Benchmark D2

VMD2
Barrel Vault Roof Under Self Weight

Overview

Reference:R. D. Cook, Concepts and Applications of Finite Element Analysis, 2nd Edition, John Wiley and Sons, Inc., 1981, pp. 284-287.
Analysis Type(s):Static Analysis (ANTYPE = 0)
Element Type(s):
4-Node Finite Strain Shell Elements (SHELL181)
8-Node Finite Strain Shell Elements (SHELL281)
Input Listing:vmd2.dat

Test Case

A cylindrical shell roof is subjected to gravity loading. The roof is supported by walls at each end and is free along the sides. Monitor the y-displacement and bottom axial stress (σz) at target point 1 along with the bottom circumference stress (σθ) at target point 2 for a series of test cases with varying skew angle β for each element type. A companion problem that studies uniform element mesh refinement is VMC3.

Figure 605: Cylindrical Shell Roof Problem Sketch

Cylindrical Shell Roof Problem Sketch

Material PropertiesGeometric PropertiesLoading and Boundary Conditions
E = 4.32 x 108 N/m2
υ = 0.0
ρ = 36.7347 kg/m3
Parameter Definitions
β = Skew Angle
L = 50 m
R = 25 m
t = 0.25 m
Θ = 40°
g = 9.8 m/sec2
At x = 0 Symmetric
At z = 0 Symmetric
At x = L UX = UY = ROTZ = 0

Representative Mesh Options

Target Solution

Target solution is obtained using a uniform 8 x 8 quadrilateral mesh of an 8-node quadrilateral shell element, (see R. D. Cook, Concepts and Applications of Finite Element Analysis).

ETYPBeta (Deg.)Alpha (Deg.)UY (1), inAxial Stress (1) Bottom,kPaHoop Stress (2) Bottom,kPa
--9090-.3016358.42-213.40

Results Comparison - Quadrilateral Elements

   Ratio
ETYPBetaAlphaUY (1)Axial Stress (1) BottomHoop Stress (2) Bottom
18165133.41.0190.9460.918
18177.51061.0370.9500.965
18190901.0480.9400.983
18111075.11.0560.9100.956
18113066.21.0550.8630.889
28165133.40.9740.9851.133
28177.51060.9990.9671.049
28190901.0040.9531.027
28111075.10.9940.9491.049
28113066.20.9710.9601.059

Assumptions, Modeling Notes, and Solution Comments

  1. The problem is designed to test singly-curved shell elements under combined membrane and bending deformation. The solid model is set up to produce irregular element shapes for quadrilateral elements. The angle β is prescribed, while the angle α is calculated from the resulting geometry. The range of β is set such that all element interior angles fall within 90° ± 45°.

  2. The target solution is obtained from the author's 8-node shell element, (see R. D. Cook, Concepts and Applications of Finite Element Analysis), under a uniform rectangular element geometry using an 8 x 8 mesh pattern.

  3. Results for uniform quadrilateral element shapes are noted in the tabular and graphical output for β = 90° and should be used as a basis for comparison of distorted element performance.

  4. Displacement results over the range of element distortion vary the greatest for SHELL181. In this problem, SHELL281 predict the displacements more accurately for mild element geometry distortion.

  5. Axial (σz) stress results, over the range of element distortion, show some variation for SHELL181, and SHELL281 elements. Hoop (σθ) stress results are less affected by irregular element shapes except at the extreme β angle range.