buckling_spring

buckling_spring, an Octave code which illustrates solutions of the buckling spring equations.

We are given three points A, B, and C:

A is at the origin (0,0);
B has coordinates (X,Y) with Y nonnegative, and the ray from A to B makes an angle of THETA with the horizontal axis.
C is at the point (2*X,0).

Springs:

A spring extends from A to B; it is normally of length 1, and is currently of length L.
A spring extends from B to C; it is normally of length 1, and is currently of length L.
A spring force is also exerted, which tends to draw the two springs together, proportional to the angle between the two springs.

Forces:

A vertical load MU is applied at point B (downward is positive);

A horizontal load LAMBDA is applied at point C (leftware is positive);

The spring force is applied perpendicularly to the axes of the two springs.

If we compute F(1), the force along the axis of one spring, and F(2), the force perpendicular to the axis of one spring, we have that F(L,THETA,LAMBDA,MU) is given by:

F(1) = - 2 ( 1 - L ) + 2 * LAMBDA * cos ( THETA ) + MU * sin ( THETA )
F(2) = 0.5 * THETA - 2 * LAMBDA * L * sin ( THETA ) + MU * L * cos ( THETA )

To explore these equations, we can first solve for MU and LAMBDA in terms of L and THETA:

LAMBDA(L,THETA) = (1-L) * cos(THETA) + 0.25 * THETA * sin(THETA) / L
MU(L,THETA) = 2 * (1-L) * sin(THETA) - 0.5 * THETA * cos(THETA) / L

We can then study the behavior of solutions by choosing a fixed value of THETA (say pi/8), and plotting LAMBDA(L,THETA) versus MU(L,THETA) over a range of values of L, say from 0.25 to 1.75. Recall that L = 1 when the springs are at their "natural" length. This approach is taken by the function BUCKLING_SPRING_L.

We can also plot the same data, but instead fix a value of L, typically in the range of 0.25 to 1.75, and the plot LAMBDA(L,THETA) versus MU(L,THETA) over a range of values of THETA, say from -3pi/8 to +3pi/8. This approach is taken by the function BUCKLING_SPRING_THETA.

Usage:

To draw lines of constant L, with THETA varying along a line:

buckling_spring_l ( l_num, theta_num )

where

l_num is the number of L lines to draw;
theta_num is the number of THETA values along each L line.

To draw lines of constant THETA, with L varying along a line:

buckling_spring_theta ( l_num, theta_num )

where

l_num is the number of L values along each THETA line;
theta_num is the number of THETA lines to draw.

Licensing:

The computer code and data files described and made available on this web page are distributed under the MIT license

Languages:

buckling_spring is available in a Mathematica version and a MATLAB version and an Octave version.

Related Data and Programs:

buckling_spring_test

Reference:

Tim Poston, Ian Stewart,
Catastrophe Theory and its Applications,
Dover, 1996,
ISBN13: 978-0486692715,
LC: QA614.58.P66.

Source Code:

buckling_spring_l.m, chooses equally spaced values of THETA between -3pi/8 and +3pi/8, and plots curves of LAMBDA(L,THETA) versus MU(L,THETA) over a range of values of L, from 0.25 to 1.75.
buckling_spring_theta.m, chooses equally spaced values of L between 0.25 and 1.75 and plots curves of LAMBDA(L,THETA) versus MU(L,THETA) over a range of values of THETA, from -3pi/8 to +3pi/8.

Last revised on 12 June 2023.