Technical science/2. Mechanics

Dr. Sc. Techn., professor Gots A. N.

Vladimir state University of a name Alexander Grigorievich and Nikolai Grigorievich Stoletovs, Russia

New schematized diagram of limit cycles under the action of normal stresses

Calculation of factors of safety of machine parts under the action of normal stresses in the case of uniaxial stress state and the asymmetric cycle of loading with amplitude σa and mean stress σm is performed on the basis of dependency S. W. Serensen, and R. S. Kinasoshvily [1]:

   ,                                            (1)

where Kσ is the effective stress concentration factor; εσ – scale factor; βσ – coefficient of the surface layer; ψσ – coefficient of influence of cycle asymmetry or coefficient, which characterizes the sensitivity of the material to the asymmetry of the cycle [2] .

The maximum amplitude of the stresses σra for laboratory sample with asymmetric cycle of loading can be expressed by the equation, well the corresponding experimental data in the range of variation of the coefficient of asymmetry

,                                    (2)

where σrm is the current value of the limiting medium stress of cycle.

In computational practice, often use a schematized diagram of the limiting amplitudes Serensen-Kinasoshvily in which the coefficient ψσ equal

,                                 (3)

where σ0 is the fatigue limit of laboratory samples in a pulsating cycle.

Because the value of σ0 in the reference literature is not given, it is recommended to define her by the approximate formulas [3]. For steels in bending and tension-compression  . Upper limits refer to mild steels. It is easy to notice that with this choice of σ0, after substitution in (3) the coefficients ψσ will be constant, independent of the mechanical characteristics of the material.

In [1] for steels calculation ψσ it is proposed that the formula

,                                       (4)

where σv is the tensile strength, MPa.

From (4) it follows that ψσ varies from 0.1 at σv = 400 MPa, while σv = 1500 MPa to 0.32.

The value of ψσ can be determined by constructing the author's proposed new schematized diagram of limit cycles sra = f(srm). To do this, use for limit cycles linear dependence Goodman [4]

,                                        (5)

and parabolic Gerbera [4]

.               (6)

Fig. 1. Chart of the limiting amplitudes for steel 40XH: 1 – direct of Goodman; 2 – Gerber parabola; 3 – marginal direct Serensen-Kinasoshvily(s0 = 1,6s-1); 4 – proposed direct s0 = 1,8s-1; 3’ – the same when s0 = 1,6s-1 4 – proposed direct schematized diagram

In Fig.1 for steel 40XH (with the characteristics of mechanical strength in MPa: tensile strength σv =1000; yield strength σ0,2=800; endurance limit of a symmetric cycle σ-1=460) the diagrams of the limiting amplitudes using the dependences (5) – direct 1 and (6) – curve 2.

For parts made from plastic materials according to (5) and (6) are valid as the threat to them is sra = f(srm) only on a portion of the chart  not only fatigue, but also the transition for the yield strength, which leads to residual deformations that distort the shape and dimensions of the part.

Therefore, the maximum stress cycles must be less not only endurance limit, and yield strength smax  = sa  + sm  < s0,2.

In order to exclude from the chart sra = f(srm) the area where the limiting maximum stress σrmax=sra + srm  > s0,2, take the straight line KL, which cuts off on the cuts the coordinate  OL and OK is equal to the yield strength (steel 40XH s0,2 = 800 MPa, Fig. 1). The equation of a line KL is:

.                                            (7)

Thus, for the parts made of plastic materials chart limit amplitude in the coordinate axes sm-sa is limited by the line 1 and the parabola 2 (Fig. 1) until they intersect at the points C1 and C2 with direct KL, and more – direct C1L or C2L. The coordinates of the points of the broken lines AC1L or AC2L give limit values and depending on the selected function sra = f(srm).

Replace plot charts Goodman and Gerber schematized diagrams. In Fig.1 by equation (2) with (3) built direct limit Serensen-Kinasoshvily 3, assuming ψσ= 0,11) and 3’, ψσ= 0.25 to crossing them with direct KL at the points and respectively. Note that the direct limit  (if taken ) will be above the Gerber parabola, which contradicts the results of studies P. Forrest [4].

For steel 40XH, using (4), find the value of ψσ= 0,22. Limit direct, built according to (4), in this case almost coincides with the straight 3’ (Fig. 1).

Build a schematized diagram using three points σ0,2, σ-1 and the coordinates of the point of intersection C2 () Gerber parabola with a straight KL. Combine in a system of dependency (7) and (8), after the decision of who will receive the coordinates of the point C2 ():

                      (8)

                      .                             (9)

Connecting points A and C2( ), get a new schematized diagram OAC2L (Fig. 1) in which the tangent of the slope of the straight AC2 to x-axis , considering the influence ys is numerically equal to the coefficient  of medium stress (constant component of the cycle) at the limit of endurance:

.      (10)

When calculating the value ys according to the formula (10) are used, only those characteristics of mechanical strength, which are listed in the reference literature.

Formulas (8) and (9) allow us to determine what type of destruction is dangerous for a known working medium sm and the amplitude sa stresses.

If during the calculation details sm/ sa < srm /sra , the duty cycle of stresses is in the field OAC2 (Fig. 1) and calculate the factor of safety should be based on (1). If sm/ sa > srm /sra, the calculation is based on [1-3]:

                                            (11)

The values of the coefficients ψσ and relations limit srm /sra, can be defined by the formulas (9), (10) and (11) for steels, if known mechanical characteristics of the materials.

In our proposed schematized diagram direct limit AC2 is located between the parabola 2 and 1 direct, i.e., it satisfies the experimental data for ductile metals [4, 5].

LITERATURE

1. Kogaev V. P., Makhutov N. A., Gusenkov A. P. Calculations of machine parts and structures for strength and durability: Handbook – M.: Mashinostroenie, 1985. – 224 p.

2. Birger I. A., Shorr B. F., Iosilevich G. B. Calculation of the strength of machine parts. Handbook. – M.: Mashinostroenie, 1993. – 640 p.

3. Handbook on strength of materials // M. N. Rudizin, P. Y. Artemov, M. I. Lyuboshitz.; Under the editorship of M. N. Radizina. – Minsk: Vysheishaya school, 1970. - 630 p.

4. Forrest P. Fatigue of metals. Translation from English. Under the editorship of S. V. Sorensen. – M.: Mashinostroenie, 1968. – 352 p.

5. Collins J. Damage of materials in structures. Analysis, prediction, prevention: Trans. from engl. – M.: Mir, 1984.– 624 p.

6. Gots A. N. The calculations of the strength of engine parts with voltages, variable in time/A. N. Gots – 3-e Izd. – M.: FORUM; infra-m, 2013 – 208 p.http://www.translate.ru/%28%F2%E0%EChttp://www.translate.ru/%28%F2%E0%EC