# Probabilistic Assessment of Damage from Same Shock Response Spectra due to Variations in Damping

Authors: Arup Maji
Journal: Shock and Vibration
 (2020)

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## Abstract

Interpretation of field data from shock tests and subsequent assessment of product safety margins via laboratory testing are based on the shock response spectra (SRS). The SRS capture how a single degree of freedom (SDOF) structure responds to the shock at differing frequencies and, therefore, no longer contain the duration or other temporal parameters pertaining to the shock. A single duration can often be included in the technical specification or in the recreation of acceleration vs. time history from the specified SRS; however, there is little basis for that beyond technical judgment. The loss of such temporal information can result in the recreated SRS being the same while its effect on a system or component can be different. This paper attempts to quantify this deficiency as well as propose a simple method of capturing damping from shock waves that can allow the original waveform to be more accurately reconstructed from the SRS. In this study the decay rate associated with various frequencies that comprise the overall shock was varied. This variation in the decay rate leads to a variation in the acceleration vs. time history, which can be correlated to a “Damage Index” that captures the fatigue damage imparted to the object under shock. Several waveforms that have the same SRS but varying rates of decay for either high- or low-frequency components of the shock were investigated. The resulting variation in stress cycles and Damage Index is discussed in the context of the lognormal distribution of fatigue failure data. It is proposed that, along with the SRS, the decay rate is also captured to minimize the discrepancy between field data and representative laboratory tests.


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## Body

## 1. Introduction

Mechanical vibration and shock have a detrimental effect on components or systems. Therefore, shock tests are conducted to ensure items can survive the repeated shocks that they are expected to endure during their lifetime. The level of shock to be applied in the shock tests is prescribed in terms of the shock response spectra (SRS). The SRS levels used for testing are typically prescribed in the terms of P99 or P95 levels (for example, P99 implies that the shock applied in the test will exceed 95% of the shock the item may see in its lifetime).An issue that arises with this approach is that SRS are not a unique representation of shock; various shock events can have the same SRS. The different shocks (decaying acceleration vs. time) corresponding to the same SRS will inflict a different amount of damage to the item of interest. In this study, the effect of 4 shocks (Trials 1–4) that have identical SRS was investigated to quantify the consequence in such variations. The 4 shocks were generated by varying the decay rate (damping) of the underlying shock acceleration vs. time.The SRS quantify the input shock, and “damping” relates to the decay rate of the input shock. Damage, on the contrary, is a consequence of the shock applied. The consequence of the shock can be measured in terms of a “Damage Index”. In this paper, a “Damage Index” is quantified in terms of the magnitude and number of stress cycles as per equation (1). Its absolute value is significant only when a specific material/structure is being considered and the stress cycles needed to cause failure are known. In the context of this paper, the absolute value of the “Damage Index” is not significant, and only the relative differences between Trial 1 through Trial 4 are significant. Damping (of the input shock) is constant for each frequency but varies among the 5 frequencies and from Trial 1 to Trial 4.Statistical data are available in the literature on how the Damage Index at failure (# of stress cycles leading to failure) varies among tests. This information can be used to assess how a variation in the number and magnitude of stress cycles relates to the probability of failure. This, in turn, allows the variation in stress cycles from the 4 trials to be related to the consequent variation in the probability of failure. The various sources of data and the analytical methods are presented in the next section.


## 2. Implications of Fatigue Test Data

In this section, test data from several sources in the literature were examined for variation in fatigue damage from test data, as defined by the standard deviation of the log10 (damage).The basic relationship between cyclic stress (ΔS) and number of cycles to failure (N) is provided by Basquin’s power law [1], also referred to as the Miner–Palmgren relation [2]:(1)ΔSβN=C,where the constant C can be thought of as a “Damage Index” or measure of accumulated damage leading to failure. The dimensional units of this parameter C are dependent on those of the underlying parameter (ΔS has units of stress, typically in MPa, and N is unitless) and hence can be converted to other units accordingly. The unitless parameter β is determined from test data using linear regression on a semilog scale (β = 6.66 was used in this paper).Paris and Erdogan [3] provided an analogous expression or slow fatigue crack growth per cycle δa/δN as a function of the stress intensity factor (K) instead of stress and the material constant A replacing C in the Miner–Palmgren relation:(2)δaδN=AΔKm.These relations form the basis for statistical analyses of fatigue data for various material-structural systems [4, 5] and standard practices used in the industry. Equation (1) is also expressed in the following form:(3)logN=1βlogCΔSorlogdamage=logC=logN+βlogΔS.The standard deviations of the quantities are thus related by the following equation:(4)σdamage=σlogN+βσlogΔS.Szala and Szala [6] investigated the fatigue life of D16CzATW aluminum alloy using fatigue test data on structural elements subject to different types of cyclic loads. Using a fatigue model based on equation (1), they arrived at a mean fatigue life parameter Nc from 6 tests. The normalized (to the mean) fatigue life parameter was calculated, and the standard deviation of log(normalized-Nc) was determined to be 10.4% (Table 1).Table 1
Mean number of fatigue life cycles from test data from Szala and Szala [6].
Test #Normalized (Nc)Log(Nc)11.240.09420.75−0.12830.91−0.04340.75−0.12551.080.03461.270.105Mean−0.010St. deviation10.4%Leonetti et al. [7] fit fatigue test data to the Miner–Palmgren cumulative damage law and looked at the deviations for butt weld joints and cover-plated beams of steel for a large number (>500) of tests. Based on the standard deviation σw of log10N, the standard deviation of fatigue damage was determined to be 29% and 19%, respectively, for the butt joint and cover plates tested.Peng et al. [8] investigated fatigue failure under combinations of small and large amplitude cyclic loading with cumulative damage defined as the summation of damage for each type of loading. Damage for each type of load was defined in terms of the Miner–Palmgren relation. The damage for various load combinations was normalized to their corresponding mean values and evaluated using a lognormal distribution, as shown in Table 2, which summarizes the variation in total damage for 3 types of metals. The standard deviation of the lognormal distribution shown in Table 2 was determined to be 14.7%, 12.3%, and 11.4%, respectively.Table 2
Fatigue damage data for various materials by Peng et al. [8].
300CVM steelAluminum-2024-T4230NiCrMoV12 steelNormalized damageLog(damage)Normalized damageLog(damage)Normalized damageLog(damage)0.76−0.1210.85−0.0720.58−0.2380.82−0.0870.78−0.1060.78−0.1071.030.0120.69−0.1640.83−0.0831.220.0860.64−0.1920.80−0.0951.030.0110.66−0.1780.74−0.1331.610.2070.70−0.1531.040.0191.110.0450.84−0.0740.91−0.0411.300.1140.74−0.1330.69−0.1621.100.0430.88−0.0570.86−0.0680.46−0.3411.180.0721.170.0690.51−0.2961.240.0951.270.1050.77−0.1121.250.0981.540.1871.050.0231.390.1441.070.0281.450.1601.400.1471.280.1060.90−0.0461.290.1091.410.1500.76−0.1201.260.1001.080.0351.130.0551.200.0800.95−0.0221.160.0640.85−0.072Standard deviation14.7%12.3%11.4%Shen [9] provided an extensive database of fatigue failure of the aluminum 2023-T4 alloy. Figure 1 shows the data on a log-log scale and the best-fit straight line. Using the inverse of the slope of this line as the measure of β (1/0.11 = 9.1), damage was calculated for each data point. The standard deviation of log(damage) was determined to be 0.27. It can be noted in Figure 1 that the scatter in data is much higher for the low-stress cycles. Therefore, this analysis was repeated using only the data ≥371.7 MPa (logΔS ≥ 2.57), as shown in Figure 2. The slope of the line has changed to 0.18 and β = 5.57. The standard deviation of log(damage) is now only 3.7% due to the lower scatter (note the small stress range for these data). Figure 3 shows how the damage remains constant in spite of the variation in the stress range due to the corresponding changes in the number of cycles to failure.Figure 1
Linear fit to fatigue failure test data (entire stress range).Figure 2
Linear fit to fatigue failure test data (higher stress range).Figure 3
Variation in damage for various stress ranges.Overall, the standard deviation of log(damage) varies from 10% to 30%, and smaller standard deviations are possible when the range of stress cycles is small. Therefore, the analyses in the next section will be based on the assumptions of the standard deviationσ (log10damage) = 10% to 30%. A comprehensive literature survey of fatigue test data is beyond the scope of this paper; the reader can use the analyses presented, henceforth, to assess the consequences for any fatigue test data relevant to their specific application.


## 3. Damage Corresponding to Different Decay Rates for the Same SRS

Shock testing specifications are based on the concept of the shock response spectra (SRS) which no longer contains the time history. The SRS were originally conceived to address the need to convey the effect of earthquake damage to civil infrastructure [10, 11] in a concise manner. The SRS are typically based on the maxi-max absolute acceleration (MMAA) of the response of an SDOF (single degree of freedom) structure to the shock acceleration vs. time. As a result, the SRS do not contain any information on the decay rate of the original wave. Different component frequencies in a shock wave may attenuate at different rates. For instance, the high-frequency component typically attenuates faster; however, the decay at different frequencies is also dependent on through what media or structure the shock wave has been transmitted. Therefore, the issues addressed in this paper pertain to the following.Damage Index (DI) is defined in the context of Miner’s rule for low-cycle fatigue damage as discussed earlier (parameterC in equation (1)). For the same SRS, how is the imparted “Damage Index” (C) affected by the varying decay rate of the different component frequencies? An implicit part of this question is the determination of what causes differences in SRS and DI as the decay rate changes. The value of the material-dependent exponent β was chosen to be 6.66.While this paper studies the influence of damping as an input parameter to shock and consequent damage, damping has also been extensively studied as a consequence of damage. Kouris et al. [12] investigated the variation in modal damping as a measure of structural damage by applying progressively greater vibration load to a building leading to “‘near-collapse damage state.” Variation in damping was proven to be a better measure of structural damage than the shift in natural frequency/modes [13].


### 3.1. Effect of Damping on the SRS

Four different acceleration time-histories with the same SRS were investigated. These acceleration vs. time datax¨t were generated using decayed sines (equation (5)), where ω is the frequency in radians and ξ is damping. The exponential decay parameter α represents the final amplitude/initial amplitude ratio after a certain time period. Five sine waves (at 100, 200, 400, 650, and 950 Hz) were added to create the total acceleration time history. Trial 1 had the amplitude of each of the 5 sine waves (acc 1–5) set to 10. As shown in Table 3, the damping of each frequency ξ was inversely proportional to the frequency as per equation (5). The exponential decay parameter α determines how the sine waves decay as per equation (5). Therefore, since ξω = α was constant for each of the 5 constituent sine waves, each of them decay to the same level at the end of the 0.08 sec duration under consideration. Figure 4 shows 3 of the 5 sine waves each decaying to the same amplitude after 0.08 sec.(5)x¨t=sinωte−ξωt,whereξω=α=Constant Exp Decay.Table 3
Synthesis of four waveforms with the same SRS.
Frequency (Hz)100200400650950Trial 1: proportional damping to get the same decayDamping0.075000.037500.018750.011540.00750Amplitude1010101010Trial 2:X3 damping of Trial 1 at 650 and 950 HzDamping0.0750.03750.018750.034620.0225Amplitude10101013.613.2Trial 3:X4 damping of Trial 1 at 650 and 950 HzDamping0.0750.03750.018750.046160.03Amplitude10101015.414.7Trial 4:X2 damping of Trial 1 at 100 and 200 HzDamping0.150.0750.018750.011540.0075Amplitude1414101010Figure 4
Accelerations at 100, 400, and 950 Hz decaying to the same final amplitude.For Trial 2, the damping of the 2 highest frequencies (650 and 950 Hz) was increased by a factor of 3. As a result, these waves decayed faster (Figure5). However, the amplitude of these two components was increased (Table 3) such that the resulting SRS were identical to that of Trial 1. Figure 5, therefore, shows a higher amplitude for the 950 Hz signal (blue); note that the actual peak is somewhat less than that of the table because of the rapid decay of the high-frequency content.Figure 5
Accelerations at 950 Hz decaying faster than 100 and 400 Hz.For Trial 3, the damping of the 2 highest frequencies (650 and 950 Hz) was increased by a factor of 4 relative to Trial 1. Once again, the amplitude of these two components was increased (Table3) such that the resulting SRS were identical to that of Trial 1. The SRS of Trials 1–3 are shown in Figure 6. The 2 waveforms (Trial 1 and Trial 2) are shown side by side in Figure 7. Due to the increase in the amplitude of the high-frequency component, Trial 2 had a higher maximum acceleration, which contributed to a greater Damage Index as will be discussed next.Figure 6
SRS of waveforms from Trial 1, Trial 2, and Trial 3.Figure 7
Waveforms from Trial 1 vs. Trial 2.
(a)(b)The SRS were computed using the MMAA after the following convolution integral that captures the response of a single degree of freedom (SDOF) spring-mass structurey¨t due to input acceleration x¨t shown in the following equation, where ω is the natural frequency of the SDOF structure and ξ is the damping constant:(6)y¨t=−ω1−ξ2∫0tx¨τe−ξωt−τsinω1−ξ2t−τdτ.Next, using the rain flow count algorithm in Matlab™, the # and amplitude of cycles (N and σ in equation (1)) were determined from the acceleration vs. time such as those shown in Figure 7. The results for all 4 trials are shown in Figure 8. Using these data and equation (1), the Damage Index (DI) was determined to be 2.90 × 1011, 3.39 × 1011, 3.99 × 1011, and 3.24 × 1011 for Trial 1 through Trial 4, respectively. The approximately 17% increase in DI for Trial 2 is due to the higher initial peak in the shock wave leading to more high-stress cycles (50–60); note that Trial 2 has a smaller # of cycles at the stress range of 0–10. The contribution of low-stress cycles to the DI is minimal due to the exponent β = 6.66 in the equation for DI. Likewise, the 38% increase in DI for Trial 3 is due to the high-stress cycle (60–70) which was not present for Trial 1.Figure 8
Stress range (σ) and corresponding cycle count (n) from 4 trials.
(a)(b)(c)(d)For Trial 4, the damping of the two lowest frequencies was increased by a factor of 2 (Table3). Figure 9 shows the resulting shock wave and the rapidly decayed 100 Hz component, which required the amplitude at that frequency to increase (to keep the same SRS). This led to the DI increasing to 3.24 × 1011 (12% higher than that of Trial 1).Figure 9
Trial 4: amplified peak at 100 Hz component and overall signal.
(a)(b)


## 3.1. Effect of Damping on the SRS

Four different acceleration time-histories with the same SRS were investigated. These acceleration vs. time datax¨t were generated using decayed sines (equation (5)), where ω is the frequency in radians and ξ is damping. The exponential decay parameter α represents the final amplitude/initial amplitude ratio after a certain time period. Five sine waves (at 100, 200, 400, 650, and 950 Hz) were added to create the total acceleration time history. Trial 1 had the amplitude of each of the 5 sine waves (acc 1–5) set to 10. As shown in Table 3, the damping of each frequency ξ was inversely proportional to the frequency as per equation (5). The exponential decay parameter α determines how the sine waves decay as per equation (5). Therefore, since ξω = α was constant for each of the 5 constituent sine waves, each of them decay to the same level at the end of the 0.08 sec duration under consideration. Figure 4 shows 3 of the 5 sine waves each decaying to the same amplitude after 0.08 sec.(5)x¨t=sinωte−ξωt,whereξω=α=Constant Exp Decay.Table 3
Synthesis of four waveforms with the same SRS.
Frequency (Hz)100200400650950Trial 1: proportional damping to get the same decayDamping0.075000.037500.018750.011540.00750Amplitude1010101010Trial 2:X3 damping of Trial 1 at 650 and 950 HzDamping0.0750.03750.018750.034620.0225Amplitude10101013.613.2Trial 3:X4 damping of Trial 1 at 650 and 950 HzDamping0.0750.03750.018750.046160.03Amplitude10101015.414.7Trial 4:X2 damping of Trial 1 at 100 and 200 HzDamping0.150.0750.018750.011540.0075Amplitude1414101010Figure 4
Accelerations at 100, 400, and 950 Hz decaying to the same final amplitude.For Trial 2, the damping of the 2 highest frequencies (650 and 950 Hz) was increased by a factor of 3. As a result, these waves decayed faster (Figure5). However, the amplitude of these two components was increased (Table 3) such that the resulting SRS were identical to that of Trial 1. Figure 5, therefore, shows a higher amplitude for the 950 Hz signal (blue); note that the actual peak is somewhat less than that of the table because of the rapid decay of the high-frequency content.Figure 5
Accelerations at 950 Hz decaying faster than 100 and 400 Hz.For Trial 3, the damping of the 2 highest frequencies (650 and 950 Hz) was increased by a factor of 4 relative to Trial 1. Once again, the amplitude of these two components was increased (Table3) such that the resulting SRS were identical to that of Trial 1. The SRS of Trials 1–3 are shown in Figure 6. The 2 waveforms (Trial 1 and Trial 2) are shown side by side in Figure 7. Due to the increase in the amplitude of the high-frequency component, Trial 2 had a higher maximum acceleration, which contributed to a greater Damage Index as will be discussed next.Figure 6
SRS of waveforms from Trial 1, Trial 2, and Trial 3.Figure 7
Waveforms from Trial 1 vs. Trial 2.
(a)(b)The SRS were computed using the MMAA after the following convolution integral that captures the response of a single degree of freedom (SDOF) spring-mass structurey¨t due to input acceleration x¨t shown in the following equation, where ω is the natural frequency of the SDOF structure and ξ is the damping constant:(6)y¨t=−ω1−ξ2∫0tx¨τe−ξωt−τsinω1−ξ2t−τdτ.Next, using the rain flow count algorithm in Matlab™, the # and amplitude of cycles (N and σ in equation (1)) were determined from the acceleration vs. time such as those shown in Figure 7. The results for all 4 trials are shown in Figure 8. Using these data and equation (1), the Damage Index (DI) was determined to be 2.90 × 1011, 3.39 × 1011, 3.99 × 1011, and 3.24 × 1011 for Trial 1 through Trial 4, respectively. The approximately 17% increase in DI for Trial 2 is due to the higher initial peak in the shock wave leading to more high-stress cycles (50–60); note that Trial 2 has a smaller # of cycles at the stress range of 0–10. The contribution of low-stress cycles to the DI is minimal due to the exponent β = 6.66 in the equation for DI. Likewise, the 38% increase in DI for Trial 3 is due to the high-stress cycle (60–70) which was not present for Trial 1.Figure 8
Stress range (σ) and corresponding cycle count (n) from 4 trials.
(a)(b)(c)(d)For Trial 4, the damping of the two lowest frequencies was increased by a factor of 2 (Table3). Figure 9 shows the resulting shock wave and the rapidly decayed 100 Hz component, which required the amplitude at that frequency to increase (to keep the same SRS). This led to the DI increasing to 3.24 × 1011 (12% higher than that of Trial 1).Figure 9
Trial 4: amplified peak at 100 Hz component and overall signal.
(a)(b)


## 4. Consequence of Damage Variations in Test Reliability Levels

### 4.1. Probability of Exceeding Damage Threshold

The previous sections showed the following:(i)
Different acceleration vs. time data from the same SRS can lead to differences in the “Damage Index.”(ii)
Variations in materials and structures result in a variation in the “Damage Index” at failure (for static loads, this is analogous to failure of any material at different stress levels).This section provides a discussion on how a variation in the fatigue-based “Damage Index” in the previous section affects the overall assessment of the probability failure. We will use the concept of P99 level as the probability of failure less than 1%. Conducting a shock test to P99 level implies that the test exceeds the real-life environment 99% of the time. So, when there is a 20% variation in the Damage Index from the different recreations of acceleration vs. time from the same SRS (based on the range of 12% to 38% variations in DI discussed earlier), how does that affect the probability of failure? This issue will be investigated in the next section considering the effect of 20% variation in the fatigue damage imparted during a test.First, lognormal statistics is discussed briefly in terms of natural log(basee), defined as y = ln(x), where x is lognormal if y follows the normal distribution. Closed-form equations provided below provide some valuable insights that can then be extended to the definition of lognormal statistics y = log10(x). If the mean and standard deviation of y is μ and σ, the mean and standard deviation of x (=ey) is μ′ and σ'. Equations for probability distribution function (PDF) and cumulative PDF (CDF) are also provided as follows:(7)mean ofx:μ′=eμ+σ2/2,standard deviation ofx:σ′=eσ2−1e2μ+σ2,(8)coefficient of variation inx:σ′μ′=eσ2−1,(9)probability distribution functionPDF:PDFx=1xσ2πe−lnx−μ2/2σ2,(10)cumulative PDFCDF:CDFx=12+12erflnx−μ2σ.As per equation (8), the coefficient of variation in x is independent of the mean μ of the underlying data y. Consequently, a change in μ only leads to a stretching of the CDF, which is also evident from equation (10) since a change in μ is offset by a corresponding change in ln(x) = y. Figure 10 shows this for a simulation using 106 randomly generated values of y (using MatLab™ randn) from which x is computed (=ey). The PDF and CDF (vs. x) are shown for σ = 0.25 and μ = 0, and 1. The larger μ (=1) shows a larger spread in the lognormal data as well as a shift in the mean value to the right. The CDF shows that the 50% values for both equal x = eμ (=1.0 and 2.72, respectively; red lines). If the value of x is increased by 20% to 1.2 and 3.26 (red dotted lines), the corresponding CDFs remain the same (0.77). Hence, a proportionate change in x leads to the same change in CDF. This will also be observed when the definition is changed to log10(x) = y.Figure 10
PDF and CDF with changing mean (0 and 1) and same standard deviation.
(a)(b)In order to investigate how the Matlab™ simulation of statistical distribution converges with an increase in the number of data (varied from 103 to 107), the theoretical values of the mean and standard deviation of xμ′ and σ′ were obtained using equation (7) and normally distributed y (with μ = 0 and σ = 1). These were then compared with the mean and standard deviation of x based on the Matlab™ random number generator to create y. Figure 11 shows how this ratio converges to 1.0 for 107 data points. Henceforth, simulations were conducted with 107 data points.Figure 11
Convergence of mean and standard deviation to theoretical values.


### 4.2. Simulation of the Effect of a 20% Change inC on Probability of Failure

The simulation involved the following steps.The PDF and CDF of 107 data points were generated using μ = 0 and varying σ (0.1 to 0.3).Using the CRF, the value ofx corresponding to a 1% probability of failure (1% probability of the material’s fatigue life being below that of the fatigue damage corresponding to the SRS) was determined. Note that this corresponds to the P99 level (99% probability of the material’s fatigue life being higher than that of the fatigue damage corresponding to the SRS).For a 20% increase inx (i.e., 1.2x), the probability of failure was determined. For instance, if the new probability of failure corresponding to 1.2x is 5%, it means that the 20% increase in x resulted in the P99 changing to P95. Figure 12 shows the probability of failure for different combinations of μ and σ (10 simulations for each). Note that an increase in σ from 0.25 to 1.0 reduces the probability of failure. This is because with increased scatter in the fatigue strength of the material, a 20% change in the damage imparted is less consequential. Note that the change in the mean value is inconsequential due to reasons discussed in the previous section (coefficient of variation is independent of the mean).Figure 12
Probability of failure (damage exceeding material capacity).Therefore, the remaining simulations (10 runs each) were done withμ = 0 and varying σ from 0.1 to 0.3; results are shown in Figure 13. As the scatter in the material’s fatigue strength decreases (decreasing σ), the consequence of the 20% change in x is progressively more consequential. For σ = 0.1, P99 changes to worse than P94, while for σ = 0.3, P99 changes only to P98.Figure 13
Probability of failure (damage exceeding material capacity).
(a)(b)


## 4.1. Probability of Exceeding Damage Threshold

The previous sections showed the following:(i)
Different acceleration vs. time data from the same SRS can lead to differences in the “Damage Index.”(ii)
Variations in materials and structures result in a variation in the “Damage Index” at failure (for static loads, this is analogous to failure of any material at different stress levels).This section provides a discussion on how a variation in the fatigue-based “Damage Index” in the previous section affects the overall assessment of the probability failure. We will use the concept of P99 level as the probability of failure less than 1%. Conducting a shock test to P99 level implies that the test exceeds the real-life environment 99% of the time. So, when there is a 20% variation in the Damage Index from the different recreations of acceleration vs. time from the same SRS (based on the range of 12% to 38% variations in DI discussed earlier), how does that affect the probability of failure? This issue will be investigated in the next section considering the effect of 20% variation in the fatigue damage imparted during a test.First, lognormal statistics is discussed briefly in terms of natural log(basee), defined as y = ln(x), where x is lognormal if y follows the normal distribution. Closed-form equations provided below provide some valuable insights that can then be extended to the definition of lognormal statistics y = log10(x). If the mean and standard deviation of y is μ and σ, the mean and standard deviation of x (=ey) is μ′ and σ'. Equations for probability distribution function (PDF) and cumulative PDF (CDF) are also provided as follows:(7)mean ofx:μ′=eμ+σ2/2,standard deviation ofx:σ′=eσ2−1e2μ+σ2,(8)coefficient of variation inx:σ′μ′=eσ2−1,(9)probability distribution functionPDF:PDFx=1xσ2πe−lnx−μ2/2σ2,(10)cumulative PDFCDF:CDFx=12+12erflnx−μ2σ.As per equation (8), the coefficient of variation in x is independent of the mean μ of the underlying data y. Consequently, a change in μ only leads to a stretching of the CDF, which is also evident from equation (10) since a change in μ is offset by a corresponding change in ln(x) = y. Figure 10 shows this for a simulation using 106 randomly generated values of y (using MatLab™ randn) from which x is computed (=ey). The PDF and CDF (vs. x) are shown for σ = 0.25 and μ = 0, and 1. The larger μ (=1) shows a larger spread in the lognormal data as well as a shift in the mean value to the right. The CDF shows that the 50% values for both equal x = eμ (=1.0 and 2.72, respectively; red lines). If the value of x is increased by 20% to 1.2 and 3.26 (red dotted lines), the corresponding CDFs remain the same (0.77). Hence, a proportionate change in x leads to the same change in CDF. This will also be observed when the definition is changed to log10(x) = y.Figure 10
PDF and CDF with changing mean (0 and 1) and same standard deviation.
(a)(b)In order to investigate how the Matlab™ simulation of statistical distribution converges with an increase in the number of data (varied from 103 to 107), the theoretical values of the mean and standard deviation of xμ′ and σ′ were obtained using equation (7) and normally distributed y (with μ = 0 and σ = 1). These were then compared with the mean and standard deviation of x based on the Matlab™ random number generator to create y. Figure 11 shows how this ratio converges to 1.0 for 107 data points. Henceforth, simulations were conducted with 107 data points.Figure 11
Convergence of mean and standard deviation to theoretical values.


## 4.2. Simulation of the Effect of a 20% Change inC on Probability of Failure

The simulation involved the following steps.The PDF and CDF of 107 data points were generated using μ = 0 and varying σ (0.1 to 0.3).Using the CRF, the value ofx corresponding to a 1% probability of failure (1% probability of the material’s fatigue life being below that of the fatigue damage corresponding to the SRS) was determined. Note that this corresponds to the P99 level (99% probability of the material’s fatigue life being higher than that of the fatigue damage corresponding to the SRS).For a 20% increase inx (i.e., 1.2x), the probability of failure was determined. For instance, if the new probability of failure corresponding to 1.2x is 5%, it means that the 20% increase in x resulted in the P99 changing to P95. Figure 12 shows the probability of failure for different combinations of μ and σ (10 simulations for each). Note that an increase in σ from 0.25 to 1.0 reduces the probability of failure. This is because with increased scatter in the fatigue strength of the material, a 20% change in the damage imparted is less consequential. Note that the change in the mean value is inconsequential due to reasons discussed in the previous section (coefficient of variation is independent of the mean).Figure 12
Probability of failure (damage exceeding material capacity).Therefore, the remaining simulations (10 runs each) were done withμ = 0 and varying σ from 0.1 to 0.3; results are shown in Figure 13. As the scatter in the material’s fatigue strength decreases (decreasing σ), the consequence of the 20% change in x is progressively more consequential. For σ = 0.1, P99 changes to worse than P94, while for σ = 0.3, P99 changes only to P98.Figure 13
Probability of failure (damage exceeding material capacity).
(a)(b)


## 5. Capturing Rate of Decay of Shock

A method is suggested for capturing the decay rate associated with the different component frequencies. This would allow the original waveform to be replicated more accurately. The SRS at each frequency are a function of both the amplitude and damping associated with that frequency. The same is also true for the FFT of a decaying shock wave. As the shock wave decays with time, the amplitude of the FFT decreases; this can be utilized to capture the damping at each frequency.The input signal at each frequencyω is a decaying sine wave of amplitude A enveloped by an exponential decay. The decaying envelope I of each sine wave can be characterized by the damping parameter ξ according to the following equation:(11)I=Ae−ξωt.Integrating equation (11) from the start to time T, one obtains the mean value of the envelope over the time period [0, T], as shown in equation (2). This mean value represents the amplitude of the Fourier transform of the decaying sine wave over this interval (P/A < 1 because of the decay):(12)P=AT∫0Te−ξωtdt=AξωT1−e−ξωT.Equation (12) has two unknowns: amplitude A and damping ξ of the sine wave and, therefore, needs to be evaluated at two different points. Therefore, by conducting a fast Fourier transform (FFT) of the shock wave at two different time intervals [0, T1] and [0, T2), one can obtain two corresponding values of the mean amplitude of the sine waves P1 and P2. Based on equation (2), equation (3) represents these two specific situations. The unknown damping ξ is then evaluated by numerically solving the following equation:(13)1−e−ξωT11−e−ξωT2=P1T1P2T2.Figures14 and 15 show the FFT of the input signal from Trial 1 and Trial 2, respectively, from 0 to 0.08 sec and from 0 to 0.04 sec, respectively. The lower numbers for 0–0.08 sec are due to the greater decay over the full duration. The peak values in Figure 14 are the same for both durations due to proportional damping and constant amplitude of each sine wave. The peak values in Figure 15 are lower for the 2 high frequencies due to the larger damping; the values for the full duration are even lower. The damping values determined using the methodology described above are shown in Table 4; both the actual and the estimated damping values are provided for comparison. The method captures the damping values very accurately for all 4 trials. The only time the estimated damping is slightly different (shaded orange) is when the duration of 0.04 sec does not include sufficient waves to be statistically representative.Figure 14
FFT of Trial 1 signal (full and 1/2 duration).Figure 15
FFT of Trial 2 signal (full and 1/2 duration).Table 4
Comparison of actual decay rates with those computed from FFT.
Frequencies100 Hz200 Hz400 Hz650 Hz950 HzTrial 1 actual0.075000.037500.018750.011540.00750Trial 1 from FFT0.074990.037500.018750.011540.00750Trial 2 actual0.0750.03750.018750.034620.0225Trial 2 from FFT0.07560.03760.01880.03460.0222Trial 3 actual0.0750.03750.018750.046160.03Trial 3 from FFT0.07570.03770.01890.04960.0280Trial 4 actual0.150.0750.018750.011540.0075Trial 4 from FFT0.14330.07410.01880.01150.0075


## 6. Conclusions

(i)
Assuming longer duration equates to a smaller damping for the same SRS. This leads to a lower Damage Index (DI) and unconservative test (high-stress cycles are eliminated).(ii)
An increase in damping leads to an increase in DI (approximately 17% and 38% for Trial 2 and Trial 3 compared to Trial 1) due to an increase in peak acceleration values. A few high cycles can dominate the Damage Index due to the exponentβ.(iii)
An increase in DI can significantly impact the estimated reliability of the test for realistic lognormal statistics of fatigue test data observed in tests of different materials. A perceived P99 test can become a P95 test or worse.(iv)
The influence of an increase in DI on reliability is less if the underlying data correlating DI to failure have a larger scatter (higherσ). Large variation in material property makes the accuracy of the test specification less consequential. The analysis process presented in this paper provides a methodology to evaluate the appropriate level of rigor and accuracy for shock test specification.(v)
The coefficient of variation in a lognormal distribution is independent of the mean of the underlying normal distribution. This implies that the mean fatigue damageμ is of no consequence to the issue (changes in the PXX level) discussed in this paper.(vi)
Using the Fourier transform of shock signals over two different durations, it is possible to compute the damping associated with the frequencies of interest with high accuracy. This would allow original waveforms to be captured more accurately vs. just the SRS.



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*Source: 8832815-2020-11-28.xml*