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Line 6: Line 6:
 
for measuring current:
 
for measuring current:
 
* resistive shunt
 
* resistive shunt
** low-side current shunt
+
* low-side current shunt
 
** high-side current shunt
 
** high-side current shunt
 
* magnetic field sense
 
* magnetic field sense
Line 15: Line 15:
 
== resistive shunt ==
 
== resistive shunt ==
  
With the resistive shunt technique,
 
all the charge flowing through the the load also flows through a resistor (the shunt resistor) in series with the load.
 
  
[https://www.electronicdesign.com/archive/article/21753058/whats-all-this-shunt-stuff-anyhow "What's All This Shunt Stuff, Anyhow?"]
+
[http://electronicdesign.com/article/articles/what-s-all-this-shunt-stuff-anyhow-2144.aspx "What's All This Shunt Stuff, Anyhow?"]
 
by Bob Pease 2002
 
by Bob Pease 2002
 
describes one way to custom-build a high-current shunt.
 
describes one way to custom-build a high-current shunt.
Line 27: Line 25:
 
Even though a copper shunt has a pretty bad resistance variation with temperature (tempco), other parts in this circuit compensate for it.
 
Even though a copper shunt has a pretty bad resistance variation with temperature (tempco), other parts in this circuit compensate for it.
  
=== low-side current shunt ===
+
== low-side current shunt ==
 
 
      +-----------------+
 
      |                |
 
      |  +            (load)
 
    (power)              |
 
      |  -            (shunt R)
 
      |                |
 
      +-----------------+
 
      |
 
      GND
 
 
 
 
Low-side is (electrically) the simplest.
 
Low-side is (electrically) the simplest.
  
Line 46: Line 33:
  
 
=== high-side current shunt ===
 
=== high-side current shunt ===
 
      +-----------------+
 
      |                |
 
      |  +            (shunt R)
 
    (power)              |
 
      |  -            (load)
 
      |                |
 
      +-----------------+
 
      |
 
      GND
 
  
 
In situations where low-side sensing is difficult ( automobile electronics bonded to the "GND" car frame; other systems where it is inconvenient to put a resistor on the "lo" power wire), we turn to high-side sensing.
 
In situations where low-side sensing is difficult ( automobile electronics bonded to the "GND" car frame; other systems where it is inconvenient to put a resistor on the "lo" power wire), we turn to high-side sensing.
Line 85: Line 62:
 
== MOSFET voltage ==
 
== MOSFET voltage ==
  
[http://www.4qdtec.com/mircl.html pseudo 'mirror' current sensing a MOSFET] -- sampling the voltage across a MOSFET while it is turned on. That voltage is linear with current but varies with temperature. If the purpose of measuring current is to turn off the MOSFET before it overheats, the variation with temperature doesn't matter. (''A true [[current mirror]] isn't useful for motors, right?'')
+
[http://www.4qdtec.com/mircl.html pseudo 'mirror' current sensing a MOSFET] -- sampling the voltage across a MOSFET while it is turned on. That voltage is linear with current but varies with temperature. If the purpose of measuring current is to turn off the MOSFET before it overheats, the variation with temperature doesn't matter. (''A true [http://en.wikipedia.org/wiki/Current_mirror current mirror] isn't useful for motors, right?'')
  
 
This uses the turned-on resistance of the MOSFET as if it were a shunt resistor.
 
This uses the turned-on resistance of the MOSFET as if it were a shunt resistor.
Line 95: Line 72:
 
==== lossless average inductor current sensing ====
 
==== lossless average inductor current sensing ====
 
The "lossless average inductor current sensing" technique:
 
The "lossless average inductor current sensing" technique:
 
    (switched)--------+-----+
 
    (power)          |    |
 
                      |    Rs
 
                      |    |
 
                (L1 + DCR)  +--- Isense+
 
                      |    |
 
                      |    C
 
                      |    |
 
                      +-----+--- Isense-
 
                      |
 
                    (load)
 
                      |
 
                    GND
 
  
 
The current through an inductor with some known internal parasitic resistance DCR can be sensed with a series resistor (Rs) and capacitor network connected in parallel with the inductor-resistor network.
 
The current through an inductor with some known internal parasitic resistance DCR can be sensed with a series resistor (Rs) and capacitor network connected in parallel with the inductor-resistor network.
The designer picks the sense components Rs and C such that Rs*C -- the time constant of the RC network -- is close enough to L/DCR -- the time constant of the inductor resistor network. Then the voltage across C is proportional to the current through L.
+
The designer picks the sense components Rs and C such that Rs*C -- the time constant of the RC network -- is close enough to L/DCR -- the time constant of the inductor resistor network -- then the voltage across C is proportional to the current through L.
 
(IR3508Z data sheet
 
(IR3508Z data sheet
 
[http://www.irf.com/product-info/datasheets/data/ir3508zmpbf.pdf])
 
[http://www.irf.com/product-info/datasheets/data/ir3508zmpbf.pdf])
 
     current through L == voltage across C * (1/DCR).
 
     current through L == voltage across C * (1/DCR).
 
<ref>
 
Dr. F.A.E.
 
[http://blog.fairchildsemi.com/2015/navigating-dcr-currents "Navigating DCR Currents"].
 
2015.
 
</ref>
 
  
 
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