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1 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU
Beam – Column Strength
- Second order effect ( P - D)
Effect of axial force on members having deformations due to
transversal or lateral loading
If the member is braced at ends;
Mnt = is the primary moment due to
transverse loads
d co = deformation due to transverse load
d c = deformation of member due to
transverse loading and axial load
M u = Mnt + Pu . d c
= B1 . Mnt
Where, B1 is a moment magnification factor for a braced member
If the member is unbraced ;
M lt = is the primary moment resulted from sway
D = lateral deflection due to sway
M u = M lt + P . D
= B2 . M lt
Where, B2 is a moment magnification factor for a unbraced member
Therefore for a general member, the final moment taking into
consideration second order effect will be in the form
M u = B1 . Mnt + B2 . M lt
Pu Pu
dcodc
Deflection after P was applied
Deflection before P was applied
dco
w u
Pu
L
Pu
M nt = wL2
/8
Primary Moment Mnt, If P = 0
PuD
Pu
M u
Secondary moment
for braced case
Secondary moment
for unbraced case
2 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU
Where, B1 = Cm ³ 1.0
1 - ( Pu / Pe1)
C m : factor accounts for type of loading and member – end moments
P e1 : Euler buckling load of the member = p2
E I / (KL)2
where, I & L for the axis of bending and (K) for a braced member
For beam-column not subjected to transverse loads
Cm = 0.60 – 0.4 M1
M2
Where;
M1: is the absolute value of smaller moment at
end
M2 : is the absolute value of larger moment at
end
and M1/M2 = - ve for single curvature
= + ve for double curvature
For beam-column subjected to transverse loads
Cm is given as in the shown table
3 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU
Where, B2 = 1 ³ 1.0
1 - ∑ Pu
∑ Pe2
Strength Equations for Beam – Column
1) when Pu ³ 0.20
f Pn
Pu + 8 Mux + Muy £ 1.0
f Pn 9 f Mnx f Mny
2) when Pu < 0.20
f Pn
Pu + Mux + Muy £ 1.0
2 f Pn f Mnx f Mny
where;
f Pn : Column design strength (obtained from column strength)
f Mnx : Beam design strength about x-x axis (obtained from beam strength)
f Mny: Beam design strength about y-y axis (obtained from beam strength)
Pu : Ultimate column load (obtained from factored loads)
Mux : Ultimate bending moment about x-x axis
(obtained from factored loads with the second order effects)
Muy : Ultimate bending moment about y-y axis
(obtained from factored loads with the second order effects)
∑ Pu = Pu1 + Pu2 + Pu3
Where, ∑ Pu is the summation of all ultimate
loads of columns in a story of frame
And, ∑ Pe2 is the summation of Euler buckling
load of all columns in the frame,
where Pe2 = p2
E I / (KL)2
where, I & L for the axis of bending and (K)
for a unbraced member

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18-Beam Column Strength (Steel Structural Design & Prof. Shehab Mourad)

  • 1. 1 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU Beam – Column Strength - Second order effect ( P - D) Effect of axial force on members having deformations due to transversal or lateral loading If the member is braced at ends; Mnt = is the primary moment due to transverse loads d co = deformation due to transverse load d c = deformation of member due to transverse loading and axial load M u = Mnt + Pu . d c = B1 . Mnt Where, B1 is a moment magnification factor for a braced member If the member is unbraced ; M lt = is the primary moment resulted from sway D = lateral deflection due to sway M u = M lt + P . D = B2 . M lt Where, B2 is a moment magnification factor for a unbraced member Therefore for a general member, the final moment taking into consideration second order effect will be in the form M u = B1 . Mnt + B2 . M lt Pu Pu dcodc Deflection after P was applied Deflection before P was applied dco w u Pu L Pu M nt = wL2 /8 Primary Moment Mnt, If P = 0 PuD Pu M u Secondary moment for braced case Secondary moment for unbraced case
  • 2. 2 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU Where, B1 = Cm ³ 1.0 1 - ( Pu / Pe1) C m : factor accounts for type of loading and member – end moments P e1 : Euler buckling load of the member = p2 E I / (KL)2 where, I & L for the axis of bending and (K) for a braced member For beam-column not subjected to transverse loads Cm = 0.60 – 0.4 M1 M2 Where; M1: is the absolute value of smaller moment at end M2 : is the absolute value of larger moment at end and M1/M2 = - ve for single curvature = + ve for double curvature For beam-column subjected to transverse loads Cm is given as in the shown table
  • 3. 3 Prepared by Prof. Shehab Mourad – Department of Civil Eng. - KSU Where, B2 = 1 ³ 1.0 1 - ∑ Pu ∑ Pe2 Strength Equations for Beam – Column 1) when Pu ³ 0.20 f Pn Pu + 8 Mux + Muy £ 1.0 f Pn 9 f Mnx f Mny 2) when Pu < 0.20 f Pn Pu + Mux + Muy £ 1.0 2 f Pn f Mnx f Mny where; f Pn : Column design strength (obtained from column strength) f Mnx : Beam design strength about x-x axis (obtained from beam strength) f Mny: Beam design strength about y-y axis (obtained from beam strength) Pu : Ultimate column load (obtained from factored loads) Mux : Ultimate bending moment about x-x axis (obtained from factored loads with the second order effects) Muy : Ultimate bending moment about y-y axis (obtained from factored loads with the second order effects) ∑ Pu = Pu1 + Pu2 + Pu3 Where, ∑ Pu is the summation of all ultimate loads of columns in a story of frame And, ∑ Pe2 is the summation of Euler buckling load of all columns in the frame, where Pe2 = p2 E I / (KL)2 where, I & L for the axis of bending and (K) for a unbraced member
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