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Stress-Wave Propagation in the infinite plate and stress distribution on the Spur Gears Transmission by dynamic photoelasticity

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Stress-Wave Propagation in the Infinite Plate

and

Stress Distribution on the Spur Gears Transmission

by Dynamic Photoelasticity

Agus Sigit PRAMONO, Yves GOURINAT

Ecole Nationale Supérieure D’Ingénieurs de Constructions Aéronautiques 1, place Emile Blouin 31056 Toulouse Cedex France

Abstract

The aim of this paper is to present an original experimental approach of dynamics of solids and structures, considering dynamic application of photoelasticity. This application is used for industrial purpose (mechanism) and pedagogical illustration.

Introduction

Photoelasticity in conjunction with high-speed photography will be used in these experiments to visualize and to study the stress-wave propagation and stress distribution on the dynamic problems. A birefringent material with low Young Modulus like Urethane rubber (7 Mpa) is a good material for these cases because the velocities of propagation are quite small than steel so that they can be captured by high-speed camera . First, very short load are applied on the infinite plate at the middle and at the corner respectively. The isochromatic-fringe pattern which represents the state stress can be analyzed for the determination of the velocities of propagation of dilatation and distortion waves . Second, transmission system by spur gear is an interesting phenomenon for visualization stress distribution on the dynamics : the stress concentration, the stress of contact and the stress of impact by clearence on the teeth can be observed. The results will be compared by numerical method with finite elements non-linear explicit dynamic algorithms .

Stress-wave propagation

In problem of stress-wave propagation, the loading is applied to the body for a time which is very short when compared to the observation interval. The stress equation of motion in plane which may be written as

(! µ) "# # +2 $2 = 2 2 u u t and (! µ) " # # +2 $2 = 2 2 v v t (1)

! is Lame’s constant and µ is the shear modulus

Stress are imparted to a localized region surrounding the load point while the remainder of the body remains stress free. The inertia terms plays the dominant role in the dynamic stress . Hence, stress or fringes are transmitted through the body by stress wave which propagate at extremely high velocities as indicated by the relations shown below :

CL = !+ µ "

2

, the dilatation velocity (2) and CT = !

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Observation of equation (2) end (3) indicates that velocity CL is greather than velocity CT. Thus the two waves which are simultaneously generated will in general have difference shapes and will travel with different velocities. As a result the wave tend to separate as they propagate and in certain instances can easily be illustrated by mean of dynamic photoelasticity techniques. Spur gears transmission

The calculation of the stress on the gear transmission is based on the fatigue resistante (curve of Woler ) and the contact stress by Hertz. But if one of the gears is stopped immediatly or there is a clearence, the impact force will be appears. In this case, the stress is very high.

To investigate the stress distribution on the mating gears, the profile of the gears were designed by AutoCad software and then were transfered by CATIA software to be made with CNC machine. The urethane material was put between two aluminium plate so that the profil of the teeth is smoothly. To modelize numerically, DYNA3D sofware is used. This software can be used to analyse multiple contact surface pairs. It also includes a frictional model base on Coulomb’s law with static and dynamic coefficients of friction. For minimize the time of calculation four teeth of drive end driven were made.

Figure 1. The isochromatic-fringe pattern on the middle and the corner of the plate by a very short load with high-speed photography.

Figure 2. Stress distribution of the mating gears with finite elements method (DYNA3D).

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References

1. Durelli ,A.J et Riley , W.F, « Introduction to Photomechanics » , Prentice-Hall,1965. 2. Marc Andre Meyer, « Dynamic Behavior of Materials », John Wiley & Sons, 1994

3. James W. Dally, « An introduction to Dynamic Photoelasticity », Experimental Mechanics, 1980.

4. Dufailly Jacques, « Etude Geometrique des Engrenages Cylindriques de Transmission de

Puissance », Ellipses.

5. John O. Hallquist, Douglas W. Stillman, Tsung-Liang Lin, « Dyna3d » , Livermore Software Technology Corporation, 1994.

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