diff options
Diffstat (limited to 'gr-radio-astronomy/src/python/usrp_ra_receiver.py')
| -rwxr-xr-x | gr-radio-astronomy/src/python/usrp_ra_receiver.py | 73 |
1 files changed, 40 insertions, 33 deletions
diff --git a/gr-radio-astronomy/src/python/usrp_ra_receiver.py b/gr-radio-astronomy/src/python/usrp_ra_receiver.py index a16f9d3f8..3f9ff85ba 100755 --- a/gr-radio-astronomy/src/python/usrp_ra_receiver.py +++ b/gr-radio-astronomy/src/python/usrp_ra_receiver.py @@ -300,17 +300,20 @@ class app_flow_graph(stdgui.gui_flow_graph): self.integrator2 = gr.fir_filter_fff (M, tapsM) self.integrator3 = gr.single_pole_iir_filter_ff(1.0) + # The detector + self.detector = gr.complex_to_mag_squared() + # Split complex USRP stream into a pair of floats - self.splitter = gr.complex_to_float (1); - - # I squarer (detector) - self.multI = gr.multiply_ff(); - - # Q squarer (detector) - self.multQ = gr.multiply_ff(); + #self.splitter = gr.complex_to_float (1); - # Adding squared I and Q to produce instantaneous signal power - self.adder = gr.add_ff(); +# # I squarer (detector) +# self.multI = gr.multiply_ff(); +# +# # Q squarer (detector) +# self.multQ = gr.multiply_ff(); +# +# # Adding squared I and Q to produce instantaneous signal power +# self.adder = gr.add_ff(); # Signal probe self.probe = gr.probe_signal_f(); @@ -332,30 +335,34 @@ class app_flow_graph(stdgui.gui_flow_graph): self.connect(self.u, self.fft_bandpass, self.scope) if self.setimode == False: - # - # The head of the continuum chain - # - self.connect(self.u, self.splitter) - - # Connect splitter outputs to multipliers - # First do I^2 - self.connect((self.splitter, 0), (self.multI,0)) - self.connect((self.splitter, 0), (self.multI,1)) - - # Then do Q^2 - self.connect((self.splitter, 1), (self.multQ,0)) - self.connect((self.splitter, 1), (self.multQ,1)) - - # Then sum the squares - self.connect(self.multI, (self.adder,0)) - self.connect(self.multQ, (self.adder,1)) - - # Connect adder output to two-stages of FIR integrator - # followed by a single stage IIR integrator, and - # the calibrator - self.connect(self.adder, self.integrator1, - self.integrator2, self.integrator3, self.cal_mult, - self.cal_offs, self.chart) +# # +# # The head of the continuum chain +# # +# self.connect(self.u, self.splitter) +# +# # Connect splitter outputs to multipliers +# # First do I^2 +# self.connect((self.splitter, 0), (self.multI,0)) +# self.connect((self.splitter, 0), (self.multI,1)) +# +# # Then do Q^2 +# self.connect((self.splitter, 1), (self.multQ,0)) +# self.connect((self.splitter, 1), (self.multQ,1)) +# +# # Then sum the squares +# self.connect(self.multI, (self.adder,0)) +# self.connect(self.multQ, (self.adder,1)) +# +# # Connect adder output to two-stages of FIR integrator +# # followed by a single stage IIR integrator, and +# # the calibrator +# self.connect(self.adder, self.integrator1, +# self.integrator2, self.integrator3, self.cal_mult, +# self.cal_offs, self.chart) + + self.connect(self.u, self.detector, + self.integrator1, self.integrator2, + self.integrator3, self.cal_mult, self.cal_offs, self.chart) # Connect calibrator to probe # SPECIAL NOTE: I'm setting the ground work here |