ESD ‐ Electrostatic Discharge

ESD ‐ Electrostatic Discharge

ESD ‐ Electrostatic Discharge EPOW6860 –Project RPI 12/14‐2007 Martin Rodgaard What is ESD? • A charged body, which gets discharged • Arcs at high voltages • Triboelectrification – Friction between two different materials, at least one insulator • Properties of ESD – 100 to 35000 voltages – Up to 1000µ Jules of energy – 3000 ‐ 4000V to se, feel or hear it Why is ESD of concern? • Potential damage of semiconductive devices – The high voltages makes the layers or isolation between the layers breakdown – The energy is allocated faster than the material can dissipate it, and can make it melt ESD ‐ Human Body Model(HBM) • Charged human body • Modeled as a capacitor and a series resistor • Values specified in ESD standards – 100pF body capacitance – 1500Ω body resistance – 4000V – 0.4µC or 800µJ of energy ESD ‐ Machine Model(MM) • Charged machine body – Production machine, typically made of metal – Therefore no series resistance • Modeled as a capacitor and series inductor • Values specified in ESD standards – 200pF body capacitance – 750nH series inductance – 400V ESD ‐ Transmission Line Pulsing(TLP) • Charged transmission line • Typical values for testing – Grate Immunity to purposes parasitic components – 50Ω coaxial cable – And therefore a good tool – 90 ‐ 100 nF/m for ESD testing – 10m generating a pulse of • Basic circuit 100ns – Diode clamps any negative reflections, so the pulse doesn’t bounce back again – High quality switch – 50Ω coaxial cable – Charged trough 10MΩ resistor TLP ‐ Basic principle • Coaxial cable • Reflections TLP ‐ Wave forms dd2 t = 0 standing wave Open V0 Z0 ZDUT Circuit V0/2 t = T /2 wave reaches DUT Wave 2 Open V Z Z reflected by a 0 0 DUT Circuit factor of 1, du V0/2 to the open circuit t = T wave reflection reaches coaxial cable again 2 Wave Open V0 Z0 ZDUT Circuit reflected by a factor of V0/2 ‐0.333, du to the ZDUT TLP ‐ Waveforms dd2 t = T1/2 half of the wave has left coaxial cable V0 Z0 ZDUT V0/2 t = T1/2 + T2/2 half of the wave has passed DUT V0 Z0 ZDUT V0/ 2 t = T1 wave has left coaxial cable No reflection V0 Z0 ZDUT of wave, du to V /2 the 50Ω 0 termination 50Ω TLP ‐ How to use this tool? • Mapping the I‐V characteristics – Trough a step increment of the voltage • Finding the Secondary breakdown point(It2) – Where the semiconductor gets permanently damaged TLP, I‐V characteristics and ESD • Linear connection between It2 and HBM ESD voltage level – The higher It2, the higher ESD robustness – So by finding It2, you get a wary good idea of a components ESD robustness ESD protection • ESD controlled workspace • ESD protection circuits on – Reducing the potential ESD chip build up – Simplest form is clamp – ESD packaging diodes, trying to direct the – ESD grounded workspace current away – Clean room(Controlled – Digital circuits is easier to humidity and particles) protect, compared to a sensitive amplifier input.

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