diff options
Diffstat (limited to 'docs/doxygen')
| -rw-r--r-- | docs/doxygen/other/main_page.dox | 18 | ||||
| -rw-r--r-- | docs/doxygen/other/pfb_intro.dox | 6 |
2 files changed, 12 insertions, 12 deletions
diff --git a/docs/doxygen/other/main_page.dox b/docs/doxygen/other/main_page.dox index 2826824647..15a56d0dec 100644 --- a/docs/doxygen/other/main_page.dox +++ b/docs/doxygen/other/main_page.dox @@ -62,7 +62,7 @@ done. A single source and sink are used with a FIR filter between them. \code - from gnuradio import gr, filter + from gnuradio import gr, filter, analog class my_topblock(gr.top_block): def __init__(self): @@ -71,7 +71,7 @@ them. amp = 1 taps = filter.firdes.low_pass(1, 1, 0.1, 0.01) - self.src = gr.noise_source_c(gr.GR_GAUSSIAN, amp) + self.src = analog.noise_source_c(gr.GR_GAUSSIAN, amp) self.flt = filter.fir_filter_ccf(1, taps) self.snk = gr.null_sink(gr.sizeof_gr_complex) @@ -203,19 +203,19 @@ running and processing data, performing the reconfiguration, and then restarting the graph by unlocking it. The following example code shows a graph that first adds two -gr_noise_source_c blocks and then replaces the gr_add_cc block with a +analog::noise_source_c blocks and then replaces the gr_add_cc block with a gr_sub_cc block to then subtract the sources. \code -from gnuradio import gr +from gnuradio import gr, analog import time class mytb(gr.top_block): def __init__(self): gr.top_block.__init__(self) - self.src0 = gr.noise_source_c(gr.GR_GAUSSIAN, 1) - self.src1 = gr.noise_source_c(gr.GR_GAUSSIAN, 1) + self.src0 = analog.noise_source_c(gr.GR_GAUSSIAN, 1) + self.src1 = analog.noise_source_c(gr.GR_GAUSSIAN, 1) self.add = gr.add_cc() self.sub = gr.sub_cc() self.head = gr.head(gr.sizeof_gr_complex, 1000000) @@ -262,15 +262,15 @@ The following example expands the previous example but sets and resets the max noutput_items both locally and globally. \code -from gnuradio import gr +from gnuradio import gr, analog import time class mytb(gr.top_block): def __init__(self): gr.top_block.__init__(self) - self.src0 = gr.noise_source_c(gr.GR_GAUSSIAN, 1) - self.src1 = gr.noise_source_c(gr.GR_GAUSSIAN, 1) + self.src0 = analog.noise_source_c(gr.GR_GAUSSIAN, 1) + self.src1 = analog.noise_source_c(gr.GR_GAUSSIAN, 1) self.add = gr.add_cc() self.sub = gr.sub_cc() self.head = gr.head(gr.sizeof_gr_complex, 1000000) diff --git a/docs/doxygen/other/pfb_intro.dox b/docs/doxygen/other/pfb_intro.dox index 429e8fe5b6..504ae87b87 100644 --- a/docs/doxygen/other/pfb_intro.dox +++ b/docs/doxygen/other/pfb_intro.dox @@ -64,9 +64,9 @@ defined to use a sample rate of \p filter_size times the signal's sampling rate. A helpful wrapper for the arbitrary resampler is found in -<b>gnuradio-core/src/python/gnuradio/blks2impl/pfb_arb_resampler.py</b>, -which is exposed in Python as <b>blks2.pfb_arb_resampler_ccf</b> and -<b>blks2.pfb_arb_resampler_fff</b>. This block is set up so that the +<b>gr-filter/python/pfb.py</b>, +which is exposed in Python as <b>filter.pfb.arb_resampler_ccf</b> and +<b>filter.pfb.arb_resampler_fff</b>. This block is set up so that the user only needs to pass it the real number \p rate as the resampling rate. With just this information, this hierarchical block automatically creates a filter that fully passes the signal bandwidth |