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Std EditionPower supply decoupling and why it matters.

License: Public Domain

Published Time:2016-11-16 19:55:31
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Description

This project is to demonstrate the need for and the basic effect of Power Supply Decoupling.

In real circuits the power supply is not an ideal zero impedance source. The supply itself has some source resistance even though it may be in the order of tens of milliOhms. The wiring and PCB traces present a resistance but more importantly in terms of impedance, they present an inductance in series with the supply and some inherent parallel capacitance to ground.

If The supply comes from some sort of regulator it will have a load current transient response that may cause the output voltage to momentarily undershoot below and then overshoot above the nominal regulated output voltage. The behaviour of this under and overshoot is an indication of the stability of the regulator and is strongly dependent on the capacitance presented at the output of the regulator. For IC regulators, the recommendations in the device datasheet MUST be followed to ensure the stability of the regulator output voltage.

Even if the supply is from the output of a properly decoupled IC regulator, the wiring, leads and PCB traces both from the regulator output to the load and from the load back to ground, present additional resistance. More importantly however, in terms of impedance, they present an inductance in series with the supply and some inherent parallel capacitance to ground.

For example a 0.1mm diameter wire has an inductance of about 10nH/cm (https://chemandy.com/calculators/round-wire-inductance-calculator.htm)

and a 0.2mm wide by 0.035mm thick (i.e. 1oz) copper PCB trace has an inductance of about 6nH/cm (https://chemandy.com/calculators/flat-wire-inductor-calculator.htm).

Bearing in mind that the wiring length includes the path from and back to the supply it is easy to see how the inductance (Lser) in series with the supply can easily be in the region of 100nH.

The stray capacitance (Cpar) distributed between the supply and the load can also easily be in the region of a few tens to a couple of hundred pF.

When a current step is drawn through a series inductance (Lser) with a parallel capacitance (Cpar) to ground, it will cause a large initial voltage drop which will then exhibit damped oscillations at the natural resonant frequency of the LC circuit above and below the supply rail. When the current ceases there will be a large intitial voltage rise which will then exhibit damped oscillations below and above the supply rail. The closer together the current start and stop times are compared to the period of the natural resonant frequency of the LC circuit, the more the response to the current start step tends to be cancelled out by the response caused by the current ceasing.

In other words if the period of the natural resonant frequency of the LC circuit formed by the series supply inductance and the parallel capacitance to ground is large compared to the time between the edges of the current steps or the width of the current spikes, the smaller the overall voltage transient at the output of this LC circuit will tend to be.

The process of making the period of the natural resonant frequency of the LC circuit significantly lower than the time between the edges of the current spikes is called Power Supply Decoupling.

In real circuits it is not possible to make L or C zero and bearing in mind that in practical circuits every connection of a device to a supply creates its own little LC circuit local to that device, in practice it is usually easier to increase C by adding one or more physical capacitors to the circuit local to each device, than it is to increase L by adding physical inductors in series with the supply to each device.

Decoupling across the supply pins is essential for all active devices such as op amps, comparators, amplifiers, voltage regulators, ADCs, DACs, gate drivers, timing and digital devices as well as across the supply and ground for discrete circuits that draw fluctuating supply currents such as transistor amplifiers, high and low side load switching circuits, motor and relay drivers.

In some cases such as low noise and RF circuits, a combination of series inductance and resistance with parallel caacitance to ground is added locally to each device but that is usually advised in the particular device datasheets and application notes and such additional decoupling measures are not generally required for most analogue and digital circuits.

This project includes simulations that demonstrate:

The basic effect of Power Supply Decoupling and the relationship between the period of the natural frequency of the LC circuit and the time interval between the edges of current steps.

Why decoupling capacitors are required to reduce supply rail transients caused by single ended load switching circuits such as transistor amplifiers and switches, relay and motor drivers;

Why decoupling capacitors are required to reduce supply rail transients caused by so-called shoot-through current spikes.

The additional effects of the same circuits driving a resistive load.

Why decoupling capacitors are essential when using bipolar technology versions of the 555 timer IC.

To run a simulation do:

CTRL+R

To view the simulation results of one or more particular circuits, select and set the probe command(s) then - in the right hand panel - set:

text type = spice

Set all other instances of the probe commands to:

text type = comment

More background information here:

https://en.wikipedia.org/wiki/Decoupling_capacitor

Documents

An example of power supply decoupling in action

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Another example of power supply decoupling in action

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More examples of power supply decoupling in action

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Decoupling 555 timer circuits

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Short vs long current pulses

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ID Designator Footprint Quantity
1 B1 NONE 1
2 B2 NONE 1
3 B3 NONE 1
4 B4 NONE 1
5 B5 NONE 1
6 C1,C2 C0805 2
7 C3,C4,C5,C6,C7 C0805 5
8 L1,L2 INDUCTOR-1206 2
9 M1,M3,M5,M7,M9 NONE 5
10 M2,M4,M6,M8,M10 SOT23 5
11 R1,R2,R3,R4 R0805 4
12 R5,R6,R7,R8,R9 R0805 5
13 R10,R11,R12,R13,R14,R5,R6,R7,R8,R9 R0805 10
14 V1 2P-5.0 1
15 V2 2P-5.0 1
16 VIMON1,VIMON2A,VIMON2B,VIMON3A,VIMON3B,VIMON4A,VIMON4B,VIMON5A,VIMON5B 2P-5.0 9
17 V2 2P-5.0 1
18 C8 RAD-0.1 1
19 C9 RAD-0.1 1
20 C10 RAD-0.1 1
21 L3 AXIAL-0.4 1
22 R15,R16,R19,R20 AXIAL-0.3 4
23 R17,R18 AXIAL-0.3 2
24 U1,U2 DIP8 2
25 V3,V4 HDR1X2 2
26 CPAR1 RAD-0.1 1
27 I1 2P-5.08 1
28 I2 2P-5.08 1
29 LSER1 AXIAL-0.4 1
30 R21 AXIAL-0.3 1

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