Objective

To determine the deformed state of a cantilever circular bar of constant cross-section under in‑plane concentrated loads and a moment applied at the free end.

Reference

J.S. Przemieniecki, Theory of matrix structural analysis, New York, McGraw-Hill, 1968.

Problem statement

A cantilever circular bar of constant cross-section is subjected at its free end to:
- a concentrated horizontal (normal) load F1;
- a concentrated vertical (tangential) load F2;
- a moment M,
all acting in the plane of the bar.

To determine the horizontal displacement X, the vertical displacement Z, and the rotation angle uY at the free end of the bar (point B).

Design model

The design model is a cantilever circular bar of constant cross-section.

Initial geometry

Initial geometry

Geometry

Radius of the arc of the longitudinal axis of the cantilever circular bar r = 3,0 m
Central angle corresponding to the arc length of the longitudinal axis of the cantilever circular bar α = 90°
Outer diameter of the circular cross-section of the bar de = 0,02 m
Inner diameter of the circular cross-section of the bar di = 0,016 m

Material properties

Modulus of elasticity Е = 2,0 * 1011 Pa
Poisson's ratio ν = 0,3

Boundary conditions

The boundary conditions are provided by applying restraints in the X, Z, and uY degrees of freedom directions (point A).

Loads

Horizontal concentrated load F1 = 10 N, applied at point B;
Vertical concentrated load F2 = 5 N, applied at point B;
Concentrated moment M = 8 N*m, applied at point B.

Output data

Design and deformed shapes

Mosaic plot of horizontal displacements along the global X-axis (w), m.

Design and deformed models
Mosaic plot of horizontal displacements along the global X-axis (w), m

Mosaic plot of vertical displacements along the global Z-axis (w), m.

Mosaic plot of rotation angles about the global Y-axis (u), rad*1000.

Mosaic plot of vertical displacements along the global Z-axis (w), m
Mosaic plot of rotation angles about the global Y-axis (u), rad*1000

Analytical solution

X = r2/(E*I)*(M+F1*r*π/4+F2*r*1/2;
Z = r2/(E*I)*(M*(π/2-1)+F1*r*1/2+F2*r*(3*π/4-2));
uY = -r/(E*I)*(M*π/2+F1*r+F2*r*(π/2-1));
I = (π*d4e/64*(1-(di/de)4).

Comparison of calculation results

Parameter (point B) Theory LIRA-FEM Error, %
Horizontal displacement X, m 3,7908*10-1 3,78823*10-1 0,0678
Vertical displacement Z, m 2,4173*10-1 2,41742*10-1 0,00496
Rotation angle uY, rad*1000 -1,6539*10-1 -1,6535*10-1 0,02419

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