EC3 does not include a formula for the elastic critical moment and hence the NCCI (Non-contradictory Complementary Information) is used here. The critical elastic moment (
Mcr
) is an input into the buckling resistance moment (
Mb,Rd
) which is crucial for assessing the capacity of a section in bending.
Calculation
📃Technical notes
The calculator is only valid for
k=1
. The effective length factor,
k
depends on the restraint conditions at supports. A value of
k=1
assumes both flanges at the supports are free to rotate on plan.
When either uniform or linear moment distribution is selected for "Applied load type", the calculator sets a default value for "Load application" while the "Support type" does not impact the calculation. The "Load application" defaults to top flange.
When either parabolic or triangular moment distribution is selected for "Applied load type", users must define the "Support type" (for calculation of
C1
and
C2
) and "Load application" (for calculation of
zg
).
The moment factor,
ψ
is only applicable for linear moment distributions, that is bending moment diagrams that are either uniform or have a linear slope. For uniform linear bending moment diagrams, the calculator automatically sets
ψ=1
. For linear bending moment diagrams with a slope,
ψ
must be defined within the range of -1 to 1.
The user can select from the following European & UK steel sections: UB (universal beams), UC (universal columns), IPE (parallel faced flange beams) or HE (wide/very wide flanged beams). The geometric properties of the cross-section are provided as per the standard: BS EN 10365:2017 - Hot rolled steel channels, I and H sections - Dimensions and masses.
Inputs
Section Properties
Section size
:HE 700 A
L
:5.00m
Applied Load Type
Applied load type
:UDL (parabolic BM)
💡Note, the below inputs are applicable based on your selected "Applied load type". Otherwise, they will not affect the calculation.
Selected "Applied load type":
UDL (parabolic BM) or Point load at midspan (triangular BM)
Applicable user input:
Support type
:Pinned/Pinned
Load application
:Section centroid
Selected "Applied load type":
End moments (linear BM)
Applicable user input:
ψ
:-0.268
Outputs
C1 factor
:1.127
C2 factor
:0.454
Mcr
:4,437kN m
Explanation
What is lateral torsional buckling?
Lateral torsional buckling occurs in members in bending. It is where the beam bends in it's minor axis and twists, as this behavior is the least stiff bending failure.
Lateral torsional buckling is particularly relevant in beams that are slender, have a significant length between supports or are not laterally supported along their length. These conditions make the beam more susceptible to twisting and lateral displacement when subjected to bending moments.
This is what lateral torsional buckling looks like:
What is the elastic critical moment?
The critical elastic moment,
Mcr
is the critical bending moment that leads to the onset of elastic lateral torsional buckling (LTB) in a beam. It is analogous to how the Euler buckling concept identifies the critical compression causing a column to succumb to elastic flexural buckling,
Mcr
is a parameter in EC3 and serves as an input into the buckling resistance moment,
Mb,Rd
which is crucial for assessing the capacity of a section in bending.
Mcr
in Eurocode 3
The following code snippets of EC3 show
Mcr
as an input to the factor
χLT
in the design buckling resistance moment,
Mb,Rd
The engineer's role is to design a beam that has an adequate bending strength to resist applied moments without experiencing LTB. This involves selecting a beam size and positioning lateral supports such that the bending stresses are within acceptable limits.
NCCI Parameters and Equations
Below are the parameters and equations as provided in NCCI SN003b, that are used in this calculator.
= length of beam between points of lateral support
k
= effective length factor related to end rotation on plan
kw
= effective length factor related to end warping, unless special provision for warping fixity is made take
kw=1
zg
= distance between the point of load application and the shear centre
In the typical scenario of a normal support conditions,
k
and
kw
are 1. When the bending moment diagram is linear between lateral constraints,
C2=0
. When the load is applied at the shear center,
zg=0
. Under these conditions the equation for
Mcr
simplifies to:
Mcr=C1L2π2EIzIzIw+π2EIzL2GIt
Load application point (
zg
parameter)
The load is generally applied to the top of the section. The parameter
zg
is positive for loads acting towards the shear centre and negative for loads acting away from the shear centre as shown in the figure below.
Point of application of the load as per NCCI Section 2
A beam with load applied to the top of the section will have a lower
Mcr
value then a beam with load applied to the bottom of the section, and hence a lower resistance to lateral torsional buckling.
Applied load type (
C1
and
C2
parameters)
The factors
C1
and
C2
are influenced by the bending moment distribution in the beam and it's support conditions. The types of bending moment distributions are listed below and shown in the image below.
Uniform or linear bending moment, when there is applied end moments only
Parabolic bending moment, when there is an applied uniformly distributed load (UDL)
Triangular bending moment, when there is an applied concentrated load
Types of bending moment distributions in a beam (Source: eurocodeapplied.com)
C1
and
C2
values for the types of moment distributions are:
Uniform or linear bending moment,
C1
is taken from Table 3.1 of NCCI (provided below) and
C2=0
Parabolic bending moment,
C1
and
C2
is taken from Table 3.2 of NCCI (provided below) for both pinned and fixed support conditions
Triangular bending moment,
C1
and
C2
is taken from Table 3.2 of NCCI (provided below) for both pinned and fixed support conditions
Table 3.1 of NCCI
C1 values for beams with a linear moment distribution as per NCCI Section 3.2
Table 3.2 of NCCI
C1 and C2 values for beams with a parabolic or triangular moment distribution as per NCCI Section 3
Ratio of end moments (
ψ
parameter)
The parameter
ψ
is the ratio of applied end moments for beams with a linear bending moment diagram.
M
is the maximum end moment and therefore the range of
ψ
is:
−1≤ψ≤1
If
ψ
is equal to 1, the moment distribution is uniform.