etic field,
errite core of one of those,
precise.
ll sensors.
as a simulated magnetic field from
I expected!
=A0 =A0 =A0 =A0 =A0 =A0 =A0--------------------- +5V from USB
=A0 =A0 =A0 =A0 =A0 =A0 | =A0 =A0 =A0 =A0 =A0|
=A0 =A0 =A0 =A0 =A0 =A0 | =A0 =A0 =A0 =A0 =A0|
=A0 =A0 =A0 =A0|---- =A0d =A0 =A0 =A0 =A0|
=A0 =A0 =A0 =A0|
=A0 =A0 =A0 |---- =A0s =A0 =A0 =A0 =3D=3D=3D
p =A0 =A0 =A0 =A0| =A0 =A0 =A0 =A0 ---
| =A0 =A0 =A0 =A0 =A0| 47 uF
=A0 =A0| =A0 =A0 =A0 =A0 =A0|
=A0[ ]1k5 =A0 =A0 =A0|
=A0 =A0 =A0 =A0 =A0 =A0| =A0 =A0 =A0 =A0 =A0|
=A0 =A0 =A0 =A0/// =A0 =A0 =A0 =A0///
the inductor!
re effects get cancelled,
u can do all sorts
...
ur sqrt LC if you like),
play with, as they are :-)
..
..
gmented in the PIC.
Hello Jan,
Temperature will be your enemy. Why not using a feedback loop where you nullify the field in the core?
This is used by LEM in their current sensors,
When you want to use the oscillator approach, you can use the second oscillator as reference for you control loop. So you adjust the bias field for the measuring coil until frequencies are equal. This loop may be slow as the frequency of your measuring oscillator increases for negative and positive currents (or you should add a DC bias field).
By using one oscillator without any fixed bias field, you can adjust the bias field to get lowest frequency. The current through you bias coil is directly proportional to the current to be measured.
Best regards,
Wim PA3DJS