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Astronomy

Friedmann scale factor

Travel through cosmic time, compare expansion histories, and discover how matter, radiation and vacuum shape expansion, collapse or a bounce.

Friedmann scale factor — Actual application image
Actual application image

What happens

Homogeneous FLRW with non-negative matter, radiation and constant vacuum energy; curvature follows closure. Today is the expanding a=1 branch. Only its connected allowed history is integrated. Simple roots give a turn or bounce; near-double roots are marked critical. Singular endpoints do not give finite H or q. The history sculpture is a diagram, not a boundary or embedding of the universe. The local galaxy lattice does not depict spatial curvature. Enlarged fixed-size galaxy symbols represent comoving markers even at early times; galaxy formation is not simulated. Proper separations scale with a; bound objects do not. The camera can pull back automatically; numerical distances remain physical. No inflation, structure growth, perturbations or ray tracing. Reference B is immutable and drawn only inside its own calculated interval.

Equations used in the module
Equations
H²/H₀² = Ω_r/a⁴ + Ω_m/a³ + Ω_k/a² + Ω_Λ
Ω_k = 1 − Ω_r − Ω_m − Ω_Λ
a″ = Ω_Λ a − Ω_m/(2a²) − Ω_r/a³   [τ = H₀t]
q = −a a″ / a′²
1 + z = a_obs/a_em,   E_photon ∝ 1/a

Related experiments

Back to catalogue
Pulsar — Actual application image

Astronomy

Pulsar

A neutron star with its radio beam tilted from its spin axis is a lighthouse, and whether you see it, how often and for how long is one line of spherical trigonometry: cos θ = cos α cos ζ + sin α sin ζ cos φ. The beam sweeps within ρ of you or it does not; the second pole may sweep past too - the interpulse - and most pulsars are never seen at all, because their beams miss the Earth. Pulse width, duty cycle and the beamed fraction of the sky are measured on the profile and the sky, not quoted.

Gravitational waves — Actual application image

Physics / Astronomy

Gravitational waves

A compact binary spirals in and its quadrupole wave crosses the plane at retarded time: the two-armed spiral tightens as the orbit decays, and the detector trace chirps.

Gravitational lensing — Actual application image

Astronomy

Gravitational lensing

Move a galaxy across a caustic, inspect mirrored images and follow light paths in 3D. Compare a finite star with the ideal point-source limit.