IsoAxis

From Math Images

Jump to: navigation, search
Image:inprogress.png

Animated IsoAxis

A dynamical system that shows the ideal motion of the model is not possible without a slight deformation.


Contents

Basic Description

Systematic animation of a mechanical system with multiple ties between the elements that compose it creates a variety of degrees of freedom that gives place to movement. The IsoAxis was discovered by Wallace Walker in 1958 (patent USA nº 3302321). The discovery took place in a project that was trying to find configurations for paper. In view of the IsoAxis discovery a new type of figures called Kaleidocycle was developed.

System's Description

The animated IsoAxis is formed by a two-dimensional folded paper that creates a grid of sixty isosceles triangles. These triangles can form a ring that has an outside in rotation forming beautiful shaped faces.

Figure 1 is the starting grid, there are a total of sixty isosceles triangles which are divided into six sectors of ten triangles. To further explain the construction, we will isolate one of these sectors.

Image:Br 4.jpg

In order to obtain the systematic explanation of the IsoAxis, the degrees of freedom have to be found. In figure 2 we take a given sector mimicking what the figure looks as the actual IsoAxis, from the individual sector we consider a vertex labeled 0. The opposition of this vertex has space that is appointed by three coordinates. If we take two additional angular coordinates we can determine the position of point 5 which is adjacent to point 0. If the points are defined, the union of this forms a straight line and with the help of another coordinate we can find the coordinate that closes the triangle, in this case it is point 1. If we take the same consideration for periods 1 to 6, these ones can be found, and 7,8 and 9 can be found by symmetry. In light of this information we need 10 points to find the answer to the system.

Image:Br2c.jpg‎

In order to make the ring structure, we have to add the necessary restrictions to the figure. Points 0, 1 and 2 have to be situated in the plane Y= \sqrt{3} X; as we see in figure 3, the points 3 and 6 have to be situated on top of the plane X=0 and from this information we can obtain 7 equations lowering down the degrees of freedom to 3. Figure 3 has points 4 and 5 as the center of the plane above the Y-Axis, if we give a latitude of the sector in the Z-Axis we can lower down the degrees of freedom to two. Figure 3 names the angles of the triangles alpha (α), beta (β), gamma (γ) and delta (δ) for further explanation.

Image:Brenda.jpg‎‎

Delta and alpha can be taken as degrees of freedom, associating delta as the direct variable for movement of the IsoAxis.

A More Mathematical Explanation

The coordinates of the points 0 to 6 can be found to be

Point 0= (UNIQf3856a78313c15-math-00000001 [...]

The coordinates of the points 0 to 6 can be found to be

Point 0= (  \sin \alpha , \sqrt{3}  \sin \alpha,  -\cos  \alpha  \sin \delta )

Point 1= (\frac{Y1}{\sqrt{3}} , Y_1, Z_1 )

Point 2 = ( \frac{Y2}{\sqrt{3}} , Y_2, Z_2 )

Point 3= (  0,\sqrt{3}  \sin  \alpha + \cos  \delta  \cos  \alpha- \sin  \delta + \sin  \beta, \cos  \delta - \cos  \beta )

Point 4 = (  0 , \sqrt{3}  \sin  \alpha + \cos \delta \cos  \alpha - \sin  \delta, \cos  \delta )

Point 5 = (  0,\sqrt{3}  \sin \alpha + \cos \delta \cos  \alpha + \sin  \delta, - \cos  \delta )

Point 6 = (  0,\sqrt{3}  \sin \alpha+ \cos \delta \cos \alpha + \sin  \delta + \sin  \gamma, - \cos  \delta + \cos  \gamma )

We can find six unknown coordinates: Y_1, Z_1, Y_2 , Z_2, \beta , \gamma This coordinate can be found analytically using equations that can be derive in the conditions of perpendicularity in between segments and the distance in between points.

System's Solution

One uses the coordinates [n, m] in order to appoint the segment that connects the vertex between n and m; ||[n, m]|| designates the distance between n and m.

The first step is to find point 1. This would be found by taking the following equations:

i. [0,5]\cdot [1,5] =0

ii.||[0, 5]|| = \sqrt{2}


By using the dot product we can expand to the following (if the vector is perpendicular then the dot product is equal to 0)

(X_0 - X_5) (X_1 - X_5) + (Y_0 - Y_5) (Y_1  - Y_5) + (Z_0 - Z_5) (Z_1 - Z_5) = 0

Replacing

X_5 by 0

X_1 by \frac{Y1}{\sqrt{3}}.

Then we obtain

(X_0 \frac{Y1}{\sqrt{3}}) + (Y_0 - Y_5) (Y_1 - Y_5) + (Z_0 - Z_5) (Z_1 - Z_5) = 0

Next

\frac{X0 Y1}{\sqrt{3}} + Y_1  (Y_0 - Y_5) + Z_1 (Z_0 - Z_5) = Y_5 ( Y_0 - Y_5) + Z_5 ( Z_0 - Z_5)

Giving

Y_1 ( \frac{X_0}{\sqrt{3}} + Y_0 -Y_5) + Z_1 (Z_0 -Z_5) = Y_5 ( Y_0 - Y_5) Z_5 ( Z_0 - Z_5)

Now

||[1,5]|| = \sqrt{2}

Means

 (X_1- X_5)^2 + (Y_1-Y_5)^2 + (Z_1 - Z_5)^2 = 2

Replacing

 X_1 by \frac{Y_1}{\sqrt{3}}

and

X_5 by  0

Gives

(\frac{Y_1}{\sqrt{3}})^2 + (Y_1 - Y_5)^2 + (Z_1 - Z_5)^2 = 2

(\frac{Y_1}{\sqrt{3}})^2 is equal to (X_1)^2

If Z_0 =Z_5 Then Y_1(\frac{X_0}{\sqrt{3}} + Y_0 - Y_5) = Y_5 (Y_0-Y_5)

So  Y_1= \frac{Y_5(Y_0 - Y_5)}{\frac{X_0}{\sqrt{3}} + Y_0 - Y_5}

We already know X_1= \frac{Y_1}{\sqrt{3}}

We also have

Z_1= Z_5 + \sqrt{2 - X_1^2 - (Y_1 - Y_5)^2}

If Z_0\neq Z_5 then divide both sides by (Z_0 - Z_5)


To get

Y_1 (\frac{\frac{X_0}{\sqrt{3}} + Y_0 - Y_5}{Z_0 - Z_5}) + Z_1 = \frac{Y_5 (Y_0 - Y_5)}{Z_0 - Z_5} + Z_5

Setting

Z_1 =B- A Y_1

Where

A = \frac{(\frac{ X_0 }{\sqrt{3}} + Y_0 - Y_5 )}{( Z_0 - Z_5 )}

B = \frac{Z_5 + ( Y_0 - Y_5 )}{ ( Z_0 - Z_5 )}

U = Y_5

V = Z_5

In which is possible to obtain Y_1 in function of (A,B,U,V) Giving

Z_1 = B - A Y_1

X_1 = \frac{Y_1 }{\sqrt{3}}

We see that

(\frac{Y_1}{\sqrt{3}})^2 + (Y_1 - U)^2 + (A - A Y_1 -V)^2 =2

This expands to

\frac{Y_1^2}{3} + Y_1^2 - 2U Y_1 + U^2 + B ^2 - 2 AB Y_1 + A ^2 Y_1 ^2 - 2 (B - A Y_1) + V ^2 =2

Which simplify

Y_1^2 (\frac{1}{3} + 1 + A ^2) + Y_1 (-2U - 2A B + 2A V)^2 -2 = 0

Giving

Y_1 = \frac{-2(A V - U - A B ) + \sqrt{4(A V - U- AB)^2 - 4(\frac{4}{3} + A^2)(U ^2 + (B - V)^2 -2)}}{2(\frac{4}{3} + A ^2)}

And then

Y_1 =\frac{ U +A (B - V) + \sqrt{(U + A (B - V))^2 - (\frac{4}{3} + A ^2)( U ^2 + (B - V)^2 - 2 )}}{\frac{4}{3} + A^2}

The solution for point 2 is analogous to point 1. This one can be found by substituting point 4 for point 5.

Work is shown


[0,4]\cdot [2,4]=0

[0,4]=<X_0 - X_4, Y_0-Y_4, Z_0-Z_4>

[2,4]=<X_2-X_4, Y_2-Y_4, Z_2-Z_4>

(X_0 - X_4)(X_2-X_4) + (Y_0-Y_4)(Y_2-Y_4)+(Z_0-Z_4)(Z_2-Z_4)=0

where

X_4= 0 and X_2 = \frac{Y_2}{ \sqrt{3} }

replacing this numbers we obtain

Y_2(\frac{X_0}{ \sqrt{3} } + Y_0-Y_4) +Z_2(Z_0-Z_4)=Y_4(Y_0-Y_4) +Z_4(Z_0-Z_4)

Then

||[2,4]||=\sqrt{2}

(X_2-X_4)^2 + (Y_2-Y_4)^2 + (Z_2-Z_4)^2=2

where we know that

X_2=\frac{Y_2}{ \sqrt{3} } and X_4=0

So

(\frac{Y_2}{ \sqrt{3} })^2 + (Y_2-Y_4)^2 + (Z_2-Z_4)^2 = 2

If Z_0=Z_4 then Y_2 (\frac{X_0}{ \sqrt{3} } + Y_0 - Y_4) = Y_4 (Y_0-Y_4)

So

Y_2= \frac{Y_4(Y_0-Y_4)}{\frac{X_0}{\sqrt{3}} + Y_0 - Y_4}

Again we know that X_2= \frac{Y_2}{\sqrt{3}}

Also

Z_2=Z_4 + \sqrt{2-X_2^2(-Y_2-Y4)^2}

If Z_0\neq Z_4 then divide by (Z_0- Z_4) to get

Y_2(\frac{\frac{X_0}{\sqrt{3}}+Y_0 - Y_4}{Z_0-Z_4}) + Z_2= \frac{Y_4(Y_0-Y_4)}{Z_0-Z_4} +Z_4

Once one have found point 1, we are able to find point 6 using perpendicularity conditions.

 [1 ,6] \cdot  [5, 6] = 0

Where

 1 = ( Y_1 - Y_5 ) \sin \gamma - ( Z_5 - Z_1 ) \cos \gamma

Y_6 = Y_5 + \sin \gamma

Z_6 = Z_5 + \cos \gamma

As shown in figure 4

Image:Figure 4.jpg

The solution for point 3 is analogous to the solution for point 6, this is also shown in Figure 4.

 1 = ( Y_2 - Y_4 ) \sin \beta - ( Z_2 - Z_4 ) \cos \beta

From figure 4 we see that

(Y_3-Y_4) = \sin \beta and (Z_3 - Z_4) = -\cos \beta

Figure 5 shows how point 4 and 5 were found.

Image:Plp.jpg

As Figure 5.2 shows,

\alpha is cut by the plane X=0.

X_0=\sin \alpha

Y_0=\sqrt{3}X_0

which equals

Y_0=\sqrt{3} \sin \alpha

In figure 5, we can see that from point 4 to point 5 cut by c, this angles are transversal, giving as a result to have equal angles, this are represented as angle \delta

Angle \omega=90^\circ - \delta

\cos \omega = \sin \delta

 \sin \omega = \cos \delta

An other important information is that

0^\prime = (0,Y_0,Z_0)

0=(X_0,Y_0,Z_0)

with this information we can asume that

Z_0=-\cos \delta \sin \delta

Z_4=\cos \delta

Z_5=-\cos \delta

We know:

X_4=0 X_5=0

this are place in plane X=0

Giving as a result:

Y_4=Y_0 - K but K= \sin \delta - \cos \alpha \cos \delta

so

Y_4=Y_0 + \cos \alpha \cos \delta - \sin \delta = \sqrt{3}\sin \alpha + \cos \alpha \cos \delta - \sin \delta

Giving

Y_5 = Y_0 + \cos \alpha \cos \delta + \sin \delta = \sqrt{3} \sin \alpha + \cos \alpha \cos \delta + \sin \delta


Why It's Interesting

The Iso-Axis model is interesting mathematically because it shows the coordination between angles and the relationship between them, the Iso-Axis shows imply Geometry in all aspects of the model. The figure is a beautiful representation of a simple piece of paper, it shows how something so simple can be much more complicated but at the same time interesting. This model shows that mathematics can be taken in to an other libel, in other words, this is an example of mathematical art. An example of the use of this models is the making of paper lamps in modern decorating designs, simple lamps that are made out of folded paper. After the discovery of the Iso-Axis the origami and some other design techniques were developed.

Image:Untitled copy.jpg


Teaching Materials

There are currently no teaching materials for this page. Add teaching materials.



Related Links

Additional Resources

Degrees of freedom

Dot product

Kaleidocycles

References

J.A Gutierrez[1]

The kaleidohedron from the IsoAxis grid:[2]

Wikipedia:[3]

Sahara Gabrielle:[4]

Wolfram MathWorld:[5]

Encyclopedia Britannica:[6]

Matematische:[7]





If you are able, please consider adding to or editing this page!

Have questions about the image or the explanations on this page?
Leave a message on the discussion page by clicking the 'discussion' tab at the top of this image page.






Personal tools