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How are similar symmetries and identical deviation interacting

Abstract and 1. Introduction

1.1 Methotopia depends on polyethylene for audio control

2 micromorphic modeling is comfortable for the limited size material

2.1 Quartet symmetry / flexible tensioner shape (in Voigt Ten

3 distraction curves

4 new considerations on comfortable micromorphic parameters

4.1 The comfortable micromorphic model regarding the change in the characteristics of the feast of the unit cell

4.2 The consistency of the comfortable micromorphic model with regard to the change in the size of the unit cell

4.3 convenient micromorphic pieces

5 Installing comfortable microscopic parameters: a specific case of the curvature of the fading (without the Pixen P and Curl P˙)

5.1 approaches

5.2 Composition

5.3 Discussion

6 Micromorphic parameters installation with bending (with a bar)

6.1 approaches and 6.2 installation

6.3 Discussion

7 Micromorphic parameter installation with enhanced motor energy (with P˙) and 7.1 approximately

7.2 Composition

7.3 Discussion

8 summary of the results obtained

9 conclusion and views, thanks and appreciation, and references

The most prominent arrangement of 4 tensioners in the quadruple quadruple symmetry

B

C distraction curves transactions with p

D Transactions for District Curbs with P Kha B.

The most prominent arrangement of 4 tensioners in the quadruple quadruple symmetry

Looking at the following spring form

Where it is a tensioner of fourth and D is one of the second requests, and the most forms L

Where the arrangement of the vector associated with the Spring model A.1

If we now divide the tensioner D in the symmetrical part and deviation, then the corresponding vector in Voigt Tennis

Because of the symmetry category that was considered, it is necessary to take into account the mixed foundational matrix that flourishes the symmetrical part and deviation from D in order to build the Sprite model Y

B

C distraction curves transactions with Halleh p


Authors:

(1) Jendrik voss, Mechanics and Structural Dynamics Institute, Dortmund Technical University and author against ([email protected]);

(2) Gianluca Rizzi, Mechanics and Structural Dynamics Institute, Dortmund Technical University;

(3) Patrizio NEF, head of non-linear analysis and modeling, College of Mathematics, Duisburg-Assen University;

(4) Angela Sanu, Institute of Mechanics Structural and Dinas, Dortmund Technical University.

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