Math 2.0

Calculus of variations and optimal control; optimization Classical problems Problem

Newton's minimal resistance problem

Builds on Integral functional with a Lagrangian densityConvex functionSurface of revolution

Problem

A solid body moves with constant speed along its axis through a rarefied medium. The particles of the medium do not interact with each other and bounce off the body elastically. Among convex bodies of revolution with base radius R>0R > 0 and height h>0h > 0, which shape has the least resistance?

In Newton's model, the body is {(x,z)∈ℝ2×ℝ:∣x∣≤R, 0≤z≤u(∣x∣)}\set{(x, z) \in \R^2 \times \R : \abs{x} \le R, \ 0 \le z \le u(\abs{x})}. Its profile u ⁣:[0,R]→[0,h]u \colon [0, R] \to [0, h] is concave and nonincreasing. The resistance is proportional to the integral functional F(u)=∫0Rr1+u′(r)2 dr.F(u) = \int_0^R \frac{r}{1 + u'(r)^2} \, dr. The problem is to minimise FF over such profiles.

Remarks

Newton stated the answer in the Principia. The optimal profile is not pointed: it has a flat disc of positive radius at the front, followed by a curved part that meets the disc at a nonzero angle. The convexity condition matters. Without it, profiles with steep zigzags make F(u)F(u) as small as one likes. But then particles would hit the body more than once, and the model no longer describes the resistance. Later work showed that convex bodies without rotational symmetry can have smaller resistance than Newton's body of the same radius and height.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Newton%27s_minimal_resistance_problem
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AboutCalculus of variations
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