#### English Title

On the curve of fastest descent in whatever resistent medium

#### Enestrom Number

42

#### Fuss Index

378

#### Original Language

Latin

#### Published as

Journal article

#### Published Date

1740

#### Written Date

1734

#### Content Summary

Euler determines various properties of the brachistochrone curve subject to friction, taking the form of (*v/c*)* ^{n}*, where

*v*is the squared velocity and

*c*is the squared velocity at which the forces of friction and gravity cancel. He derives the brachistochrone property 2

*v*/

*r*=

*N*, where

*r*is the radius of curvature and

*N*is the component of force that is perpendicular to the curve. Euler recalls that the frictionless solution reads

*s*

^{2}= 2

*a*(

*s*–

*x*), for some constant

*a*, which is the already-established equation for a cycloid. He further considers the frictionless case with centripetal force taking the form

*y*, where

^{m}*y*is the distance to the attracting point. If

*a*is the initial distance from this point, the solution reads

*Az*

^{2}=

*a*

^{m+3}–

*y*

^{m+3}for some constant

*A*. Now, looking at the brachistochrone with friction, Euler calls the horizontal coordinate

*y*and the vertical coordinate

*x*. Defining

*p*=

*ds*/

*dx*, Euler finds that the equation 1/(

*p*

^{3n}

*q*

^{n}) =

*ng*

^{n-1}/(2

^{n-1}

*c*

^{n}) ∫ (

*p*

^{2}–1)

^{n-1}

*dp*/

*p*

^{2n}=

*P*

^{-n}must always hold, which reduces conveniently for

*n*=1. He then finds the solution

*s*= c∙ln((

*s*–

*ax*–

*ac*+

*c*)/(

*c*–

*ac*)), after which he proceeds to look for some expressions for the involved arc length. He ends by looking at how other methods would have influenced the solution and how this solution relates to the tautochrone.

#### Original Source Citation

Commentarii academiae scientiarum Petropolitanae, Volume 7, pp. 135-149.

#### Opera Omnia Citation

Series 1, Volume 25, pp.41-53.

#### Record Created

2018-09-25