Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Ponytail
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
== Scientific studies == [[File:Street Parade 2013 033.jpg|thumb|A woman's ponytail from the side]] The first equation of state for hair was developed by C. F. van Wyk in 1946.<ref>Wyk, C. M. V. (1946). "[https://doi.org/10.1080/19447024608659279 20βNote On The Compressibility Of Wool]." ''Journal of the Textile Institute Transactions'', 37(12).</ref> Scientists in the UK have formulated a [[mathematical model]] that predicts the shape of a ponytail given the length and random curvature (or curliness) of a sample of individual hairs. The Ponytail Shape Equation provides an understanding of how a ponytail is swelled by the outward pressure which arises from interactions between the component hairs.<ref name=Scienceponytail>"[https://www.bbc.co.uk/news/science-environment-17012795 Science behind ponytail revealed]."(2012, 13 February)</ref> The researchers developed a general [[Continuum (theory)|continuum theory]] for a bundle of hairs, treating each hair as an elastic filament with random intrinsic curvature. From this they created a [[differential equation]] for the shape of the bundle relating the elasticity, gravity, and orientational disorder and extracted a simple [[equation of state]] to relate the swelling pressure to the measured random curvatures of individual hairs.<ref name=Goldstein2012>Goldstein, R. E., Warren, P. B., & Ball, R. C. (2012). "[https://doi.org/10.1103/physrevlett.108.078101 Shape of a Ponytail and the Statistical Physics of Hair Fiber Bundles]." ''Physical Review Letters'', 108(7).</ref><ref>{{cite journal|title=Synopsis: Ponytail physics|url=http://physics.aps.org/synopsis-for/10.1103/PhysRevLett.108.078101|journal=Physical Review Letters|date=13 February 2012|volume=5|doi=10.1103/PhysRevLett.108.078101|pmid=22401258|access-date=14 February 2012|last1=Goldstein|first1=R. E.|last2=Warren|first2=P. B.|last3=Ball|first3=R. C.|issue=7|page=078101|arxiv=1204.0371|s2cid=31964168}}</ref> The equation itself is a fourth order non linear differential equation.<ref name=Goldstein2012 /> The Rapunzel number is a ratio used in this equation to calculate the effects of gravity on hair relative to its length.<ref name=Goldstein2012 /> {{math|''Ra'' β‘ ''{{sfrac|L|l}}''}} This number determines whether a ponytail looks like a fan or whether it arcs over and becomes nearly vertical at the bottom. A short ponytail of springy hair with a low Rapunzel number, fans outward. A long ponytail with a high Rapunzel number, hangs down, as the pull of gravity overwhelms the springiness. It is now also known why jogger's ponytails swing side to side.<ref name="Keller2012">Keller, J. B. (2010). "[https://doi.org/10.1137/090760477 Ponytail Motion]." ''SIAM Journal on Applied Mathematics'', 70(7), 2667β2672.</ref> An up and down motion is too unstable: a ponytail cannot sway forward and backward because the jogger's head is in the way. Any slight jostling causes the up and down movement to become a side to side sway. The research on the shape of the ponytail won the authors the [[Ig Nobel]] for Physics in 2012.<ref>{{cite web | url=http://www.improbable.com/ig/winners/#ig2012 | title=The 2012 Ig Nobel Prize Winners | work=Improbable Research | date=August 2006 | access-date=14 August 2016}}</ref> The Rapunzel number is important for the [[computer graphics]] and [[animation]] industry, as it helps animators resolve challenges relating to the realistic digital representation of hair and hair movement.<ref name=Scienceponytail />
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)