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Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

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692

COLuMNS

In this case, a relationship can be found between the pinned–pinned column’s maximum

deflection v max , which occurs at x = L/2, and the load P. First,

v

max

⎡ kL kL kL ⎤

= e tan sin + cos − 1

⎣⎢ 2 2 2 ⎦⎥

⎡ 2 2

sin ( kL/2)

cos ( kL/2)

= e⎢

+ − 1⎥

⎣ cos( kL/2)

cos( kL/2)

⎡ 1 ⎤ ⎡ kL ⎤

= e⎢

−1⎥ = e sec −1

⎣cos( kL/2)

⎦ ⎣⎢ 2 ⎦⎥

(b)

Then, since k 2 = P/EI, Equation (b) can be restated in terms of the load P and the flexural

rigidity EI as

v

max =

⎡ ⎛ L P ⎞ ⎤

e⎢sec⎜

⎟ − 1⎥

⎣ ⎝ 2 EI ⎠ ⎦

(c)

Equation (c) indicates that, for a given column in which E, I, and L are fixed and e > 0, the

column exhibits lateral deflection for even small values of the load P. For any value of e,

the quantity

⎛ L P ⎞

sec⎜

⎟ − 1

⎝ 2 EI ⎠

approaches positive or negative infinity as the argument of the function approaches π/2, 3π/2,

5π/2,…, and the deflection v increases without bound, indicating that the critical load corresponds

to one of these angles. If π/2 (the angle that yields the smallest load) is chosen, then

or

from which it follows that

L P π

=

2 EI 2

P

cr

P

EI

π

=

L

2

π EI

= (16.19)

2

L

which is the Euler formula discussed in Section 16.2.

Unlike an Euler column, which deflects laterally only if P equals or exceeds the Euler

buckling load, an eccentrically loaded column deflects laterally for any value of P. To illustrate

this property, the quantities E, I, and L can be eliminated from Equation (b) by

using Equation (16.19) to produce an expression for the maximum lateral column deflection

in terms of P and P cr . From Equation (16.19), let EI = P cr L 2 /π 2 . Substituting this expression

into Equation (b) then gives

v

max

⎡ ⎛ L P ⎞ ⎤ ⎡ ⎛

2

L P π ⎞ ⎤

π P

= e⎢sec⎜

⎟ − 1⎥ = e⎢sec 1 e sec 1

2 EI

2

2

⎣ ⎝ ⎠ ⎦ ⎝ Pcr

L

⎟ − ⎥

⎣⎢

⎠ ⎦⎥ =

⎡ ⎛ ⎞ ⎤

⎢ ⎜ ⎟ − ⎥

⎣⎢

⎝ 2 Pcr

⎠ ⎦⎥

(d)

From this equation, it would appear that the maximum deflection becomes infinite as

P approaches the Euler buckling load P cr ; however, under these conditions, the slope of the

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