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Use of a curved grating in shadow moiré

Shadow moiré with a non-plane grating has been used to investigate the large displacements of a uniformly loaded hyperboloid-parabolic shell

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Abstract

The shadow-moiré method has been extended to study the large displacements of a uniformly loaded hyperbolic-paraboloid shell. The new technique employs a curved grating which is everywhere equidistant from the initial position of the surface, as in the application of a plane grating in the study of plates. The theory of the curved grating is developed. Experimental verification is reported and a significant increase in accuracy over the equivalent plane grating is observed. The proposed improvement can be applied to the study of any ruled surface.

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Abbreviations

a :

half length of hypar (mm)

b :

half width of hypar (mm)

c :

half height of hypar (mm)

d :

vertical distance between model and grating in the initial state (curved grating) (mm)

k :

index referring to a line of the grating (dimensionless)

L :

horizontal distance between light source and edge of model (mm)

l :

index referring to a line of the shadow of the grating (dimensionless)

M :

vertical distance from grating to observer (plane grating) (mm); vertical distance from reference plane to observer (curved grating) (mm)

N :

moiré-fringe order (dimensionless)

p :

pitch of the grating (mm)

T :

horizontal distance between the edge of the surface and the edge of the grating (mm)

W :

vertical distance from the grating to the light source (plane grating) (mm); vertical distance from the reference plane to the light source (curved grating) (mm)

x,y,z :

coordinates on the model surface (plane grating) (mm)

x′,y′,z′ :

coordinates on the model surface (curved grating) (mm)

x m ,y m :

coordinates measured in the grating plane (plane grating) (mm); coordinates measured in the reference plane (curved grating) (mm)

γ:

angle between the vertical and the light rays from the observer to the model (rad)

δ:

vertical distance between the grating and the point (x, y, z) (plane grating) (mm); vertical distance between the grating and the point (x′, y′, z′) (curved grating) (mm)

θ:

angle between the vertical and the light ray from the source to the model (rad)

References

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Work was performed while he was Research Associate, Swiss Federal Institute of Technology, Lausanne, Switzerland.

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Marasco, J. Use of a curved grating in shadow moiré. Experimental Mechanics 15, 464–470 (1975). https://doi.org/10.1007/BF02318361

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  • DOI: https://doi.org/10.1007/BF02318361

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