01.02.2013 Views

MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd

MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd

MYSTERIES OF THE EQUILATERAL TRIANGLE - HIKARI Ltd

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Applications 101<br />

(a)<br />

Figure 3.32: Triangular Lower and Upper Bounds: (a) Vibrating Membrane.<br />

(b) Cylinder Under Torsion. [243]<br />

to the cross-section. The couple resisting such torsion is equal to θµP where<br />

θ is the twist or angle of rotation per unit length and µ is the shear modulus.<br />

So defined, P is a purely geometric quantity depending on the shape and<br />

size of the cross-section. Figure 3.32(a) shows one of the vibrational modes<br />

of a triangular membrane while Figure 3.32(b) shows the shear stress in the<br />

cross-section of an equilateral triangular prism under torsion.<br />

T<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

1<br />

0.8<br />

0.6<br />

y<br />

0.4<br />

0.2<br />

0<br />

0<br />

Figure 3.33: Fundamental Mode [219]<br />

Application 33 (Laplacian Eigenstructure). The eigenvalues and eigenfunctions<br />

of the Laplace operator, ∆ := ∂2<br />

∂x2 + ∂2<br />

∂y2, on the equilateral triangle<br />

play an important role in Applied Mathematics.<br />

0.2<br />

0.4<br />

x<br />

0.6<br />

0.8<br />

1<br />

(b)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!