Fri., Jan. 27

Reblogged from gregruben.

Posted 2 days ago.

commonchant:

Gunta Stolzl Bauhaus weaving

commonchant:

Gunta Stolzl Bauhaus weaving

Fri., Jan. 27

Posted 2 days ago.

Wed., Jan. 25

Reblogged from puremagenta.

Posted 4 days ago.

puremagenta:

MOTTO, unknown (if you know the source, let me know!)

puremagenta:

MOTTO, unknown (if you know the source, let me know!)

Wed., Jan. 25

Posted 4 days ago.

Camila Leon

Camila Leon

Wed., Jan. 25

Reblogged from boomsams.

Posted 4 days ago.

Wed., Jan. 25

Posted 4 days ago.

Mon., Jan. 23

Posted 6 days ago.

Mon., Jan. 23

Reblogged from puremagenta.

Posted 6 days ago.

(Source: kissface)

Sun., Jan. 22

Reblogged from good.

Posted 1 week ago.

good:

Sometimes the perfect thing to brighten your day is to watch an 8-year-old sing Hardcore. 

laughingsquid:

My First Hardcore Song by an 8-Year-Old Punk Rock Girl Named Juliet

Thu., Jan. 19

Posted 1 week ago.

:These images are excerpts from the bifurcation diagrams of various one-dimensional maps, including the logistic map [third from top], the hat map [second from bottom], and the cosine map [top image]. Each of these dynamical systems model various physical phenomena in the real world. For example, the logistic map is a crude model of population dynamics with reproduction and limited resources, and it is often used as an example of the period-doubling route to chaos. Typical of chaotic systems, many regions in these figures exhibit self-similarity and reflect the order that emerges out of chaos.These images were generated numerically by iterating the discrete-time maps above as a bifurcation parameter is varied. The bifurcation parameter is plotted as the y-axis (elevation), and at each elevation, the stratified layer represents the attracting set of the dynamical system for that particular choice of bifurcation parameter. Bifurcation refers to a qualitative change in the behavior or topology of a dynamical system as a parameter is varied.” 
via Princeton’s Art of Science Gallery

:These images are excerpts from the bifurcation diagrams of various one-dimensional maps, including the logistic map [third from top], the hat map [second from bottom], and the cosine map [top image]. Each of these dynamical systems model various physical phenomena in the real world. For example, the logistic map is a crude model of population dynamics with reproduction and limited resources, and it is often used as an example of the period-doubling route to chaos. Typical of chaotic systems, many regions in these figures exhibit self-similarity and reflect the order that emerges out of chaos.

These images were generated numerically by iterating the discrete-time maps above as a bifurcation parameter is varied. The bifurcation parameter is plotted as the y-axis (elevation), and at each elevation, the stratified layer represents the attracting set of the dynamical system for that particular choice of bifurcation parameter. Bifurcation refers to a qualitative change in the behavior or topology of a dynamical system as a parameter is varied.” 

via Princeton’s Art of Science Gallery