Reliability is not a number on a datasheet. It is a probability curve derived from accelerated stress tests that try to kill the device as fast as possible so you do not have to wait ten years to find out if it works. When you qualify a discrete semiconductor — a MOSFET, a diode, a transistor — you are not checking if it turns on. You are checking if it will still turn on after ten thousand thermal shocks, a hundred thousand power cycles, and five years of humidity soaking.
The methods used to judge this reliability are standardized, but the interpretation is where engineering judgment matters. A test result that looks like a pass to one engineer is a ticking time bomb to another. Here is how to read the data and separate real reliability from marketing fluff.
The most common reliability test for discrete packages is temperature cycling. You dip the device from -55°C to +175°C, hold it at each extreme, and repeat. The goal is to fatigue the solder joints and the wire bonds until they crack.
The industry standard is JESD22-A104. The typical qualification requires 1000 cycles for commercial grade and 3000 cycles for automotive grade. But the number of cycles is meaningless without the dwell time and the ramp rate. A fast ramp rate of 10°C per second creates different stress than a slow ramp of 2°C per second. Fast ramps induce thermal shock, which cracks brittle materials like ceramic or glass passivation. Slow ramps induce creep, which deforms soft materials like solder.
The data is plotted on a Coffin-Manson graph, which relates the number of cycles to failure (Nf) against the plastic strain range (Δε). If the data points fall on a straight line with a slope between -1.5 and -2.0, the failure mechanism is fatigue, and you can extrapolate the life to field conditions using the Arrhenius equation. If the slope is flat or erratic, the failure is not fatigue — it is a random defect like a void or a contaminant. Do not extrapolate random defects. They do not follow physics.
Temperature cycling tells you about mechanical fatigue. HAST tells you about corrosion and moisture ingress. The device is cooked in a pressure cooker at 130°C and 85 percent relative humidity with a bias voltage applied.
The bias is the critical part. You are not just soaking the part; you are electrochemically migrating metal ions from the lead frame to the die. If the mold compound has micro-cracks, moisture gets in, the bias voltage drives the ions, and you get dendritic growth that shorts the device.
A standard HAST duration is 96 hours or 168 hours. For automotive applications, 1000 hours is common. The failure criterion is usually a shift in leakage current or a drop in breakdown voltage. If the leakage current increases by more than one order of magnitude, the insulation is compromised. Do not rely on visual inspection after HAST. The damage is internal. You need electrical parametric testing at every interval.
If you want to test the package seal without the electrical stress, run an Unbiased HAST (UHAST). No voltage is applied. The only failure mechanism is moisture expansion causing "popcorn" cracking of the mold compound.
This is vital for plastic packages with large die sizes. If the moisture content inside the mold exceeds the solubility limit during reflow, the water turns to steam, the internal pressure spikes, and the package cracks. UHAST at 130°C for 96 hours is the standard check. If the package survives without cracking or delaminating, the moisture barrier is sufficient.
Chamber temperature cycling heats the whole board. Power cycling heats only the die. This is a massive difference. In power cycling, the junction temperature swings from 25°C to 150°C in seconds. The solder joint sees a massive shear strain because the silicon die expands much more than the copper lead frame.
The test standard is JESD22-A104 or JESD22-A107. The cycle profile is critical. You need a fast ramp-up (less than 10 seconds) and a controlled cool-down. The number of cycles to failure (Nf) is usually much lower than temperature cycling — often 10,000 to 50,000 cycles for a good package.
The failure mode is always solder joint cracking or wire bond heel cracking. If the device fails electrically (short or open) before the solder cracks, the die attach has failed. Sintered silver die attach should survive 100,000 cycles. Solder die attach usually fails around 20,000 to 40,000 cycles.
During power cycling, you monitor the on-resistance (Rds(on)) or forward voltage (Vf) in real-time. A healthy device shows a stable Rds(on) with minor fluctuations. A failing device shows a sudden, permanent step-increase in Rds(on).
That step is the crack. It means the current path has been interrupted or the contact area has reduced. Do not wait for the device to fail completely. Stop the test when the Rds(on) shifts by more than 5 percent. That is your reliability limit.
Electrical tests tell you that it failed. Cross-sectioning tells you why. You cut the package in half, polish the joint, and look at it under a microscope.
A good joint has a uniform intermetallic layer (IMC) that is 2 to 4 micrometers thick. A bad joint has a thick, scalloped IMC layer (over 5 micrometers) which indicates excessive time above liquidus or too high a peak temperature. It might also have Kirkendall voids — empty spaces inside the IMC caused by unequal diffusion rates of copper and tin.
If you see cracks at the pad interface, the pad design is wrong (sharp corners). If you see cracks in the bulk solder, the alloy is too brittle (needs more bismuth or antimony). If you see cracks at the component lead, the CTE mismatch is too high (need a softer solder or a clip bond).
Optical inspection cannot see inside a plastic package. X-ray is mandatory for high-reliability discrete devices.
You are looking for two things: voids and wire bond shape. A void larger than 25 percent of the pad area in a power device is a failure. It reduces thermal conductivity and creates a stress concentration point.
For wire bonds, check the loop height. If the loop is touching the die or the mold compound, it will short out under vibration or thermal stress. The loop should be free-standing and symmetrical. Asymmetrical loops indicate a bad bonder setup or a lifted bond foot.
For leaded discrete packages (TO-220, TO-247), vibration is the primary killer. The leads act as cantilever beams. Resonance usually occurs between 500 Hz and 2000 Hz.
The test is typically 10 to 20 G rms across 20 Hz to 2000 Hz for 30 minutes per axis. The failure mode is lead fatigue at the glass seal or the mold interface. If the lead breaks at the glass seal, the package is hermetically compromised. If it breaks at the mold, the mechanical support is gone.
For surface mount packages, vibration is less critical because the solder joint dampens the energy. But for large power packages with heavy heatsinks, the heatsink can amplify the vibration at the mounting point. Always test the assembly, not just the bare part.
A 1500 G shock for 0.5 milliseconds simulates a drop event. For small SMD packages (0402, 0201), this is the main qualification test. The failure mode is ceramic cracking (for ceramic packages) or pad cratering (for PCB pads).
Pad cratering is when the copper pad lifts off the FR-4 substrate under the component. It happens because the board is too thin or the pad is too close to a via. If you see pad cratering in your cross-sections, increase the board thickness or move the pad away from the board edge. There is no solder paste fix for this. It is a board design failure.
Do not look at the average life. Look at the Weibull slope (beta).
If beta is less than 1.0, you have infant mortality. The failures are random defects — bad solder joints, contamination, ESD damage. These are screened out by burn-in.
If beta is between 1.0 and 4.0, you have wear-out failures. This is normal fatigue. The life is predictable. This is what you want.
If beta is greater than 4.0, you have a very tight distribution. This usually means the test was not run long enough to see the tail of the distribution, or the sample size was too small. Do not trust a high beta with a small sample size. It is statistical fiction.
Once you have the Weibull parameters (characteristic life eta and slope beta) from the accelerated test, you use the Arrhenius model to extrapolate to 125°C junction temperature (the standard field condition).
The acceleration factor (AF) is calculated based on the activation energy (usually 0.7 eV for solder fatigue). If your test at 150°C gives a life of 100,000 cycles, the life at 125°C might be 1,000,000 cycles.
But be careful. The Arrhenius model assumes the failure mechanism does not change. If you change the failure mechanism (e.g., from solder fatigue to wire bond fatigue) by changing the temperature, the extrapolation is invalid. Always verify the failure mode at the test condition matches the expected field failure mode. If they do not match, the data is useless.
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