Abstract
Theoretical and experimental studies on the influence of boundary conditions on the buckling of stiffened cylindrical shells and their vibrations are discussed. The effect of prebuckling deformations on the buckling loads and vibrations of stiffened shells is studied and compared with that in the case of unstiffened shells. The in-plane boundary conditions are found to be of particular importance for stiffened cylindrical shells and their effect differs significantly from that in unstiffened shells. The effect of axial restraints, which are found to be of prime importance in stringer-stiffened shells, are also studied.
By correlation with the vibration tests on the same shells a method is developed for definition of the actual boundary conditions of a stiffened shell non- destructively.
The effect of eccentricity of loading on stringer-stiffened shells is studied experimentally and correlated with vibration tests on the same shells.
Preliminary results of a non-destructive experimental method for prediction of buckling loads based on vibration testing of stiffened shells are also presented.
The research reported in this paper has been sponsored in part by the Air Force Office of Scientific Research, through the European Office of Aerospace Research, United States Air Force under Contract F44620-71-C-0116 and Grant 72-2394.
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Abbreviations
- A1, A2:
-
Cross section of stringer and ring, respectively
- a :
-
Ring spacing (distance between centers of rings)
- A, B :
-
Constants
- b 1 :
-
Stringer spacing (distance between centers of stringers)
- C1, C2, C3, C4:
-
Notation for clamped boundary conditions
- c1 :
-
Width of stringer
- d1 :
-
Height of stringer
- E :
-
Young’s modulus
- e1, e2 :
-
Stringer or ring eccentricity, respectively (distance from shell middle surface to stiffener centroid)
- ē:
-
Eccentricity of loading (distance from shell middle surface to the point of application of load)
- f :
-
Frequency
- h :
-
Thickness of shell
- I11, I22:
-
Moment of inertia of stringer or ring stiffener cross-section about its centroidal axis
- k 1 :
-
Axial elastic restraint
- k 4 :
-
Rotational elastic restraint
- L :
-
Length of shell
- M x :
-
Moment resultant in axial direction
- m :
-
Number of half longitudinal waves
- N x :
-
Axial membrane force resultant
- N xy :
-
Shear membrane force resultant
- n :
-
Circumferential wave number
- P :
-
Compressive axial load
- P CR :
-
Theoretical buckling load
- P PRE :
-
Theoretical buckling load with nonlinear prebuckling deformations considered
- P mem :
-
Theoretical buckling load with prebuckling deformation neglected
- P EXP :
-
Experimental buckling load
- R :
-
Radius to shell middle surface
- SS1, SS2, SS3, SS4:
-
Notation for simply supported boundary conditions
- u, v, w :
-
Displacements in axial, circumferential and radial directions respectively (radial direction positive inward)
- x :
-
Axial coordinate
- Z :
-
(1 - v 2)1/2 (L/R)2 (R/h), Batdorf shell parameter
- v :
-
Poisson’s ratio
- Q PRE :
-
PPRE/Pmem
- Q :
-
PEXP/Pmem, “linearity”
- η +1 :
-
Torsional stiffness parameter of stringer (see [3] or [22])
- φ:
-
Circumferential coordinate
- γ:
-
Free parameter for exponent of frequency
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Singer, J., Rosen, A. (1976). The Influence of Boundary Conditions on the Buckling of Stiffened Cylindrical Shells. In: Budiansky, B. (eds) Buckling of Structures. International Union of Theoretical and Applied Mechanics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-50992-6_21
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