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#!/usr/bin/env python3
import numpy as np
import logging
import os
from bisect import bisect_left, bisect_right
logger = logging.getLogger(__name__)
class DataProcessor:
def __init__(self, sync_data, et_timestamps, et_power):
"""
Creates DataProcessor object.
:param sync_data: input timestamps (SigrokResult)
:param energy_data: List of EnergyTrace datapoints
"""
self.raw_sync_timestamps = []
# high-precision LA/Timer timestamps at synchronization events
self.sync_timestamps = []
# low-precision energytrace timestamps
self.et_timestamps = et_timestamps
# energytrace power values
self.et_power_values = et_power
self.sync_data = sync_data
self.start_offset = 0
# TODO determine automatically based on minimum (or p1) power draw over measurement area + X
# use 0.02 for HFXT runs
self.power_sync_watt = 0.011
self.power_sync_len = 0.7
self.power_sync_max_outliers = 2
def run(self):
"""
Main Function to remove unwanted data, get synchronization points, add the offset and add drift.
:return: None
"""
# remove Dirty Data from previously running program (happens if logic Analyzer Measurement starts earlier than
# the HW Reset from energytrace)
use_data_after_index = 0
for x in range(1, len(self.sync_data.timestamps)):
if self.sync_data.timestamps[x] - self.sync_data.timestamps[x - 1] > 1.3:
use_data_after_index = x
break
time_stamp_data = self.sync_data.timestamps[use_data_after_index:]
# Each synchronization pulse consists of two LogicAnalyzer pulses, so four
# entries in time_stamp_data (rising edge, falling edge, rising edge, falling edge).
# If we have less then twelve entries, we observed no transitions and don't even have
# valid synchronization data. In this case, we bail out.
if len(time_stamp_data) < 12:
raise RuntimeError(
f"LogicAnalyzer sync data has length {len(time_stamp_data)}, expected >= 12"
)
self.raw_sync_timestamps = time_stamp_data
# NEW
datasync_timestamps = []
sync_start = 0
outliers = 0
pre_outliers_ts = None
# TODO only consider the first few and the last few seconds for sync points
for i, timestamp in enumerate(self.et_timestamps):
power = self.et_power_values[i]
if power > 0:
if power > self.power_sync_watt:
if sync_start is None:
sync_start = timestamp
outliers = 0
else:
# Sync point over or outliers
if outliers == 0:
pre_outliers_ts = timestamp
outliers += 1
if outliers > self.power_sync_max_outliers:
if sync_start is not None:
if (pre_outliers_ts - sync_start) > self.power_sync_len:
datasync_timestamps.append(
(
sync_start,
pre_outliers_ts,
)
)
sync_start = None
if power > self.power_sync_watt:
if (self.et_timestamps[-1] - sync_start) > self.power_sync_len:
datasync_timestamps.append((sync_start, pre_outliers_ts))
# print(datasync_timestamps)
# time_stamp_data contains an entry for each level change on the Logic Analyzer input.
# So, time_stamp_data[0] is the first low-to-high transition, time_stamp_data[2] the second, etc.
# -> time_stamp_data[2] is the low-to-high transition indicating the end of the first sync pulse
# -> time_stamp_data[-8] is the low-to-high transition indicating the start of the first after-measurement sync pulse
start_timestamp = datasync_timestamps[0][1]
start_offset = start_timestamp - time_stamp_data[2]
end_timestamp = datasync_timestamps[-2][0]
end_offset = end_timestamp - (time_stamp_data[-8] + start_offset)
logger.debug(
f"Measurement area: ET timestamp range [{start_timestamp}, {end_timestamp}]"
)
logger.debug(
f"Measurement area: LA timestamp range [{time_stamp_data[2]}, {time_stamp_data[-8]}]"
)
logger.debug(f"Start/End offsets: {start_offset} / {end_offset}")
if abs(end_offset) > 10:
raise RuntimeError(
f"synchronization end_offset == {end_offset}. It should be no more than a few seconds."
)
# adjust start offset
with_offset = np.array(time_stamp_data) + start_offset
logger.debug(
f"Measurement area with offset: LA timestamp range [{with_offset[2]}, {with_offset[-8]}]"
)
# adjust stop offset (may be different from start offset due to drift caused by
# random temperature fluctuations)
with_drift = self.addDrift(
with_offset, end_timestamp, end_offset, start_timestamp
)
logger.debug(
f"Measurement area with drift: LA timestamp range [{with_drift[2]}, {with_drift[-8]}]"
)
self.sync_timestamps = with_drift
# adjust intermediate timestamps. There is a small error between consecutive measurements,
# again due to drift caused by random temperature fluctuation. The error increases with
# increased distance from synchronization points: It is negligible at the start and end
# of the measurement and may be quite high around the middle. That's just the bounds, though --
# you may also have a low error in the middle and error peaks elsewhere.
# As the start and stop timestamps have already been synchronized, we only adjust
# actual transition timestamps here.
if os.getenv("DFATOOL_COMPENSATE_DRIFT"):
with_drift_compensation = self.compensateDrift(with_drift[4:-8])
self.sync_timestamps[4:-8] = with_drift_compensation
def addDrift(self, input_timestamps, end_timestamp, end_offset, start_timestamp):
"""
Add drift to datapoints
:param input_timestamps: List of timestamps (float list)
:param end_timestamp: Timestamp of first EnergyTrace datapoint at the second-to-last sync point
:param end_offset: the time between end_timestamp and the timestamp of synchronisation signal
:param start_timestamp: Timestamp of last EnergyTrace datapoint at the first sync point
:return: List of modified timestamps (float list)
"""
endFactor = 1 + (end_offset / ((end_timestamp - end_offset) - start_timestamp))
# endFactor assumes that the end of the first sync pulse is at timestamp 0.
# Then, timestamps with drift := timestamps * endFactor.
# As this is not the case (the first sync pulse ends at start_timestamp > 0), we shift the data by first
# removing start_timestamp, then multiplying with endFactor, and then re-adding the start_timestamp.
sync_timestamps_with_drift = (
input_timestamps - start_timestamp
) * endFactor + start_timestamp
return sync_timestamps_with_drift
def compensateDrift(self, sync_timestamps):
from dfatool.pelt import PELT
pelt = PELT(min_dist=5, with_multiprocessing=False)
expected_transition_start_timestamps = sync_timestamps[::2]
transition_start_candidate_weights = list()
compensated_timestamps = list()
drift = 0
for i, expected_start_ts in enumerate(expected_transition_start_timestamps):
# assumption: maximum deviation between expected and actual timestamps is 5ms.
# We use ±10ms to have some contetx for PELT
et_timestamps_start = bisect_left(
self.et_timestamps, expected_start_ts - 10e-3
)
et_timestamps_end = bisect_right(
self.et_timestamps, expected_start_ts + 10e-3
)
timestamps = self.et_timestamps[et_timestamps_start : et_timestamps_end + 1]
energy_data = self.et_power_values[
et_timestamps_start : et_timestamps_end + 1
]
candidate_weight = dict()
for penalty in (1, 2, 5, 10, 15, 20):
for changepoint in pelt.get_changepoints(energy_data, penalty=penalty):
if changepoint in candidate_weight:
candidate_weight[changepoint] += 1
else:
candidate_weight[changepoint] = 1
transition_start_candidate_weights.append(
list(
map(
lambda k: (timestamps[k], candidate_weight[k]),
candidate_weight.keys(),
)
)
)
"""
# drift between expected and actual / estimated start timestamps at the previous transition.
# For the first transition, the "previous transition" is the led sync pulse, which has already
# been adjusted, so we have a guaranteed drift of 0.
drift = 0
for i, expected_start_ts in enumerate(expected_transition_start_timestamps):
# assumption: after adjusting for the previous drift, the actual start timestamp is ± 1 ms away.
expected_start_ts += drift
"""
candidates = sorted(
map(lambda x: x[0], transition_start_candidate_weights[i])
)
expected_start_ts += drift
expected_end_ts = sync_timestamps[i * 2 + 1] + drift
right_sync = bisect_left(candidates, expected_start_ts)
left_sync = right_sync - 1
if left_sync > 0:
left_diff = expected_start_ts - candidates[left_sync]
else:
left_diff = None
if right_sync < len(candidates):
right_diff = candidates[right_sync] - expected_start_ts
else:
right_diff = None
if left_diff is None and right_diff is None:
# compensated_timestamps.append(None)
# compensated_timestamps.append(None)
compensated_timestamps.append(expected_start_ts)
compensated_timestamps.append(expected_end_ts)
continue
if right_diff is None and left_diff < 5e-4:
print(expected_start_ts, drift, -left_diff)
compensated_timestamps.append(expected_start_ts - left_diff)
compensated_timestamps.append(expected_end_ts - left_diff)
drift -= left_diff
continue
if left_diff is None and right_diff < 5e-4:
print(expected_start_ts, drift, right_diff)
compensated_timestamps.append(expected_start_ts + right_diff)
compensated_timestamps.append(expected_end_ts + right_diff)
drift += right_diff
continue
if left_diff is not None and right_diff is not None:
if left_diff < right_diff and left_diff < 1e-3:
print(expected_start_ts, drift, -left_diff)
compensated_timestamps.append(expected_start_ts - left_diff)
compensated_timestamps.append(expected_end_ts - left_diff)
drift -= left_diff
continue
if right_diff < left_diff and right_diff < 1e-3:
print(expected_start_ts, drift, right_diff)
compensated_timestamps.append(expected_start_ts + right_diff)
compensated_timestamps.append(expected_end_ts + right_diff)
drift += right_diff
continue
# compensated_timestamps.append(None)
# compensated_timestamps.append(None)
compensated_timestamps.append(expected_start_ts)
compensated_timestamps.append(expected_end_ts)
# TODO calculate drift for "None" timestamps based on the previous and next known drift value
if os.getenv("DFATOOL_EXPORT_DRIFT_COMPENSATION"):
import json
from dfatool.utils import NpEncoder
with open(os.getenv("DFATOOL_EXPORT_DRIFT_COMPENSATION"), "w") as f:
json.dump(
[
expected_transition_start_timestamps,
transition_start_candidate_weights,
],
f,
cls=NpEncoder,
)
return compensated_timestamps
def export_sync(self):
# [1st trans start, 1st trans stop, 2nd trans start, 2nd trans stop, ...]
sync_timestamps = list()
for i in range(4, len(self.sync_timestamps) - 8, 2):
sync_timestamps.append(
(self.sync_timestamps[i], self.sync_timestamps[i + 1])
)
# EnergyTrace timestamps
timestamps = self.et_timestamps
# EnergyTrace power values
power = self.et_power_values
return {"sync": sync_timestamps, "timestamps": timestamps, "power": power}
def plot(self, annotateData=None):
"""
Plots the power usage and the timestamps by logic analyzer
:param annotateData: List of Strings with labels, only needed if annotated plots are wished
:return: None
"""
def calculateRectangleCurve(timestamps, min_value=0, max_value=0.160):
import numpy as np
data = []
for ts in timestamps:
data.append(ts)
data.append(ts)
a = np.empty((len(data),))
a[0::4] = min_value
a[1::4] = max_value
a[2::4] = max_value
a[3::4] = min_value
return data, a # plotting by columns
import matplotlib.pyplot as plt
fig, ax = plt.subplots()
if annotateData:
annot = ax.annotate(
"",
xy=(0, 0),
xytext=(20, 20),
textcoords="offset points",
bbox=dict(boxstyle="round", fc="w"),
arrowprops=dict(arrowstyle="->"),
)
annot.set_visible(True)
rectCurve_with_drift = calculateRectangleCurve(
self.sync_timestamps, max_value=max(self.et_power_values)
)
plt.plot(self.et_timestamps, self.et_power_values, label="Leistung")
plt.plot(self.et_timestamps, np.gradient(self.et_power_values), label="dP/dt")
plt.plot(
rectCurve_with_drift[0],
rectCurve_with_drift[1],
"-g",
label="Synchronisationsignale mit Driftfaktor",
)
plt.xlabel("Zeit von EnergyTrace [s]")
plt.ylabel("Leistung [W]")
leg = plt.legend()
def getDataText(x):
# print(x)
dl = len(annotateData)
for i, xt in enumerate(self.sync_timestamps):
if xt > x and i >= 4 and i - 5 < dl:
return f"SoT: {annotateData[i - 5]}"
def update_annot(x, y, name):
annot.xy = (x, y)
text = name
annot.set_text(text)
annot.get_bbox_patch().set_alpha(0.4)
def hover(event):
if event.xdata and event.ydata:
annot.set_visible(False)
update_annot(event.xdata, event.ydata, getDataText(event.xdata))
annot.set_visible(True)
fig.canvas.draw_idle()
if annotateData:
fig.canvas.mpl_connect("motion_notify_event", hover)
plt.show()
def getStatesdfatool(self, state_sleep, with_traces=False, algorithm=False):
"""
Calculates the length and energy usage of the states
:param state_sleep: Length in seconds of one state, needed for cutting out the UART Sending cycle
:param algorithm: possible usage of accuracy algorithm / not implemented yet
:returns: returns list of states and transitions, starting with a transition and ending with astate
Each element is a dict containing:
* `isa`: 'state' or 'transition'
* `W_mean`: Mittelwert der Leistungsaufnahme
* `W_std`: Standardabweichung der Leistungsaufnahme
* `s`: Dauer
"""
if algorithm:
raise NotImplementedError
end_transition_ts = None
timestamps_sync_start = 0
energy_trace_new = list()
# sync_timestamps[3] is the start of the first (UNINITIALIZED) state (and the end of the benchmark-start sync pulse)
# sync_timestamps[-8] is the end of the final state and the corresponding UART dump (and the start of the benchmark-end sync pulses)
self.trigger_high_precision_timestamps = self.sync_timestamps[3:-7]
self.trigger_edges = list()
for ts in self.trigger_high_precision_timestamps:
# Let ts be the trigger timestamp corresponding to the end of a transition.
# We are looking for an index i such that et_timestamps[i-1] <= ts < et_timestamps[i].
# Then, et_power_values[i] (the mean power in the interval et_timestamps[i-1] .. et_timestamps[i]) is affected by the transition and
# et_power_values[i+1] is not affected by it.
#
# bisect_right does just what we need; bisect_left would correspond to et_timestamps[i-1] < ts <= et_timestamps[i].
# Not that this is a moot point in practice, as ts ≠ et_timestamps[j] for almost all j. Also, the resolution of
# et_timestamps is several decades lower than the resolution of trigger_high_precision_timestamps.
self.trigger_edges.append(bisect_right(self.et_timestamps, ts))
# Loop over transitions. We start at the end of the first transition and handle the transition and the following state.
# We then proceed to the end of the second transition, etc.
for i in range(2, len(self.trigger_high_precision_timestamps), 2):
prev_state_start_index = self.trigger_edges[i - 2]
prev_state_stop_index = self.trigger_edges[i - 1]
transition_start_index = self.trigger_edges[i - 1]
transition_stop_index = self.trigger_edges[i]
state_start_index = self.trigger_edges[i]
state_stop_index = self.trigger_edges[i + 1]
# If a transition takes less time than the energytrace measurement interval, its start and stop index may be the same.
# In this case, et_power_values[transition_start_index] is the only data point affected by the transition.
# We use the et_power_values slice [transition_start_index, transition_stop_index) to determine the mean power, so we need
# to increment transition_stop_index by 1 to end at et_power_values[transition_start_index]
# (as et_power_values[transition_start_index : transition_start_index+1 ] == [et_power_values[transition_start_index])
if transition_stop_index == transition_start_index:
transition_stop_index += 1
prev_state_duration = (
self.trigger_high_precision_timestamps[i + 1]
- self.trigger_high_precision_timestamps[i]
)
transition_duration = (
self.trigger_high_precision_timestamps[i]
- self.trigger_high_precision_timestamps[i - 1]
)
state_duration = (
self.trigger_high_precision_timestamps[i + 1]
- self.trigger_high_precision_timestamps[i]
)
# some states are followed by a UART dump of log data. This causes an increase in CPU energy
# consumption and is not part of the peripheral behaviour, so it should not be part of the benchmark results.
# If a case is followed by a UART dump, its duration is longer than the sleep duration between two transitions.
# In this case, we re-calculate the stop index, and calculate the state duration from coarse energytrace data
# instead of high-precision sync data
if (
self.et_timestamps[prev_state_stop_index]
- self.et_timestamps[prev_state_start_index]
> state_sleep
):
prev_state_stop_index = bisect_right(
self.et_timestamps,
self.et_timestamps[prev_state_start_index] + state_sleep,
)
prev_state_duration = (
self.et_timestamps[prev_state_stop_index]
- self.et_timestamps[prev_state_start_index]
)
if (
self.et_timestamps[state_stop_index]
- self.et_timestamps[state_start_index]
> state_sleep
):
state_stop_index = bisect_right(
self.et_timestamps,
self.et_timestamps[state_start_index] + state_sleep,
)
state_duration = (
self.et_timestamps[state_stop_index]
- self.et_timestamps[state_start_index]
)
prev_state_power = self.et_power_values[
prev_state_start_index:prev_state_stop_index
]
transition_timestamps = self.et_timestamps[
transition_start_index:transition_stop_index
]
transition_power = self.et_power_values[
transition_start_index:transition_stop_index
]
state_timestamps = self.et_timestamps[state_start_index:state_stop_index]
state_power = self.et_power_values[state_start_index:state_stop_index]
transition = {
"isa": "transition",
"W_mean": np.mean(transition_power),
"W_std": np.std(transition_power),
"s": transition_duration,
"count_dp": len(transition_power),
}
if with_traces:
transition["plot"] = (
transition_timestamps - transition_timestamps[0],
transition_power,
)
state = {
"isa": "state",
"W_mean": np.mean(state_power),
"W_std": np.std(state_power),
"s": state_duration,
}
if with_traces:
state["plot"] = (state_timestamps - state_timestamps[0], state_power)
transition["W_mean_delta_prev"] = transition["W_mean"] - np.mean(
prev_state_power
)
transition["W_mean_delta_next"] = transition["W_mean"] - state["W_mean"]
energy_trace_new.append(transition)
energy_trace_new.append(state)
return energy_trace_new
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