Question 11.2: A long, slender column ABC is pin supported at the ends and ...

A long, slender column ABC is pin supported at the ends and compressed by an axial load P (Fig. 11-15). Lateral support is provided at the midpoint B in the plane of the figure. However, lateral support perpendicular to the plane of the figure is provided only at the ends.
The column is constructed of a standard steel shape (IPN 220) having modulus of elasticity E = 200 GPa and proportional limit \sigma_{p l} = 300 MPa . The total length of the column is L = 8m .
Determine the allowable load P_{\text{allow}}using a factor of safety n = 2.5 with respect to Euler buckling of the column.

11-15
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Because of the manner in which it is supported, this column may buckle in either of the two principal planes of bending. As one possibility, it may buckle in the plane of the figure, in which case the distance between lateral supports is L/2 = 4 and bending occurs about axis 2–2 (see Fig. 11-9c for the mode shape of buckling).

As a second possibility, the column may buckle perpendicular to the plane of the figure with bending about axis 1–1. Because the only lateral support in this direction is at the ends, the distance between lateral supports is L = 8 m (see Fig. 11-9b for the mode shape of buckling ).

Column properties. From Table E-2, Appendix E, we obtain the following moments of inertia and cross-sectional area for an IPN 220 column:

I_{1}=3060 \mathrm{~cm}^{4} \quad I_{2}=162 \mathrm{~cm}^{4} \quad A=39.5 \mathrm{~cm}^{2}

TABLE E-2        
Properties of European Standard Beams                     

Designation Mass
per
meter
Area
of
section
Depth
of
section
Width
of
section
Thickness Strong axis 1-1 Weak axis 2-2
G A h b t_{w} t_{t} I_{1} S_{1} r_{1} I_{2} S_{2} r_{2}
Kg/m {cm}^{2} mm mm mm mm {cm}^{4} {cm}^{3} cm {cm}^{4} {cm}^{3} cm
IPN 550
IPN 500
166
141
212
179
550
500
200
185
19
18
30
27
99180
68740
3610
2750
21.6
19.6
3490
2480
349
268
4.02
3.72
IPN 450
IPN 400
115
92.4
147
118
450
400
170
155
16.2
14.4
24.3
21.6
45850
29210
2040
1460
17.7
15.7
1730
1160
203
149
3.43
3.13
IPN 380
IPN 360
IPN 340
IPN 320
IPN 300
84
76.1
68
61
54.2
107
97
86.7
77.7
69
380
360
340
320
300
149
143
137
131
125
13.7
13
122
11.5
10.8
20.5
19.5
18.3
17.3
16.2
24010
19610
15700
12510
9800
1260
1090
923
782
653
15
14.2
13.5
12.7
11.9
975
818
674
555
451
131
114
98.4
84.7
72.2
3.02
2.9
2.8
2.67
2.56
IPN 280
IPN 260
IPN 240
IPN 220
IPN 200
47.9
41.9
36.2
31.1
26.2
61
53.3
46.1
39.5
33.4
280
260
240
220
200
119
113
106
98
90
10.1
9.4
8.7
8.1
7.5
15.2
14.1
13.1
12.2
11.3
7590
5740
4250
3060
2140
542
442
354
278
214
11.1
10.4
9.59
8.8
8
364
288
221
162
117
61.2
51
41.7
33.1
26
2.45
2.32
2.2
2.02
1.87
IPN 180
IPN 160
IPN 140
IPN 120
IPN 100
21.9
17.9
14.3
11.1
8.34
27.9
22.8
18.3
14.2
10.6
180
160
140
120
100
82
74
66
58
50
6.9
6.3
5.7
5.1
4.5
10.4
9.5
8.6
7.7
6.8
1450
935
573
328
171
161
117
81.9
54.7
34.2
7.2
6.4
5.61
4.81
4.01
81.3
54.7
35.2
21.5
12.2
19.8
14.8
10.7
7.41
4.88
1.71
1.55
1.4
1.23
1.07
IPN 80 5.94 7.58 80 42 3.9 5.9 77.8 19.5 3.2 6.29 3 0.91
Note: Axes 1-1 and 2-2 are principal centroidal axes.

Critical loads. If the column buckles in the plane of the figure, the critical load is

P_{\mathrm{cr}}=\frac{\pi^{2} E I_{2}}{(L / 2)^{2}}=\frac{4 \pi^{2} E I_{2}}{L^{2}}

Substituting numerical values, we obtain

P_{c \mathrm{r}}=\frac{4 \pi^{2} E l_{2}}{L^{2}}=\frac{4 \pi^{2}(200 \mathrm{~GPa})\left(162 \mathrm{~cm}^{4}\right)}{(8 \mathrm{~m})^{2}}=200 \mathrm{~kN}

If the column buckles perpendicular to the plane of the figure, the critical load is

P_{\mathrm{cr}}=\frac{\pi^{2} E I_{1}}{L^{2}}=\frac{\pi^{2}(200 \mathrm{~GPa})\left(3060 \mathrm{~cm}^{4}\right)}{(8 \mathrm{~m})^{2}}=943.8 \mathrm{~kN}

Therefore, the critical load for the column (the smaller of the two preceding values)

P_{\mathrm{cr}}=200 \mathrm{~kN}

and buckling occurs in the plane of the figure.
Critical stresses. Since the calculations for the critical loads are valid only if the material follows Hooke’s law, we need to verify that the critical stresses do not exceed the proportional limit of the material. In the case of the larger critical load, we obtain the following critical stress:

\sigma_{\mathrm{cr}}=\frac{P_{\mathrm{cr}}}{A}=\frac{943.8 \mathrm{~kN}}{39.5 \mathrm{~cm}^{2}}=238.9 \mathrm{~MPa}

Since this stress is less than the proportional limit (\sigma_{p l} = 300 MPa) , both critical-load calculations are satisfactory.
Allowable load. The allowable axial load for the column, based on Euler buckling, is

P_{\text {allow }}=\frac{P_{\mathrm{cr}}}{n}=\frac{200 \mathrm{~kN}}{2.5}=79.9 \mathrm{~kN}

in which n = 2.5 m is the desired factor of safety.

2

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