This document discusses the stick and rope problem of finding a smooth function that maximizes the area under the graph subject to the constraint that the length of the graph is a given fixed value.
The problem is analyzed for the case where both ends of the rope are fixed at zero. It is shown that when the fixed length is between 1 and π/2, the optimal solution is a segment of a circle with its center on the vertical line at t=1/2.
The proof uses Lagrange multipliers to derive an equation that the optimal function must satisfy, showing it is the equation of a circle. Boundary conditions then determine the circle's parameters. Special cases for longer rope lengths are also discussed
Organic Name Reactions for the students and aspirants of Chemistry12th.pptx
On the Stick and Rope Problem - Draft 1
1. On The Stick and Rope Problem
Iwan Pranoto
Institute of Technology Bandung
pranoto@math.itb.ac.id
November 19, 2012
2. Problem
Isoperimetric Problem in Halfplane?
Finding a smooth function x on I = [0, 1] satisfying
x(0) = x(1) = 0 and the area formed by the graph of x and the
interval I is maximum, with a constrain: the length of the graph of
x must be , where is a positive number given but fixed.
3. Stick and Rope
Figure: Free Ends, Left; Fixed Ends, Right
In this paper, we consider the right situation.
5. We assume x(t) ≥ 0 for all t. Therefore, the area A of the region
bounded by the graph of x and I is to be maximized
1
A[x] = x(t) dt,
0
and at the same time the length L[x] = , where
1
L[x] = 1 + (x)2 dt.
˙ (1)
0
6. Results
Theorem
If 1 < ≤ π , the optimal solution of the problem is a segment of a
2
circle whose center is on the vertical line t = 1 .
2
7. Proof
Using Lagrange method, define a new form
1
¯
A[x, x, λ] =
˙ x(t) − λ 1 + (x)2 −
˙ dt.
0
After substituting this into the Euler-Lagrange equation, we obtain
∂
x(t) − λ 1 + (x)2 −
˙
∂x
d ∂
= x(t) − λ 1 + (x)2 −
˙ . (2)
dt ∂x
˙
8. This leads to
d λx
˙
1= .
dt 1 + (x)2
˙
After integrating both sides with respect to t, we obtain
λx
˙
t= + C1
1 + (x)2
˙
for some constant C1 . Thus, x must satisfy
(λx)2
˙
(t − C1 )2 = . (3)
1 + (x)2
˙
9. Since x vanishes only if t = C1 , one obtains
˙
1 + (x)2
˙ λ2
2
= .
x
˙ (t − C1 )2
Thus,
1 λ2 − (t − C1 )2
= ,
x2
˙ (t − C1 )2
or
(t − C1 )
x =±
˙ .
λ2 − (t − C1 )2
Therefore, x must satisfy
x = ± λ2 − (t − C1 )2 + C2
for some constant C2 , or
(x − C2 )2 = λ2 − (t − C1 )2 . (4)
10. This means, x must satisfy the equation of a circle whose center is
(C1 , C2 )
(t − C1 )2 + (x − C2 )2 = λ2 . (5)
After using the conditions x(0) = x(1) = 0, one obtains C1 = 1 .2
Thus, the circle’s center must lie on the vertical line t = 1 .
2
One may compute the other constants, the center’s ordinate −|C2 |
and radius |λ|, geometrically.
12. How if > π/2?
We consider = 2 and a special kind of functions:
m
1 1
x(t) = a |t − |m − ,
2 2
where m is any natural number greater than 1 and a is some
constant to be chosen, depending on m.
Figure: Table, Left; Numerical Results, Right
13. How About A Rectangle and A Semicircle?
Figure: The Area = (1 − π ) ≈ 0.60730091830 · · ·
8