamic response against its envelope.
omega=4; zeta=0.08 t=linspace(0,8,401) x=exp(-zeta*omega*t)*cos(omega*sqrt(1-zeta^2)*t) plot(t,x,"Damped response")

The complex structure starts with a simple antisymmetric tensor from Hamiltonian mechanics.
J=[0,1;-1,0] J@J

A single expression generates an entire entropy curve.
p=linspace(0.01,0.99,199) H=-(p*log2(p)+(1-p)*log2(1-p)) plot(p,H,"Binary entropy")

Typed slots distinguish upper/lower variance from barred/unbarred conjugation.
h=metric([1,0;0,1],"V","hermitian") u=indexed([1+i,2],"^a","V") tinner(u,u,h) # 6

A finite-dimensional numerical adaptation of the antisymmetric connection in a rotating frame.
W=[0,3,-2;-3,0,1;2,-1,0] transpose(W)+W W@[1,0,0]

Measured inputs retain identity, so using the same variable twice preserves the dependency.
a=measure(2,0.1,"m") sigma(a-a) # 0