The practical formula for the stability analysis
It is comfortable to have one formula under any bar slenderness ratio then two formulas (Euler and Jasinsky) as each of them is good for a certain range of the slenderness ratio. This practical formula being applied widely in the construction design has the form (9.12)
where is the allowable working stress in compression; is the reduction coefficient for the allowable working stress (or a coefficient of buckling). The value depends on the material and the slenderness ratio. Its values are given in tabl. 9.1; A is the bar cross section area. The value can be considered as the allowable stress in the stability analysis, i.e. (9.13)
The allowable working stress has the form:
(9.14)
where is the limit stress taken as the yield stress for plastic materials or the ultimate strength for the brittle ones. The relation between the coefficient the critical stress the limit stress of the safety factor coefficients n and stability can be derived as follows: from which (9.15) Using the formula (9.14) we get
(9.16)
To select the section the formula is led to the following form:
(9.17)
The value has to be set as the slenderness ratio is unknown because the section area A is unknown but the slenderness ratio depends on it. Then one has to determine i min and λ values from tabl. 9.1 It is recommended to take φ 1 = 0.5. And then we find the values A, l min. If we receive a large difference between the values and , the calculation must be repeated setting a new value
and so on as long as the difference between the successive values do not exceed 4-6%. For bars which sections have considerable weakness (for example, from holes) besides the stability design, the strength analysis must be done by the formula (9.18)
where is the working area (net) of the bar section. In the stability design the total section area is taken. In some cases (for example, in the machine-building construction element design) the values of the safety stability coefficients provided for composing the tables of the coefficients are insufficient. In this case the design must be done by using the demanded coefficient and Euler’s or Jasinsky’s formula. It must be done the same in the design of the bar stability from materials which do not have coefficients in the table Tabl. 9.1.
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