Uneingeschränkter Zugang

Description of Residual Stress Distribution in the Surface Layer After Heat Treatment and Shot Peening


Zitieren

INTRODUCTION

Dynamic surface shot peening is a continuous process of changing the state of the surface layer consisting of plastic deformation and other processes accompanying this phenomenon, the most important of which are phase transformations. Shot peening is characterised by the formation of compressive residual stresses. The quantities determining the state of compressive stresses are: the value of maximum stresses, the depth of their deposition and the distribution in the hardened surface layer. Research on the shot peening process is relatively more widely and more often used for the selection and optimisation of technological parameters and for forecasting the obtained states of stresses and deformation.

An X-ray diffractometer of the PSF-3M type from the Rigaku Company (Japan) was used to measure stresses on the surface of the samples, using a chromium lamp, using the sin2(ψ) method. The 40 × 40 mm amples, having a hardness of 30–50 HRC, were made of C45 steel. Four types of shot were used to harden the surface layer of the samples: cast steel shot SW170 with a diameter of 0.4 mm and SW330 with a diameter of 0.8 m and a hardness of 470 HV; and steel shot StD-03 with a diameter of 0.4 mm and StD-06 with a diameter of 0.6 mm and a hardness of 640 HV. The shot peening time of the sample was 120sec. The air pressure during peening was 0.45MPa. The depth of the hardened layer was in the order of 0.8 mm. The subsequent layers of the samples with the thickness of 0.04–0.06 mm were removed by an electrochemical method. The number of removed layers was in the range of 10–12. For the analytical description of the measurements of the residual stress distribution tests after heat treatment and shot peening, the multiple step regression program REGSTEP.EXE1 was used (using the results the work of Mońka and Janowski [1]). The independent variables in the stress tests were: the depth of the hardened layer deposition d, the hardness of the HRC sample and the type of shot marked with successive natural numbers N (1, 2, 3, 4). Residual stresses σ MPa measured by X-ray diffraction were the dependent variable.

The test results (d, HRC, N, σ) were entered into the stepwise multiple regression program REGSTEP.EXE. In total, 128 experiments were carried out as part of the present study. The studies in the factor space (d ε <0.0–0.8> mm, HRC ε <25–50>, N ε <1, 2, 3, 4>) were not performed according to the rules of the planned experiment [9], but were random. The residual stress distribution function σ, derived from the REGSTEP.EXE program, is a function of three second-degree independent variables with interactions. The obtained function σ is used to obtain the tabular distribution of stresses into the surface layer using the FUNVAL3.EXE2 program. The REGPOLY.EXE3 polynomial regression program was used for analytical recording of the tabular distribution of residual stresses. The EXCEL Microsoft Office 2000 program was used to graphically present the distribution of residual stresses in the form of a polynomial.

TEST METHOD OF RESIDUAL STRESS DISTRIBUTION AFTER HEAT TREATMENT AND SHOT PEENING
X-ray diffractometer

The PSF-3M X-ray diffractometer was used to study the distribution of residual stresses in the surface layer with a thickness of 0.8 mm [2], [,3],[12].

A test sample with dimensions 40 mm × 40 mm is placed on the base of the instrument. The measurement zone on the sample is located in the central part of the sample. The diffractometer is equipped with two movable arms: one arm with a chromium X-ray lamp is used to set the angle of incidence ψ of the beam of X-ray waves on the surface of the sample, and the other arm with a transducer is used to process the reflected beam of X-ray waves, bent on the steel crystal lattice.

The X-ray method of measuring residual stresses is used for metals with a crystalline structure. Residual stresses are introduced into the surface layer of the object by heat treatment and shot peening, which causes displacements in the crystal lattice of the metal.

The stream of X-rays, after being reflected from the displaced crystal lattices, undergoes diffraction and is recorded in the transducer of the diffractometer [3], [12]. The image of the stream of X-ray waves after diffraction is shown in Fig. 1 [3]. For the subsequent angles of incidence ψ of the stream of X-ray waves on the surface of the object, the parameter 2Θ of the top of the diffraction profile is recorded. The deformation of the crystallographic lattice in the metal after heat treatment and shot peening, recorded during the measurement with a diffractometer, is calculated from the following relationships:

Figure 1.

Profiles of diffraction lines obtained at different angles of incidence ψ of the beam of X-ray waves: (A) horizontal axis – angle 2Θ; and (b) vertical axis – intensity of X-ray diffraction.

bragg’s formula [3], [11], given by the following expression:

nλ=2dhklsinΘ

where λ indicates the X-ray wave length (Ao), dhkl the distance between the planes of the crystal lattice of the metal and Θ the angle of incidence of the X-ray beam; and

Hooke’s law relating the deformations ε to a plane state of stresses σ, as follows:

εx=εy=vσyE

where E indicates Young’s modulus for the material (in megapascals) and ν the Poisson’s ratio for the material.

From the quoted relationships in Eqs (1) and (2), the dependence for the calculation of residual stresses in the X-ray method using the sin2 ψ method was derived in the following formula:

σΘ=E1+υm

where m indicates the angular coefficient of a straight line approximating a set of points with the coordinates (sin2 ψ, 2Θ) obtained from the measurements using the X-ray diffractometer.

An example of a test protocol [1] of the measurement of residual stresses using the X-ray diffractometer with an approximation line in coordinates (sin2 ψ, 2Θ) is shown in Fig. 2.

Figure 2.

Report on the measurement of residual stresses using the X-ray method, using the PSWF-3M device from the Rigaku Company: Young’s modulus E = 210,000.0 MPa and Poisson’s ratio ν = 0.280.

The printout (Fig. 2) shows:

the value of residual stresses σΘ = –35,270 Mpa for the material with the following properties:

E = 210,000 MPa – Young’s modulus, and

v = 0.280 – Poisson’s ratio;

as well as,

the approximation line in the coordinates: (sin2 ψ, 2Θ), on which the slope factor m is read (Eq. (3)).

Station for electrochemical removal of material layers

In order to obtain the results of measuring residual stresses in the surface layer as a function of the distance d mm from the shot peened surface, a station for removing material layers using the electrochemical method was developed [1], [4]. The adopted parameters of the electrochemical process allowed for the removal of a layer with a thickness of 0.04–0.06 mm in one etching cycle. Ten to twelve cycles of layer removal were performed. Measurements of residual stresses σ were carried out using the X-ray diffraction method on the successive obtained surfaces. The distance between the successive layers was determined by using as a basis an average of the measurements of sample thickness obtained following the etching cycle.

Research materials

The tests of the shot peening process were carried out on samples that were heat treated (hardened and tempered at different temperatures to obtain different values of HRC hardness) and subjected to the pneumatic shot peening process [1]. The samples were divided into six groups as a function of hardness (HRC):

(1) HRC samples ε <25, 30>, (2) HRC samples ε <30, 35>, (3) HRC samples ε <35, 40>, (4) HRC samples ε <40, 45>, (5) HRC samples ε <45, 50> and (6) HRC samples ε (<50).

The samples were subjected to pneumatic shot peening with the following parameters:

four types of shot, marked with the numbers of the N set (1, 2, 3, 4):

1 – SW170 cast steel shot, granulation 0.4 mm, hardness 470 HV,

2 – SW330 cast steel shot, granulation 0.8 mm, hardness 470 HV,

2 – StD-03 steel shot, granulation 0.4 mm, hardness 640 HV, and

2 – Std-06 steel shot, granulation 0.6 mm, hardness 640 HV;

constant air pressure p = 0.45 MPa,

shot peening time t = 120 s,

100% shot peened surface coverage, and

the sample was rotating.

The shot peening process [8] was performed using the PEEN-IMP device, a patented station (patent PL204718), shown in Fig. 3.

Figure 3.

PEEN-IMP device for pneumatic peening (patent PL204718).

Test results

The test results are summarised in Table 1. A total of 128 experiments were carried out. The independent variables are:

Measurements of stresses σ MPa as a function of distance d mm from the surface.

LP Distance from the surface d mm Hardness HRC Steel shotN 1,2,3,4 Stresses σ MPa
1 0.000 35 1 −506.37
2 0.079 35 1 −465.59
3 0.127 35 1 −390.06
4 0.194 35 1 −397.08
5 0.241 35 1 −244.17
6 0.299 35 1 −209.32
7 0.399 35 1 −232.61
8 0.456 35 1 −172.24
25 0.000 30 2 −448.40
26 0.046 30 2 −540.25
27 0.106 30 2 −571.50
28 0.150 30 2 −547.69
29 0.210 30 2 −527.38
30 0.258 30 2 −514.13
31 0.315 30 2 −427.26
32 0.340 30 2 −354.94
33 0.396 30 2 −305.50
70 0.000 45 3 −682.34
71 0.051 45 3 −602.13
72 0.111 45 3 −615.84
73 0.191 45 3 −552.10
74 0.206 45 3 −395.75
75 0.227 45 3 −259.79
76 0.340 45 3 −249.39
77 0.393 45 3 −293.09
78 0.419 45 3 −195.22
120 0.000 50 4 −643.16
121 0.116 50 4 −737.91
122 0.166 50 4 −745.57
123 0.220 50 4 −509.45
124 0.284 50 4 −394.01
125 0.347 50 4 −432.17
126 0.401 50 4 −321.01
127 0.462 50 4 −254.92
128 0.565 50 4 −261.30

where 0.000 indicates the free surface of the sample.

deposition depth of residual stresses x1 ε <0. ÷ 0.8>,

material hardness x2 ε <25 ÷ 50>, and

the type of shot used marked x3 ε <1, 2, 3, 4>.

The dependent variable is the residual stress σ MPa.

The selected test measurements of stresses for the shot N = 1, 2, 3, 4 are summarised in Table 1.

The meddle in the stresses measured on the surface of the samples after heat treatment were:

hardness in the range of 25–30 HRC, stresses – б = –22 MPa;

hardness in the range of 35–40 HRC, stresses – б = –28 MPa; and

hardness in the range of 45–50 HRC, stresses – б = –145 MPa.

The test results (d, HRC, N, σ) (Table 1) were entered into the REGSTEP.EXE stepwise multiple regression program. The program creates the σ MPa second-degree polynomial function of three independent variables (layer depth d, material hardness HRC and shot type N).

RESIDUAL STRESS FUNCTIONS OF THREE VARIABLES IN A MULTIPLE REGRESSION PROGRAM

The REGSTEP.EXE stepwise multiple regression program makes it possible to create many regression functions:

linear,

linear exponentials with the e base,

second-degree non-linear, where the number of independent variables is one to four, and

the listed functions may have variables written in natural or logarithm form.

The form of the regression function is related to the number of experiments entered into the REGSTEP.EXE program. For three independent variables with interactions, the minimum number of experiments entered into the program is 10 [9]. The second-degree regression function created by the program for three independent variables with interactions is as follows:

y=c0+c1x1+c2x2+c3x3+c5x1x2+c6x1x3+c7x2x3++c8x12+c9x22+c10x32

where c0, c1, c2, c3, c4, c5, c6, c7, c8, c9 and c10 are coefficients calculated by the program.

The c4 coefficient determines the y independent variable, has the value c4 = 1 and is not printed by the program.

After entering the data (Table 1) into the REGSTEP.EXE program, the coefficients of the regression function (Table 2) and their statistical evaluation were obtained using the Student’s t-test (T-VALUE). Regression coefficients are written in exponential format (E).

Coefficients of the regression function calculated by the program for the results of measurements.

Variable number Regression coefficient Std. Error of reg. coeff. Computed T-value
(c1) 1 −0.845537E+02 303.47275 −0.279
(c7) 7 −0.865059E+01 1.82461 −4.741
(c6) 6 0.259431E+02 52.86755 0.491
(c2) 2 −0.109254E+03 26.07856 −4.189
(c10) 10 0.798438E+02 14.47331 5.517
(c9) 9 0.160997E+01 0.35632 4.518
(c3) 3 −0.114981E+03 60.96822 −1.886
(c5) 5 0.138582e+02 7.15698 1.936
(c8) 8 0.493962E+03 288.88644 1.710
(c0) 0.168799E+04

For example, in Table 3, the results of the last (ninth) step of the statistical evaluation of the obtained regression function are presented.

Statistical evaluation of the obtained regression function using the statistical parameters R2 (the square of the multiple correlation coefficient) and F (Snedecor’s test).

STEP 9
VARIABLE ENTERED..... 8
(FORCED VARIABLE)
SUM OF SQUARES REDUCED IN THIS STEP.... 18743.844
PROPORTION REDUCED IN THIS STEP........ 0.006
CUMULATIVE SUM OF SQUARES REDUCED...... 2162765.250
CUMULATIVE PROPORTION REDUCED.......... 0.741 OF 2919265.000
FOR 9 VARIABLES ENTERED
MULTIPLE CORRELATION COEFFICIENT... 0.861
(ADJUSTED FOR D.F.)........... 0.851
SQUARE MULTIPLE CORRELATION COEFFICIENT ⊠ 0.741
F-VALUE FOR ANALYSIS OF VARIANCE... 37.483
STANDARD ERROR OF ESTIMATE......... 80.069
(ADJUSTED FOR D.F.)........... 82.716

The REGSTEP.EXE program is based on IBM subprograms [7]. The more important components’in Table 3 have the following equivalents:

SQUARE MULTIPLE CORRELATION COEFFICIENT = 0.741 (R2 = 0.741 – multiple correlation coefficient)

F-VALUE FOR ANALYSIS OF VARIANCE... 37.483 (F Snedecor’s test = 37.483).

T-VALUE – Student’s t-test for regression function coefficients marked: 1, 2, 3, 5, 6, 7, 8, 9, 10

REGRESSION COEFFICIENT – coefficients of the regression function (1, 2, 3, 5, 6, 7, 8, 9, 10)

The regression function has the computational form:

y=0.168799E+04+0.845537E+02x1+0.109254E+03x2+0.114981E+03x3+0.138582e+02x1x2+0.259431E+02x1x3+0.865059E+01x2x3++0.493962E+03x12+0.160997E+01x22+0.798438E+02x32}

The functional form in Eq. (5) allows the calculation of the values of residual stresses in the factor space determined for the values of the variables:

x1(depthd<0.00.8>mmx2(hardnessHRC)<2550>x3(shotN)<1,2,3,4> }

PROGRAM FOR CALCULATING THE TABULAR DISTRIBUTION OF RESIDUAL STRESSES

The polynomial regression function in Eq. (5) makes it possible to calculate the value of residual stresses into the material σ for the assumed parameters of the factor space in Eq. (6) [5], [10], [11]. For practical purposes, the universal FUNVAL3.EXE program was developed, which, for the assumed values of the coefficients of the regression function and the values of three independent variables (x1, x2, x3), calculates the value of the function in Eq. (5).

Table 4 presents the results of the calculations employed for ascertaining the tabular distribution of residual stresses as a function of every 0.10-mm change in the X1 depth extending into the surface layer.

Values of residual stresses σ as a function of changing the X1 depth extending into the surface layer calculated by the FUNVAL3.EXE program.

Type of function - NATURAL -N-
Values of Bi coefficients in the calculated function
B0= 0.1688E+04, B1= −0.8455E+02, B2= −0.1093E+03,
B3= −0.1150E+03
B12= 0.1386E+02, B13= 0.2594E+02, B23= −0.8651E+01,
B11= 0.4940E+03, B22= 0.1610E+01, B33= 0.7984E+02
NUMBER OF POINTS N = 8
Values of X1, X2, X3 variables at set points
X1 X2 X3
0.000 35.0000 1.0000
0.1000 35.0000 1.0000
0.2000 35.0000 1.0000
0.3000 35.0000 1.0000
0.4000 35.0000 1.0000
0.5000 35.0000 1.0000
0.6000 35.0000 1.0000
0.7000 35.0000 1.0000
0.8000 35.0000 1.0000
Xi depth and Yi function values at set points
No. Xi Yi
1 0.000 −501.1677
2 0.1000 −454.0123
3 0.2000 −396.5508
4 0.3000 −329.2101
5 0.4000 −251.9901
6 0.5000 −164.8909
7 0.6000 −67.9124
8 0.7000 38.9453
9 0.8000 155.6822
ANALYTICAL RECORD OF RESIDUAL STRESS DISTRIBUTION

The distribution of residual stresses shown in the tabular form (Table 4) is additionally presented in the analytical notation. The polynomial regression program REGPOLY.EXE developed on IBM subprograms was used to record the analytical tabular distribution of residual stresses (Table 4) [7]. The program for the tabular stress distribution generates successive polynomial regression functions of one variable, until the moment when the next added monomial does not improve the accuracy of the calculation of the value of the entire polynomial.

As a result of the calculations of the REGPOLY.EXE program, the second-degree polynomial describing the distribution of residual stresses in the surface layer was obtained. The second-degree function takes the following form:

y=a0+a1x+a2x2

The constants in the polynomial in Eq. (7) have the following values:

a0=0.50159×103,a1=0.42643×103and a2=0.49396×103.

The notation of the residual stress distribution function is as follows:

σ=0.50159103+0.42643103x+0.49396103x2[MPa]

The EXCEL Microsoft Office 2000 program was used to obtain a graphic form of the tabular distribution of residual stresses (Table 4). The stress distribution diagram is shown in Fig 4.

Figure 4:

Graph of residual stress distribution in the sample after shot peening:

sample NR50 (HRC, 35 MPa), shot N = 1,

curve 1 – measured distribution of residual stresses, to a depth of 0.5 mm,

curve 2 – distribution of residual stresses created by REGSTEP.EXE, represented by the equation: y = 493,96x2 + 426,43x_501,59.

Curve 1 (Fig. 4) presents the values of the residual stresses σ MPa measured by the sin2 Θ method using a diffractometer. Curve 2 represents the average value obtained by the REGSTEP.EXE stepwise multiple regression program. The presented curve 2 with the fixed parameters of the shot peening process allows an estimation of the distribution of residual stresses in the hardened surface layer.

SUMMARY AND CONCLUSIONS

A total of 128 experiments involving the measurement of residual stresses performed on the C45 steel samples after heat treatment and shot peening [8] were used to determine the form of the regression function of three independent variables (depth extending into the material, hardness of the C45 steel (HRC) and shot in the shot peening process). The REGSTEP.EXE stepwise multiple regression program was used. The test samples were shot peened on both sides in a device for pneumatic shot peening [1]. An X-ray diffractometer was used to measure the stresses. The successive layers of material 0.04–0.06 mm thick were removed from the samples by electrochemical etching. The FUNVAL3.EXE function value program was used to obtain a tabular distribution of residual stresses into the material. The REGPOLY.EXE polynomial regression program was used to record the analytical distribution of residual stresses into the material. The results of the obtained calculations satisfactorily reproduce distributions of stresses in the surface layer, which is confirmed by the following statistical parameters: R2 (squared multiple correlation coefficient), Fisher’s Snedecor test and Student’s t-tests for regression function coefficients. The obtained regression function allows for the initial determination of shot peening parameters, and is recommended for obtaining the value of residual stresses in the surface layer.

The number of laborious experiments needed for determining the regression function of three independent variables can be reduced by applying the rules of the planned experiment [9].

eISSN:
2545-2835
Sprache:
Englisch
Zeitrahmen der Veröffentlichung:
4 Hefte pro Jahr
Fachgebiete der Zeitschrift:
Technik, Einführungen und Gesamtdarstellungen, andere, Geowissenschaften, Materialwissenschaft, Physik