NEW DATABASE - 350 MILLION DATASHEETS FROM 8500 MANUFACTURERS
NEW DATABASE - 350 MILLION DATASHEETS FROM 8500 MANUFACTURERS
| Catalog Datasheet Results | Type | Document Tags |
| Abstract: International Reliability Physics Symposium 1990, Page 12. [27] W. C. Riordan and R. M. Vasquez "Statistical , on Reliability of Electron Devices, Failure Physics and Analysis 1993. [7] W. Gerling "Modern , ] Accelerated Testing by Nelson. [11] AT&T Reliability Handbook. [12] Statistical Tables by Murdoc and Barnes. , Physics Symposium, 1986, Pages 44�. �� ADI Reliability Handbook [14] J Ferro "An Accelerated , Work." Proceedings 29th I.E.E.E. International Reliability Physics Symposium 1991, Page 1. [22] A. ... | Original |
5 pages, |
symposium gunn diode datasheet ED-36 Betel ED36 kc 2462 datasheet abstract |
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| Abstract: the papers presented at these conferences. At the 1995 IEEE International Physics Symposium held in , Physics and Analysis Germany Oct. 1992 Reliability Yield & Quality, Correlation For A Particular Failure Mechanism 31 st IEEE International Reliability Physics Symposium Atlanta, GA Mar. 1993 , On Thin gate Oxide Quality 32nd IEEE International Reliability Physics Symposium San Jose April , Reliability Physics Symposium Las Vegas Mar 1995 Design Rules For Reliable Surface Micromachined Sensors ... | Original |
3 pages, |
symposium research paper and gate datasheet abstract |
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| Abstract: DesignCon 2009 A New Jitter Classification Method Based on Statistical, Physical, and , statistical distribution and spectral properties. The physical jitter properties are first discussed in terms , conventional statistical deterministic jitter (DJ)- and random jitter (RJ)based jitter separation and , and combined. Finally, the values and advantages of the new physical and statistical combined jitter , , holds six patents, and is awaiting approval on eight others. Dr. Li holds a PhD in physics, an MSE in ... | Original |
15 pages, |
simple F.M. transmitter pioneer pll CP-01052-1 CP-01052-1 abstract |
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| Abstract: Field failure experience Physics of failure method Qualification procedure: Fig. 4 , is then extrapolated to end-use conditions by means of a predetermined statistical model to give an , statistical model equation (2). 2 2TD AF 10 9 FIT (1) For cyclic stress the Coffin , for this graph because the values are not fixed but subject to statistical distribution. Field , subscribe to this method for calculation of failure rate. Physics of failure method: This is relatively a ... | Original |
8 pages, |
IEC60749-5 IEC60068-2-6 IEC60068-2-27 IEC60068-2-14 failure analysis IGBT AN5945-5 LN27638 AN5945-5 abstract |
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| Abstract: hp35s Physics, AP Statistics (a graphing calculator with statistical capabilities is expected), PSAT/NMSQT, SAT , view entries, results, menus and prompts · Simplify physics with 42 built-in physical constants, plus , TestsTM in Math 1 & 2, ACT, PSAT/NMSQT, AP Chemistry/Physics, PLAN, EXPLORE © 2007 Hewlett-Packard ... | Original |
2 pages, |
LCD hp dot scientific calculator CR2032 calculator lcd display battery CR2032 8 digit lcd calculator display lcd scientific calculator display datasheet abstract |
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| Abstract: Field failure experience Physics of failure method Qualification procedure: The principle , is then extrapolated to end-use conditions by means of a predetermined statistical model to give an , statistical model equation (2). 2 2TD AF 10 9 FIT (1) For cyclic stress the Coffin Manson , subscribe to this method for calculation of failure rate. Physics of failure method: This is relatively a , , which is quantified by the physics of failure models for each failure mechanism. Although this method ... | Original |
7 pages, |
MTBF IGBT module IEC60068-2-14 IEC60068-2-27 IEC60068-2-6 IEC60749-5 igbt module testing AN5945-3 igbt qualification circuit IEC60068-2-14 vibration MTBF IGBT fit igbt failure IEC60749 LN26894 AN5945-3 abstract |
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| Abstract: failure per billion hours (109 hours). Both MTBF and are statistical quantities and if the failure , Qualification procedure Theoretical calculation Physics of failure method Field failure experience: This , by means of a predetermined statistical model to give an estimate of the failure rate in the field , conjunction with Chi square statistical model equation (2). E 1 1 V2 AF exp a T T k , program. It used a large statistical sample for a high degree of confidence. Although the devices were ... | Original |
11 pages, |
217F Thyristor missile statistical Physics IEC60068-2-14 IEC60068-2-6 IEC60749-12 IEC60749-34 IEC60749 IEC60749-23 IEC60747-6 IEC60749-25 AN5948-2 LN26862 AN5948-2 abstract |
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| Abstract: Energy Physics, Civilian nuclear applications, harsh environment robotic, etc.) for which the radiation , volume markets (e.g., New equipment for High Energy Physics) have changed the approach. New technologies , Energy Physics The High Energy Physics is probably the most severe environment for electronics. The , , statistical process control, learning curve, etc. Moreover, by using ultimate technology, Atmel offers to , Dual use prod- Specific Design Rules Nuclear Reactor Environment High Energy Physics ... | Original |
8 pages, |
nuclear radiation detector DMILL van allen belt satellite van allen belt metal detector plans datasheet abstract |
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| Abstract: Energy Physics, Civilian nuclear applications, harsh environment robotic, .) for which the radiation , equipment for High Energy Physics ) have changed the approach. New technologies, originally developed to , dominated by neutrons. Tens of MRAD and 1015 n/cm² are frequently required. High Energy Physics The High Energy Physics is probably the most severe environment for electronics. The particle flux , statistical process control, learning curve . Moreover, by using ultimate technology, Atmel offers to ... | Original |
8 pages, |
neutron detector van allen belt satellite DMILL "electromagnetic pulse" metal detector plans datasheet abstract |
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| Abstract: to illustrate this approach [83�]. An IEEE International Reliability Physics Symposium paper , experimental design techniques to verify the impact of statistical process control on the reliability of the , critical statistical process control parameters, and introduced the notion of statistical reliability , enhanced the use of statistical process and reliability control to maintain process reliability as shown , Devices, Failure Physics and Analysis 1993. [7] W. Gerling "Modern Reliability Assurance of Integrated ... | Original |
11 pages, |
statistical process control failure rate TDDB Microtherm datasheet abstract |
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| Over 1.1 million files (1986-2013): html articles, reference designs, gerber files, chemical content, spice models, programs, code, pricing, images, circuits, parametric data, RoHS data, cross references, pcns, military data, and more. Please note that due to their age, these files do not always format correctly in modern browsers. Disclaimer. |
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| not only the average values of required parameters but also their statistical distribution. 1 parameters are not directly measurable and others are not related to the physics of the device but are structure The schematic is shown in figure 3. The statistical data for manufacturing processes and .1.2 Statistical Analysis The statistical input data allows COSMOS to output not only the average value of the required response but also its statistical distribution. The average value is also given divided into www.datasheetarchive.com/files/stmicroelectronics/stonline/books/ascii/docs/3674-v1.htm |
STMicroelectronics | 25/05/2000 | 17.58 Kb | HTM | 3674-v1.htm |
| required parameters but also their statistical distribution. 1. INTRODUCTION The modelling of power related to the physics of the device but are simply fit parameters to model the device as close as is shown in figure 3. The statistical data for manufacturing processes and device design (figure 4 . C oss , C rss , gate-charge, etc.). 3.1.2 Statistical Analysis The statistical input data allows COSMOS to output not only the average value of the required response but also its statistical www.datasheetarchive.com/files/stmicroelectronics/stonline/books/ascii/docs/3674.htm |
STMicroelectronics | 20/10/2000 | 18.15 Kb | HTM | 3674.htm |
| definition through production and release. Ideally you will have a HNC/HND/Degree in Electronics, Physics knowledge of project management, statistical process control, FMEA, design of experiments and problem www.datasheetarchive.com/files/international-rectifier/docs/wcd00001/wcd00116.htm |
International Rectifier | 06/10/1998 | 9.1 Kb | HTM | wcd00116.htm |
| a scalable, physics based Sub-Circuit model1. This model is based on the Philips standard models MM new physics based dynamic electro thermal large signal model for RF LDMOS FETs", IEEE MTT-S 2004 parameters are set to 1. The expected statistical distributions of the spreading of the bond www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLC573_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| is described by a scalable, physics based Sub-Circuit model1. This model is based on the Philips .P.J.G. Versleijen, V.J. Bloem, J.A. van Steenwijk, O.I. Yanson, "A new physics based dynamic electro thermal large reserved. Application note Rev. 01 - 25-09-2008 6 of 10 The expected statistical distributions of the www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLF578_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| transistor die is described by a scalable, physics based Sub-Circuit model1. This model is based on the .P.J.G. Versleijen, V.J. Bloem, J.A. van Steenwijk, O.I. Yanson, "A new physics based dynamic electro thermal large expected statistical distributions of the spreading of the bond-wire inductances and matching capacitances www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLF878_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| is described by a scalable, physics based Sub-Circuit model1. This model is based on the Philips .P.J.G. Versleijen, V.J. Bloem, J.A. van Steenwijk, O.I. Yanson, "A new physics based dynamic electro thermal large .V. 2008. All rights reserved. Application note Rev. 01 - 12-08-2008 6 of 10 The expected statistical www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLF574_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| is described by a scalable, physics based Sub-Circuit model1. This model is based on the Philips Steenwijk, O.I. Yanson, "A new physics based dynamic electro thermal large signal model for RF LDMOS FETs each element2. By default, these parameters are set to 1. The expected statistical distributions of www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLF571_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| , physics based Sub-Circuit model1. This model is based on the Philips standard models MM11 for the with the 1. See: M.P.J.G. Versleijen, V.J. Bloem, J.A. van Steenwijk, O.I. Yanson, "A new physics parameters are set to 1. The expected statistical distributions of the spreading of the bond www.datasheetarchive.com/download/61813360-596980ZC/71691.zip (AN_BLF871_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 23/10/2012 | 57734.64 Kb | ZIP | 71691.zip |
| a scalable, physics based Sub-Circuit model1. This model is based on the Philips standard models MM new physics based dynamic electro thermal large signal model for RF LDMOS FETs", IEEE MTT-S 2004 parameters are set to 1. The expected statistical distributions of the spreading of the bond www.datasheetarchive.com/download/78581398-597038ZC/blf573_ads_model.zip (AN_BLC573_LDMOS_Transistor_Model_REV0p1.pdf) |
NXP | 22/10/2012 | 279.7 Kb | ZIP | blf573_ads_model.zip |