Application nr. 3 (Ultimate Limit State) Resistance of member cross-section
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1 Application nr. 3 (Ultimate Limit State) Resistance of member cross-section
2 1)Resistance of member crosssection in tension Examples of members in tension: - Diagonal of a truss-girder - Bottom chord of a truss girder - Element of an X diagonal
3 Application: design of member in tension with bolted end connections Initial data: Design value of the tension axial load: N Ed = dan = N HEA profile required Bolted end connection = two bolt holes of 14 mm diameter in each flange (bolts M12) S235 Steel with f y = 2350 dan/cm 2
4 Equation used for design: The design value of the tension force N Ed at each cross section shall satisfy: Where: N t,rd = design tension resistance
5 First step: sizing of the profile Previous formula used as an equation of equilibrium: In which: N Ed = N t,rd N t, Rd Areq f y Areq f y N Ed M0 = 1,0 M 0 M 0
6 Calculation of the required area (A req ) for the HEA tension member: Areq Areq 24,0 cm 1,0 The actual area of the HEA profile in tension is chosen from HEA profile tables and shall be: A act A req 2 From profile table: HE120A profile with A = A act =25,3 cm 2 > A req
7 Step two: Checking of the member Performed using the relation: Where: N Ed = dan N t, Rd min N pl, Rd ; Nu, Rd
8 N pl,rd = design plastic resistance of the gross cross-section (without bolt holes) Aact f y 25, N pl, Rd ,0 M 0 dan
9 N u,rd = the design ultimate resistance at the net cross-section (end section with bolt holes) N u, Rd 0,9 A net M 2 f u Where: f u = 3400 dan/cm 2 for S235 steel, and M2 = 1,25
10 Bolted end connection of the member
11 Cross-section of the chosen profile with fastener (bolt) holes
12 Calculation of the net area (A net ) = gross area minus holes for bolts The net cross-section area at holes for fasteners: A net = A act n f x d x t f = 25,3 4 x 1,4 x 0,8 = 20,82 cm 2 n f = number of fasteners per cross-section = 4 fasteners (bolts) in this case Evidently, A net < A act
13 Consequently: 0,9 20, u ,25 N, Rd dan Finally: Nt, Rd min N pl, Rd dan; Nu, Rd dan Result: N t,rd = dan
14 Member checking: N N Ed t, Rd ,106 1,0 NOT OK!! A bad choice was made for the HEA profile from the profile table (the area of the chosen profile is too small!). A larger profile should be chosen!
15 Cross section of the NEW chosen profile with fastener holes:
16 Geometric characteristics and resistances for HE140A A act = 31,4 cm 2 A net = 31,4-4 x 1,4 x 0,85 = 26,64 cm 2 N N pl, Rd u, Rd 31, dan 1,0 0,9 26, ,25 dan N ; N dan Nt, Rd min pl, Rd u, Rd 65215
17 Tension member final checking: N Ed ,86 1,0 N t, Rd Member profile HE140A OK!
18 2) Resistance of member crosssection in pure bending Object of the application: simply supported beam under uniformly distributed load (q) OBSERVATION: Mid-span cross-section (section 1-1) is submitted to maximum bending moment (M max ) and no shear force (V=0) The maximum shear force appears on the support (V max ) where the bending moment is null (M=0).
19 Static scheme of the beam:
20 Step1: Sizing of the beam cross-section under pure bending (section 1-1) INITIAL DATA: IPE profile required (other profiles also possible!) Value of uniformly distributed load q=800 dan/m Value of the span: L=12,0 m Steel grade: S235 fy=2350 dan/cm 2
21 Formula to check member resistance in bending: Where: 2 beam q L ,0 M Ed M max danm dancm
22 Sizing procedure: Equation of equilibrium used for sizing: M Ed = M c,rd In case of class 1 or 2 cross sections for bending (as the IPE profiles usually are) member resistance in bending becomes: M c, Rd M pl, Rd W pl M f 0 y Where M0 =1,0 and W pl = plastic modulus of beam cross-section
23 Consequently: req Wpl f y req M max M 0 M max Wpl M 0 f y And: W req pl , ,8 cm Required value! 2350 The actual value of section plastic modulus is further on chosen from the IPE profile tables.
24 For IPE 300 in the table we have: W act pl W table,4 cm 3 req 612, 8 pl. y pl 628 W cm 3 OBSERVATION: The chosen cross-section in the table is of class 1 under pure bending (see last column of the table) which confirms the employed formula for sizing.
25 STEP 2: Checking of member crosssection under pure bending Checking performed in section (1-1) of the beam Checking formula:
26 In previous formula: M M Ed c, Rd M W max pl dancm f M 0 y 628, ,0 dancm And consequently: Profile OK! 0,976 1,0
27 3) Checking of the beam cross-section under pure shear in section (2-2): Checking formula to EN : The design value of the shear force V Ed at each cross section shall satisfy: Where V c,rd is the design shear resistance
28 In previous formula: V V Ed c, RD q L Vmax V pl, Rd dan In absence of the torsion, the design plastic shear resistance V pl,rd is given by the formula: V pl, Rd A v f M 0 y 3 Where A v is the shear area
29 Calculation of the shear area value A v In case of I sections (i.e. IPE!) taken from the profile table, the shear area may be calculated using: A v =A-2 b t f +(t w +2r)t f
30 Geometry of chosen profile crosssection (IPE 300):
31 For IPE 300 we obtain from the profile table: A = 53,8 cm 2 (gross cross-section) r = 15 mm = 1,5 cm (inner radius of profile) Consequently: A v = 53,8-2 15,0 1,07+(0,71+2 1,5) 1,07 =25,67 cm 2
32 Cross-section checking in shear: 25, V pl, Rd ,0 3 dan Checking of the member under pure shear: V V Ed pl, Rd ,137 1,0
33 OBSERVATIONS: The value 0,137 obtained for the ratio shows a small influence of the shear force on profile cross-section Pure bending or pure shear are rather rare practical cases. The most often in practice we have combined bending and shear (see next example)
34 4)Member resistance under combined bending and shear According to code provisions, where the shear force is present simultaneously with a bending moment, allowance shall be made for its effect on the moment resistance
35 Actually, shear force presence may diminish the moment resistance: a) Where the shear force is less than half the plastic shear resistance, its effect on the moment resistance may be neglected. This is equivalent with the following relation: V V Ed pl, Rd 0,5 If upper relation is satisfied, we can neglect the effect of the shear force on the moment resistance
36 b) Where the shear force is larger than half of the plastic shear resistance, or: V V Ed pl, Rd 0,5 the design value of the moment resistance will be diminished by using a reduced strength value: f * y 1 f y
37 In the previous: 2V V Ed pl, Rd 1 2 Consequently, the checking formula in bending becomes: M M Ed c, Rd 1,0 Where: M c, Rd W pl M 0 f * y
38 PRACTICAL EXAMPLE: Cantilever with length= 1,0 m loaded with a concentrated force P at its end Value of the concentrated force P=30000 dan = N IPE profile required for cantilever beam S235 steel grade f y =2350 dan/cm 2
39 STATIC SCHEME AND DIAGRAMS: M max =P L=30000 danm V max =V Ed =30000 dan
40 OBSERVATION: In section (1-1) on the diagram, the maximum value of the bending moment appears together with the shear force (typical to cantilever structures)
41 Step 1: Sizing of the cantilever crosssection in bending Equilibrium equation for sizing: M Ed M max M c, Rd M max W req pl M 0 f y req Wpl 2350 req Wpl 1276,6 cm 1,0 3
42 From the profile table, for IPE 400 we obtain: W act pl W 1307 pl, y cm 3 W req pl
43 Step 2: Checking of the shear force influence V V Ed pl, Rd dan A M v 0 f y 3
44 Geometry of the cross section and geometric characteristics: A=84,5 cm 2 (gross area for IPE 400) A v =A-2 b t f +(tw+2r)t f = = 84, ,35+(0,86+2 2,1) 1,35 =42,73 cm 2
45 Influence of shear force: V V V pl, Rd Ed pl, Rd 42, , ,517 0, dan CONSEQUENCE: Allowance shall be made for the effect of shear force on the moment resistance
46 Calculation of the diminishing factor: V 2 V Ed pl, Rd , , 0012 Calculation of the diminished strength: f * y ( 1 ) f (1 0,0012) dan / cm y 2
47 Calculation of the diminished moment resistance: Wpl f y M c, Rd ,0 M 0 * dancm Checking of the cross-section in bending using the diminished moment resistance: M M Ed c, Rd ,978 1,0 Cross-section OK!
48 OBSERVATION: As evident for the present example, generally the influence of the shear force on the moment resistance is small or to neglect. Most often, in practical cases, in structures working predominant in bending, shear force influence is neglected, according to code conditions.
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