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2013 | OriginalPaper | Buchkapitel

8. Beam with Shear Contribution

verfasst von : Andreas Öchsner, Markus Merkel

Erschienen in: One-Dimensional Finite Elements

Verlag: Springer Berlin Heidelberg

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Abstract

By this element the basic deformation bending under consideration of the shear influence will be described. First, several basic assumptions for the modeling of the Timoshenko beam will be introduced and the element used in this chapter will be distinguished from other formulations. The basic equations from the strength of materials, meaning kinematics, the equilibrium as well as the constitutive equation will be introduced and used for the derivation of a system of coupled differential equations. The section about the basics is ended with analytical solutions. Subsequently the Timoshenko bending element will be introduced with the definitions for load and deformation parameters which are commonly accepted at the handling via the FE method. The derivation of the stiffness matrix at this point also takes place via various methods and will be described in detail. Besides linear shape functions a general concept for an arbitrary arrangement of the shape functions will be introduced.

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Fußnoten
1
For a function \(f(x,y)\) of two variables usually a TAYLOR’ s series expansion of first order is assessed around the point \((x_0, y_0)\) as follows: \(f(x,y)=f(x_0+\text{d} x,y_0 +\text{d} x)\approx f(x_0, y_0)+\left(\displaystyle \frac{\partial f}{\partial x}\right)_{x_0, y_0}\times (x-x_0)+\left(\displaystyle \frac{\partial f}{\partial y}\right)_{x_0, y_0}\times (y-y_0)\).
 
2
A closer analysis of the shear stress distribution in the cross-sectional area shows that the shear stress does not just alter through the height of the beam but also through the width of the beam. If the width of the beam is small compared to the height, only a small change along the width occurs and one can assume in the first approximation a constant shear stress throughout the width: \(\tau _{xy}(y,z) \rightarrow \tau _{xy}(y)\). See for example [1, 2].
 
3
One notes that in the English literature often the so-called form factor for shear is stated. This results as the reciprocal of the shear correction factor.
 
4
Maple\(^{\textregistered} \), Mathematica\(^{\textregistered} \) and Matlab\(^{\textregistered} \) can be listed at this point as commercial examples.
 
5
A numerical Gauss integration with two integration points yields the same results as the exact analytical integration.
 
6
For this see Fig. 8.6 and the supplementary problem 8.6.
 
7
One considers the definition of \(I_z\) and \(A\) in Eq. (8.111) and divides the fraction by \(h^3\).
 
8
For this see Fig. 8.6 and the supplementary problem 8.6.
 
9
The numerical integration according to the GaussLegendre method with \(n\) integration points integrates a polynomial, which degree is at most \(2n-1\), exactly.
 
10
MacNeal hereford uses the expression ‘residual bending flexibility’ [16, 17].
 
11
For this see the supplementary problem 8.5.
 
12
At the so-called Lagrange interpolation, \(m\) points are approximated via the ordinate values with the help of a polynomial of the order \(m-1\). In the case of the Hermite interpolation the slope of the regarded points is considered in addition to the ordinate value. For this see Chap. 6.
 
13
It needs to be remarked that the influence of distributed loads is disregarded in the derivation. If distributed loads occur, the equivalent nodal loads have to be distributed on the remaining nodes.
 
14
A similar example is presented in [19].
 
15
For this see the supplementary problem 8.6.
 
Literatur
1.
Zurück zum Zitat Timoshenko SP, Goodier JN (1970) Theory of elasticity. McGraw-Hill, New YorkMATH Timoshenko SP, Goodier JN (1970) Theory of elasticity. McGraw-Hill, New YorkMATH
2.
Zurück zum Zitat Beer FP, Johnston ER Jr, DeWolf JT, Mazurek DF (2009) Mechanics of materials. McGraw-Hill, Singapore Beer FP, Johnston ER Jr, DeWolf JT, Mazurek DF (2009) Mechanics of materials. McGraw-Hill, Singapore
3.
Zurück zum Zitat Cowper GR (1966) The shear coefficient in Timoshenko’s beam theory. J Appl Mech 33:335–340MATHCrossRef Cowper GR (1966) The shear coefficient in Timoshenko’s beam theory. J Appl Mech 33:335–340MATHCrossRef
5.
Zurück zum Zitat Weaver W Jr, Gere JM (1980) Matrix analysis of framed structures. Van Nostrand Reinhold Company, New York Weaver W Jr, Gere JM (1980) Matrix analysis of framed structures. Van Nostrand Reinhold Company, New York
6.
Zurück zum Zitat Gere JM, Timoshenko SP (1991) Mechanics of materials. PWS-KENT Publishing Company, Boston Gere JM, Timoshenko SP (1991) Mechanics of materials. PWS-KENT Publishing Company, Boston
7.
Zurück zum Zitat Gruttmann F, Wagner W (2001) Shear correction factors in Timoshenko’s beam theory for arbitrary shaped cross-sections. Comput Mech 27:199–207MATHCrossRef Gruttmann F, Wagner W (2001) Shear correction factors in Timoshenko’s beam theory for arbitrary shaped cross-sections. Comput Mech 27:199–207MATHCrossRef
9.
Zurück zum Zitat Reddy JN (1984) A simple higher-order theory for laminated composite plate. J Appl Mech 51:745–752MATHCrossRef Reddy JN (1984) A simple higher-order theory for laminated composite plate. J Appl Mech 51:745–752MATHCrossRef
10.
Zurück zum Zitat Reddy JN (1997) Mechanics of laminated composite plates: theory and analysis. CRC Press, Boca RatonMATH Reddy JN (1997) Mechanics of laminated composite plates: theory and analysis. CRC Press, Boca RatonMATH
11.
Zurück zum Zitat Reddy JN (1997) On locking-free shear deformable beam finite elements. Comput Method Appl Mech Eng 149:113–132MATHCrossRef Reddy JN (1997) On locking-free shear deformable beam finite elements. Comput Method Appl Mech Eng 149:113–132MATHCrossRef
12.
Zurück zum Zitat Wang CM (1995) Timoshenko beam-bending solutions in terms of Euler-Bernoulli solutions. J Eng Mech-ASCE 121:763–765CrossRef Wang CM (1995) Timoshenko beam-bending solutions in terms of Euler-Bernoulli solutions. J Eng Mech-ASCE 121:763–765CrossRef
13.
Zurück zum Zitat Cook RD, Malkus DS, Plesha ME, Witt RJ (2002) Concepts and applications of finite element analysis. Wiley, New York Cook RD, Malkus DS, Plesha ME, Witt RJ (2002) Concepts and applications of finite element analysis. Wiley, New York
14.
Zurück zum Zitat Reddy JN (2006) An introduction to the finite element method. McGraw Hill, Singapore Reddy JN (2006) An introduction to the finite element method. McGraw Hill, Singapore
15.
Zurück zum Zitat MacNeal RH (1994) Finite elements: their design and performance. Marcel Dekker, New York MacNeal RH (1994) Finite elements: their design and performance. Marcel Dekker, New York
16.
Zurück zum Zitat Russel WT, MacNeal RH (1953) An improved electrical analogy for the analysis of beams in bending. J Appl Mech 20:349–355 Russel WT, MacNeal RH (1953) An improved electrical analogy for the analysis of beams in bending. J Appl Mech 20:349–355
17.
18.
Zurück zum Zitat Reddy JN (1999) On the dynamic behaviour of the Timoshenko beam finite elements. Sadhana-Acad Proc Eng Sci 24:175–198MATH Reddy JN (1999) On the dynamic behaviour of the Timoshenko beam finite elements. Sadhana-Acad Proc Eng Sci 24:175–198MATH
19.
Zurück zum Zitat Steinke P (2010) Finite-Elemente-Methode–Rechnergestützte Einführung. Springer, Berlin Steinke P (2010) Finite-Elemente-Methode–Rechnergestützte Einführung. Springer, Berlin
20.
Zurück zum Zitat Hibbeler RC (2008) Mechanics of materials. Prentice Hall, Singapore Hibbeler RC (2008) Mechanics of materials. Prentice Hall, Singapore
Metadaten
Titel
Beam with Shear Contribution
verfasst von
Andreas Öchsner
Markus Merkel
Copyright-Jahr
2013
Verlag
Springer Berlin Heidelberg
DOI
https://doi.org/10.1007/978-3-642-31797-2_8

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