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author | Nao Pross <np@0hm.ch> | 2021-12-05 23:36:10 +0100 |
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committer | Nao Pross <np@0hm.ch> | 2021-12-05 23:36:10 +0100 |
commit | f3841a7720eb395b8f6408780e7b540a4d8c4127 (patch) | |
tree | 27f0131a1e0e04a1f3bf5b0f9781a3b23e5dbd94 /tests | |
parent | Merge branch 'master' of github.com:NaoPross/Fading (diff) | |
download | Fading-f3841a7720eb395b8f6408780e7b540a4d8c4127.tar.gz Fading-f3841a7720eb395b8f6408780e7b540a4d8c4127.zip |
Nicer notation in block_phase
Diffstat (limited to '')
-rw-r--r-- | tests/correlator/correlator.grc | 56 | ||||
-rwxr-xr-x | tests/correlator/correlator.py | 10 | ||||
-rw-r--r-- | tests/correlator/epy_block_0.py | 9 |
3 files changed, 30 insertions, 45 deletions
diff --git a/tests/correlator/correlator.grc b/tests/correlator/correlator.grc index c34e5a9..ff09a40 100644 --- a/tests/correlator/correlator.grc +++ b/tests/correlator/correlator.grc @@ -527,35 +527,33 @@ blocks: \ - start.offset\n\n # unpack pmt values into start and end phase\n \ \ sphase = pmt.to_python(start.value)\n ephase = pmt.to_python(end.value)\n\ \n # compute frequency offset between start and end\n phasediff\ - \ = ephase - sphase\n\n if phasediff > np.pi:\n phasediff\ - \ -= 2*np.pi\n\n elif phasediff < -np.pi:\n phasediff += 2*np.pi\n\ - \n freq = phasediff / nsamples\n\n # save this one for the last\ - \ block (see variable `end' in self.work)\n self.lastfreq = freq\n\n\ - \ # debugging\n print(f\"Correction for chunk of {nsamples:2d}\ - \ samples is \" \\\n f\"sphase={sphase: .4f} rad and freq={freq*1e3:\ - \ .4f} milli rad / sample\")\n\n # compute chunk values\n return\ - \ sphase * np.ones(nsamples) + freq * np.arange(0, nsamples)\n\n def work(self,\ - \ input_items, output_items):\n counter = self.nitems_written(0)\n\n\ - \ # nicer aliases\n inp = input_items[0]\n out = output_items[0]\n\ - \n # read phase tags\n is_phase = lambda tag: pmt.to_python(tag.key)\ - \ == \"phase_est\"\n tags = list(filter(is_phase, self.get_tags_in_window(0,\ - \ 0, len(inp))))\n\n if not tags:\n print(f\"There were no\ - \ tags in {len(inp)} samples!\")\n out[:] = inp\n return\ - \ len(out)\n\n # debugging\n print(f\"Processing {len(tags)} tags\ - \ = {tags[-1].offset - tags[0].offset} \" \\\n f\"samples out of\ - \ {len(inp)} input samples\")\n\n # compute \"the middle\"\n enough_samples\ - \ = lambda pair: ((pair[1].offset - pair[0].offset) > 0)\n pairs = list(filter(enough_samples,\ - \ zip(tags, tags[1:])))\n chunks = [ self.block_phase(start, end) for\ - \ (start, end) in pairs ]\n middle = np.concatenate(chunks) if chunks\ - \ else []\n\n # compute values at the end, we do not have informations\ - \ about the future\n # but we can use the frequency of the last tag to\ - \ approximate\n nback = len(inp) - (tags[-1].offset - counter)\n \ - \ print(f\"Processing {nback} samples at the back of the buffer\")\n \ - \ end = np.ones(nback) * pmt.to_python(tags[-1].value) \\\n \ - \ + self.lastfreq * np.arange(0, nback)\n\n # compute the \"start\"\ - , using the last tag from the previous call\n nfront = tags[0].offset\ - \ - counter\n print(f\"Processing {nfront} samples at the front of the\ - \ buffer\")\n start = self.block_phase(self.last, tags[0])[-nfront:]\ + \ = (ephase - sphase) % (2 * np.pi)\n freq = phasediff / nsamples\n\n\ + \ # save this one for the last block (see variable `end' in self.work)\n\ + \ self.lastfreq = freq\n\n # debugging\n print(f\"Correction\ + \ for chunk of {nsamples:2d} samples is \" \\\n f\"sphase={sphase:\ + \ .4f} rad and freq={freq*1e3: .4f} milli rad / sample\")\n\n # compute\ + \ chunk values\n return sphase * np.ones(nsamples) + freq * np.arange(0,\ + \ nsamples)\n\n def work(self, input_items, output_items):\n counter\ + \ = self.nitems_written(0)\n\n # nicer aliases\n inp = input_items[0]\n\ + \ out = output_items[0]\n\n # read phase tags\n is_phase\ + \ = lambda tag: pmt.to_python(tag.key) == \"phase_est\"\n tags = list(filter(is_phase,\ + \ self.get_tags_in_window(0, 0, len(inp))))\n\n if not tags:\n \ + \ print(f\"There were no tags in {len(inp)} samples!\")\n out[:]\ + \ = inp\n return len(out)\n\n # debugging\n print(f\"\ + Processing {len(tags)} tags = {tags[-1].offset - tags[0].offset} \" \\\n \ + \ f\"samples out of {len(inp)} input samples\")\n\n # compute\ + \ \"the middle\"\n enough_samples = lambda pair: ((pair[1].offset - pair[0].offset)\ + \ > 0)\n pairs = list(filter(enough_samples, zip(tags, tags[1:])))\n\ + \ chunks = [ self.block_phase(start, end) for (start, end) in pairs ]\n\ + \ middle = np.concatenate(chunks) if chunks else []\n\n # compute\ + \ values at the end, we do not have informations about the future\n #\ + \ but we can use the frequency of the last tag to approximate\n nback\ + \ = len(inp) - (tags[-1].offset - counter)\n print(f\"Processing {nback}\ + \ samples at the back of the buffer\")\n end = np.ones(nback) * pmt.to_python(tags[-1].value)\ + \ \\\n + self.lastfreq * np.arange(0, nback)\n\n # compute\ + \ the \"start\", using the last tag from the previous call\n nfront =\ + \ tags[0].offset - counter\n print(f\"Processing {nfront} samples at\ + \ the front of the buffer\")\n start = self.block_phase(self.last, tags[0])[-nfront:]\ \ \\\n if self.last and nfront else np.zeros(nfront)\n\n \ \ # compute correction\n correction = np.exp(-1j * np.concatenate([start,\ \ middle, end]))\n length = len(correction)\n\n # write outputs\n\ diff --git a/tests/correlator/correlator.py b/tests/correlator/correlator.py index d9dedb2..fddf8ea 100755 --- a/tests/correlator/correlator.py +++ b/tests/correlator/correlator.py @@ -7,7 +7,7 @@ # GNU Radio Python Flow Graph # Title: Correlator Test # Author: Naoki Pross -# GNU Radio version: 3.8.2.0 +# GNU Radio version: 3.8.1.0 from distutils.version import StrictVersion @@ -37,7 +37,6 @@ from gnuradio import eng_notation import epy_block_0 import epy_block_1 import numpy as np - from gnuradio import qtgui class correlator(gr.top_block, Qt.QWidget): @@ -390,7 +389,6 @@ class correlator(gr.top_block, Qt.QWidget): self.connect((self.epy_block_0, 0), (self.digital_constellation_decoder_cb_0, 0)) self.connect((self.epy_block_0, 0), (self.qtgui_const_sink_x_0_0, 0)) - def closeEvent(self, event): self.settings = Qt.QSettings("GNU Radio", "correlator") self.settings.setValue("geometry", self.saveGeometry()) @@ -471,8 +469,6 @@ class correlator(gr.top_block, Qt.QWidget): - - def main(top_block_cls=correlator, options=None): if StrictVersion("4.5.0") <= StrictVersion(Qt.qVersion()) < StrictVersion("5.0.0"): @@ -481,9 +477,7 @@ def main(top_block_cls=correlator, options=None): qapp = Qt.QApplication(sys.argv) tb = top_block_cls() - tb.start() - tb.show() def sig_handler(sig=None, frame=None): @@ -499,9 +493,9 @@ def main(top_block_cls=correlator, options=None): def quitting(): tb.stop() tb.wait() - qapp.aboutToQuit.connect(quitting) qapp.exec_() + if __name__ == '__main__': main() diff --git a/tests/correlator/epy_block_0.py b/tests/correlator/epy_block_0.py index dbdadd1..aa3065a 100644 --- a/tests/correlator/epy_block_0.py +++ b/tests/correlator/epy_block_0.py @@ -46,14 +46,7 @@ class blk(gr.sync_block): ephase = pmt.to_python(end.value) # compute frequency offset between start and end - phasediff = ephase - sphase - - if phasediff > np.pi: - phasediff -= 2*np.pi - - elif phasediff < -np.pi: - phasediff += 2*np.pi - + phasediff = (ephase - sphase) % (2 * np.pi) freq = phasediff / nsamples # save this one for the last block (see variable `end' in self.work) |