Skip to main content

Ramp-to-Failure Testing

  • Chapter
  • First Online:
Reliability Physics and Engineering
  • 2053 Accesses

Abstract

Engineers are constantly confronted with time issues. Applying a constant stress and waiting for failure can be very time-consuming. Thus, it is only natural to ask the question—does a rapid time-zero test exist that can be used on a routine sampling basis to monitor the reliability of the materials/devices? The answer to this question is often yes and it is called the ramp-to-failure test. While the test is destructive in nature (one has to sacrifice materials/devices), it is generally much more rapid than conventional constant-stress time-to-failure tests. The relative quickness of the test also enables the gathering of more data and thus the gathering of better statistics.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 89.00
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Hardcover Book
USD 119.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    One should always question the existence of a yield stress ξyield. Some materials have a yield stress, some do not. Even if a material has a reported yield point, a slight crack/defect existing in the material may have an adverse impact on the yield point. The stress riser at the crack-tip/defect may produce a local stress in the material well above the yield stress. Degradation would now be expected even though the average stress may be below ξyield.

  2. 2.

    Generally, the slower the ramp rate, the closer the ramp test results will match actual constant-stress time-to-failure results.

  3. 3.

    Reminder—any cum fraction F can be used to determine β provided that the corresponding ξbd (F%) is also used. If one chooses to use F = 0.1, then β = 2.25/{γ [ξbd(63 %) - ξbd(10 %)]}.

  4. 4.

    If one uses F = 0.1 then β = 2.25/{(n + 1)ln[ξbd(63%)/ξbd(10%)]}.

Bibliography

  • Anolick, E. and G. Nelson: Low-Field Time-Dependent Dielectric Breakdown, IEEE International Reliability Symposium Proceedings, 8 (1979).

    Google Scholar 

  • Berman, A.: Time-Zero Dielectric Breakdown by a Ramp Method, IEEE International Reliability Symposium Proceedings, 204 (1981).

    Google Scholar 

  • McPherson, J.: Stress-Dependent Activation Energy, IEEE International Reliability Symposium Proceedings, 12 (1986).

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Problems

Problems

  1. 1.

    Capacitor dielectrics were randomly selected and ramp-to-breakdown tested at 105 °C, using a linear ramp rate of R = dE/dt = 0.5 MV/cm/s. During ramp-to-breakdown testing, it was determined that the breakdown distribution could be approximated by a normal distribution with: (Ebd)50 = 12 MV/cm and σ = 1.0 MV/cm. Determine the expected time-to-failure for 1 % of the capacitors at an operational field of 5 MV/cm at 105 °C. Assume an exponential acceleration factor with γ = 4.0 cm/MV.

    Answer: TF(1 %) = 2.1 years

  2. 2.

    Turbine blades were randomly selected and ramped-to-rupture at 700 °C using a tensile stress with a linear ramp rate of R = dσstress/dt = 5 MPa/min. During ramp-to-rupture testing, it was determined that the rupture distribution could be approximated by a normal distribution with: (σrupture)50 = 250 MPa with a standard deviation of σ = 25MPa. Determine the expected time-to-failure for 1 % of the turbine blades at an operational tensile stress of 15 MPa at 700 °C. Assume a power-law acceleration factor with n = 4.0 and (because of small cracks) no yield point.

    Answer: TF(1 %) = 0.4 years

  3. 3.

    Analyze Problem 1 except this time, assume a power-law acceleration with n = 40.

Answer: TF(1 %) = 4,297 years

  1. 4.

    Analyze Problem 2, except this time assume an exponential acceleration with γ = 0.06/MPa.

Answer: TF(1 %) = 0.3 years

  1. 5.

    Steel pipes were randomly selected for pressurizing-to-rupture testing. Using a linear ramp rate of R = dP/dt = 5 kpsi/min, the rupture data tended to obey a Weibull distribution with (Prupture)63 = 200 kpsi and a Weibull slope of β = 10. Determine the expected time-to-failure for 1 % of the pipes at an operational pressure of 5 kpsi. Assume that the stress in the cylindrical pipes is directly proportional to the pressure and assume a power-law acceleration factor with an exponent of n = 4 and (because of small cracks) no yield point.

Answer: TF(1 %) = 3.9 years

  1. 6.

    Suspension cables were randomly selected for tensile stressing-to-rupture testing. Using a linear ramp rate of R = dσTensile/dt = 4 kpsi/min, the rupture data tended to obey a Weibull distribution with (σrupture)63 = 250 kpsi and a Weibull slope of β = 12. Determine the expected time-to-failure for 1 % of the cables at an operational pressure of 2 kpsi. Assume a power-law acceleration factor with an exponent of n = 4 and (because of small defects) no yield point.

Answer: TF(1 %) = 854 years

  1. 7.

    With no yield point, Eq. (11.16) reduces to:

    $$ \mathrm{TF}\left(F\%\right)=\frac{1}{n+1}\left[\frac{\xi_{\mathrm{op}}}{R}\right]{\left[\frac{\xi_{\mathrm{bd}}\left(F\%\right)}{\xi_{\mathrm{op}}}\right]}^{n+1}, $$

    which is valid when the stress ξ is linearly ramped at a constant rate R (R = dξ/dt = constant) until failure occurs. Show that, if the stress is proportional to the power-law of some other parameter S,

    $$ \xi ={C}_o{S}^m, $$

    then the time-to-failure equation becomes:

    $$ \mathrm{TF}\left(F\%\right)=\frac{1}{n+1}\left[\frac{S_{\mathrm{op}}^m}{R_1}\right]{\left[\frac{S_{\mathrm{bd}}\left(F\%\right)}{S_{\mathrm{op}}}\right]}^{m\left(n+1\right)}, $$

    where the ramp rate R1 is given by:

    $$ {R}_1={mS}^{m-1}\left(\frac{\mathrm{d}S}{\mathrm{d}t}\right)=\mathrm{constant}. $$
  2. 8.

    Using the results from Problem 7, metal storm shutters with small cracks were randomly selected for storm testing. The shutters were tested in a wind tunnel by ramping the wind speed S until the shutters failed. The stress σ in the shutters, due to the wind, is proportional to the square of the wind speed: σ = C0S2. Using a constant ramp rate of R1 = 2S(dS/dt) = 10 (mph)2/min, the failure data tended to obey a Weibull distribution with (S)63 = 100 mph and a Weibull slope of β = 10. Determine the expected time-to-failure for 1 % of the shutters with a nominal constant wind speed of 25 mph. Assume a power-law acceleration factor of at least n = 6, and because of the small cracks, no yield point.

Answer: TF(1 %) = 7.2 years

Rights and permissions

Reprints and permissions

Copyright information

© 2019 Springer Nature Switzerland AG

About this chapter

Check for updates. Verify currency and authenticity via CrossMark

Cite this chapter

McPherson, J.W. (2019). Ramp-to-Failure Testing. In: Reliability Physics and Engineering. Springer, Cham. https://doi.org/10.1007/978-3-319-93683-3_11

Download citation

  • DOI: https://doi.org/10.1007/978-3-319-93683-3_11

  • Published:

  • Publisher Name: Springer, Cham

  • Print ISBN: 978-3-319-93682-6

  • Online ISBN: 978-3-319-93683-3

  • eBook Packages: EngineeringEngineering (R0)

Publish with us

Policies and ethics