- Em promoção!
- -1,10 €
Sensor de presença Microondas - RCWL-0516
DESCRIÇÃO EM PORTUGUÊS BREVEMENTE DISPONÍVEL
Se tiver alguma dúvida neste produto não hesite em contactar-nos.
*Atenção: as imagens são meramente ilustrativas.
There is a lively discussion on the project issue tracker. So make sure you check it out.
RCWL-0516 is a doppler radar microwave motion sensor module which can act as an alternative to a PIR motion sensor. This git repository is an attempt to collect the rather scant information on this board in one place.
Operating frequency: The product specification omits the operating frequncy. I found a carrier at 3.181GHz on my unit using a HackRF One SDR radio (see spectrum plot below). I suspect this frequency will vary from device to device: it would be difficult to have a tight specification with such a simple RF circuit on FR4 PCB.
Working voltage: 4 - 28V. It provides a convenient 3.3V output to drive a MCU (good for 100mA ?).
The forward side of the board is the side with components. This side should face the objects being detected. Do not obstruct forward side with anything metalic. The back side should have clearance of more than 1cm from any metal.
|3V3||3.3V regulated output. Max 100mA (?)|
|OUT||Trigger: high (3.3V) if motion detected. 0V normally.|
|VIN||4 - 28V supply voltage|
|CDS||LDR 10-20k RL, U_LDR > 0.7V = On|
There are two parts to this circuit: 1. A microwave frequency transmitter/receiver/mixer and 2.a much lower frequency part based on an IC (marked RCWL-9196) which is very similar to the BISS0001 IC used in PIR motion detectors.
First the microwave part:
The best explanation of how the microwave part of this works is in patent EP3091605A1. It describes as similar type of module operating at 5.8GHz.
At the heart of the RF is a Q1 a MMBR941M high frequency NPN transistor  in what is probably a Colpitt oscillator  configuration. The schematic above is misleading because it omits a key inductor and capacitors constructed from PCB traces (a microline inductor and capacitor). The inductor is the S curve trace on the top surface and capacitors are the ring structure on the bottom surface and also the rectangular block to the left of the S curve. Using the formula at reference  below I calculte the inductance of the S curve to be (very approximately) 10nH.
A critical function of a doppler radar is to be able to 'mix' the reflected signal with the transmitted signal to arrive at a frequency which is the difference between the transmitted and reflected signal. In this board Q1 also cleverly assumes the function of the mixer: [TODO: this really needs to be explained].
The low doppler frequency difference is extracted by a low pass RC filter (C9 = 1nF, R3 = 1k, fc = 1/2πRC ≈ 160kHz) and amplified by the RCWL-9196 IC and treated exactly the same as a signal from a PIR sensor.
Update 4 Jan 2017: finally found the signal at 3.181GHz with the HackRF One SDR! One interesting observation: waving my hand in front of the sensor causes significant changes in the transmitting frequency, shifting by up to 1MHz. My theory: the low frequency doppler shift causes small changes in the transistor base bias. I used spice simulations to verify that small changes to transistor base bias causes changes in oscillation frequency. By running a few simulations I estimate that 1µV change in bias will change oscillation frequncy by 1.4MHz.
The low frequncy part
The core of the low frequncy signal processing is an IC marked RCWL-9196. The schematic says (in chinese) that it's similar to a BISS0001 PIR IC. But there are differences. Unfortunately I can't find any hard information (eg datasheet) on this. Nor can I find any information on the brand/company name "RCWL".
|1||A Retriggerable & non-retriggerable mode select (A=1 : re-triggerable)||3.3V regulated output (100mA max?)|
|2||VO Detector output pin (active high)||same|
|3||RR1 Output pulse width control (Tx)||same?|
|4||RC1 Output pulse width control (Tx)||same?|
|5||RC2 Trigger inhibit control (Ti)||same?|
|6||RR2 Trigger inhibit control (Ti)||same?|
|8||VRF RESET & voltage reference input (Normally high. Low=reset)||Vin (4 - 28V)|
|9||VC Trigger disable input (VC > 0.2Vdd=enable; Vc < 0.2Vdd =disabled)||same|
|10||IB Op-amp input bias current setting||?|
|11||Vdd Supply voltage||3.3V regulated output (again?)|
|12||2OUT 2nd stage Op-amp output||same|
|13||2IN- 2nd stage Op-amp inverting input||same|
|14||1IN+ 1st stage Op-amp non-inverting input||same|
|15||1IN- 1st stage Op-amp inverting input||same|
|16||1OUT 1st stage Op-amp output||same|
On the back of the board (the side without components) are pads for 3 optional components (0805 dimensions).
|C-TM||Regulate the repeat trigger time. The default (unpopulated) time is 2s. A SMD capacitor to extend the repeat trigger time. Pin 3 of the IC emits a frequency (f), and the tigger time in seconds is given by (1/f) * 32678|
|R-GN||The default detection range is 7m, adding a 1M resistor reduces it to 5m|
|R-CDS||the VCC is in parrel connection with CDS(RCWL-9196 pin 9) through R-CDS. Connect the LDR at the R-CDS to turn off the detecting function at night. (?? TODO: make sense of this)|
I started with an example Colpitt circuit  and substituted the 2N3904 NPN with a MMBR941 (Spice model from ). I am using the Windows LTSpice from Linear Technologies (available as free download , also works with Linux under Wine emulator). See colpitt.asc for a working Colpitt oscillator and rcwl-0516.asc for a model of the RCWL-0516 (however it does not oscillate!).
Doppler effect calculations
If ft is the transmitted frequency, fr is the reflected frequency (as measured by the common transmit/receive antenna on the sensor), v is the speed of the target relative to the sensor (negative if receeding, positive if advancing toward sensor), c is the speed of light and fd = (fr-fd) is the doppler shift, then:
fr = ft (c + v) / (c - v)
fd = fr - ft = 2v ft / (c - v)
If ( c << v) then fd ≈ 2v ft / c
Assume typical human motion speed of v = 1 m/s. ft = 3.181GHz, c = 2.998E8 m/s, then fd = 10Hz.
Também poderá gostar