I was thinking decoupling, but you would have to overdimension them because of the high tolerance and temperature stability. And doesn't a 1uF capacitor (instead of 100nF) have the same inductance problems as a 1uF X7R for decoupling?
Are there other applications where the tolerances and variations are so little important that a Y5V or Z5U could be preferred over X5R or X7R? I realize they're somewhat cheaper but that doesn't count if the quality is too bad to be useful, IMO.
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I would say the uses can vary depending on your initial project goals/specifications (e.g. what temperature range you want the circuit to perform under, voltage range etc) |
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In most home consumer electronics, rated to operate from only (say) 10C - 35C, the temperature coefficient doesn't matter that much. The poor tolerance could be compensated for by using multiple low cost Y5V/Z5U capacitors. Also sometimes the standard 100nF decoupling capacitor can be made smaller without significant performance loss. |
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I suspect that in many applications, if a "10uF" cap with an inferior dielectric, paralleled with a good 0.1uF cap, will work as effectively for bypassing as would an ideal 1uF cap, but will cost less than a 1uF cap with a good dielectric. On the other hand, I've sometimes thought that for bypassing devices which will be switched on and off fairly often, having a cap whose capacitance dropped off sharply with voltage could actually be an advantage. Suppose one has a 3.3-volt device which draws 1mA, needs 1uF of bypassing, and is needed for 1ms once per second; the device will completely drain the cap between uses. Charging the cap to 3.3 volts will require 3.3 microcoulombs of electricity, every time the cap is switched off, that energy will be wasted. Every second, the device will require one coulomb of energy during the 1ms that it's "on", and burn 3.3uC uselessly after it's "turned off". In effect, the cap would be wasting three times as much energy as the device was actually using. Now suppose that one could get a cap with a capacitance of 3.3uF at below 0.1 volts, and zero capacitance above that, and one wired that cap in parallel with the power switching device; assume further that the input to the power switching device has 100uF of usable capacity. To allow for inductance in that cap or the 100uF board cap, the device also has 0.1uF of "normal" capacitance in parallel with it. In that scenario, each on/off cycle will require charging the 0.1uF cap to 3.3 volts, requiring 0.33uC, and charging the 3.3uF cap to 0.1 volts (no energy will be spent charging it from 0.1 to 3.3 volts) using another 0.33uC. So energy wastage would be cut from 3.3uC (or 330% of the current usefully employed by the device) to 0.66uC (or 66% of the current usefully employed). Wastage would be cut by 80%; energy consumption would be cut by over 60%. In practice, I doubt one can get caps of suitable values with such a sharp fall-off of capacity versus voltage, but if one could, it would be possible to greatly enhance the efficiency of some battery-powered devices. |
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bulk bulk bulk bulk bulk bulk bulk bulk.... Bulk capacitance, where you need to store as much energy as possible in a given package. You supplement it with smaller capacitors that have better high-frequency characteristics if you want good overall bypassing. |
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Cheap Z5U and Y5V dielectrics will loose typical 80% of capacitance at rated voltage. So a smaller X7R will do the job too even at higher frequency. Dont be fooled! |
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