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gfuse
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*.pyc
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cmake_minimum_required(VERSION 2.8.3)
project(svo_analysis)
find_package(catkin REQUIRED COMPONENTS rospy)
include_directories(${catkin_INCLUDE_DIRS})
catkin_python_setup()
#catkin_package(CATKIN_DEPENDS sensor_msgs)
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## SVO Analysis
#### Download Test Data
Create a folder where you will store all datasets, e.g.:
mkdir Datasets
In your `.bashrc` script, create a new environment variable pointing to the dataset folder:
export SVO_DATASET_DIR=${HOME}/Datasets
Source your new `.bashrc` script, go to the new dataset folder and download the test data:
source ~/.bashrc
cd ${SVO_DATASET_DIR}
wget http://rpg.ifi.uzh.ch/datasets/sin2_tex2_h1_v8_d.tar.gz -O - | tar -xz
#### Run Benchmark
In the _CMakeLists.txt_ of SVO you need to set the `TRACE` flag to `TRUE` and recompile SVO.
Afterwards run
rosrun svo_analysis benchmark.py sin2_tex2_h1_v8_d
The script will create a new folder in `svo_analysis/results/`, run svo on the dataset and save the tracefile in this folder and at the end it will run some scripts to generate plots from the tracefile.
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comparison_name: speed
experiment_sets:
- label: 'old'
experiments:
- 20140415_1028_svo_ros_synthetic_speed_1404150920_plane_straight_speed4
- 20140415_1028_svo_ros_synthetic_speed_1404150928_plane_straight_speed5
- 20140415_1028_svo_ros_synthetic_speed_1404150935_plane_straight_speed6
- 20140415_1028_svo_ros_synthetic_speed_1404150940_plane_straight_speed7
- label: 'new'
experiments:
- 20140513_0949_svo_ros_synthetic_speed_1404150920_plane_straight_speed4
- 20140513_0949_svo_ros_synthetic_speed_1404150928_plane_straight_speed5
- 20140513_0949_svo_ros_synthetic_speed_1404150935_plane_straight_speed6
- 20140513_0949_svo_ros_synthetic_speed_1404150940_plane_straight_speed7
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comparison_name: textures
experiment_sets:
- label: 'T1'
experiments:
- 20140516_1449_svo_ros_synthetic_all_str_tex1_h1_v6_d
- 20140516_1449_svo_ros_synthetic_all_str_tex1_h1_v9_d
- 20140516_1449_svo_ros_synthetic_all_str_tex1_h1_v12_d
- label: 'T2'
experiments:
- 20140516_1449_svo_ros_synthetic_all_str_tex2_h1_v6_d
- 20140516_1449_svo_ros_synthetic_all_str_tex2_h1_v9_d
- 20140516_1449_svo_ros_synthetic_all_str_tex2_h1_v12_d
- label: 'T3'
experiments:
- 20140516_1449_svo_ros_synthetic_all_str_tex3_h1_v6_d
- 20140516_1449_svo_ros_synthetic_all_str_tex3_h1_v9_d
- 20140516_1449_svo_ros_synthetic_all_str_tex3_h1_v12_d
# - label: 'T4'
# experiments:
# - 20140516_1449_svo_ros_synthetic_all_str_tex4_h1_v6_d
# - 20140516_1449_svo_ros_synthetic_all_str_tex4_h1_v9_d
# - 20140516_1449_svo_ros_synthetic_all_str_tex4_h1_v12_d
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*.yaml
!.gitignore
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<package>
<name>svo_analysis</name>
<version>0.0.1</version>
<description>
Python scripts to analyse performance of SVO.
</description>
<maintainer email="[email protected]">Christian Forster</maintainer>
<author>Christian Forster</author>
<license>BSD</license>
<buildtool_depend>catkin</buildtool_depend>
<build_depend>rospy</build_depend>
<run_depend>python-rospkg</run_depend>
<run_depend>python-yaml</run_depend>
<run_depend>rospy</run_depend>
</package>
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.gitignore
!.gitignore
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#!/usr/bin/python
"""
Created on Sat Aug 10 18:21:47 2013
@author: Christian Forster
"""
import os
import yaml
import rospkg
import argparse
import time
import vikit_py.cpu_info as cpu_info
import vikit_py.ros_node as ros_node
import evaluate
import shutil
def run_experiment(dataset, params):
# load dataset parameters
params['dataset_directory'] = os.path.join(os.environ['SVO_DATASET_DIR'], dataset)
if not os.path.exists(params['dataset_directory']):
raise Exception("Provided dataset folder does not exist.")
dataset_params_file = os.path.join(params['dataset_directory'], 'dataset_params.yaml')
dataset_params = yaml.load(open(dataset_params_file,'r'))
# load algorithm parameters
algo_params_file = os.path.join(rospkg.RosPack().get_path('svo_ros'),
'param', params['param_settings']+'.yaml')
algo_params = yaml.load(open(algo_params_file,'r'))
# combine all parameters
if 'rig_size' not in dataset_params or dataset_params['rig_size'] == 1:
params = dict(params.items() + algo_params.items() + dataset_params['cam0'].items())
else:
params = dict(params.items() + algo_params.items() + dataset_params.items())
if 'dataset_is_blender' in dataset_params:
params['dataset_is_blender'] = dataset_params['dataset_is_blender']
else:
params['dataset_is_blender'] = False
if 'dataset_first_frame' in dataset_params:
params['dataset_first_frame'] = dataset_params['dataset_first_frame']
else:
params['dataset_first_frame'] = 0
# dump experiment params to file and copy the other parameter files:
params_dump_file = os.path.join(params['trace_dir'],'params.yaml')
with open(params_dump_file,'w') as outfile:
outfile.write(yaml.dump(params, default_flow_style=False))
shutil.copyfile(dataset_params_file,
os.path.join(params['trace_dir'], 'dataset_params.yaml'))
# copy the groundtruth trajectory to the trace dir for later evaluation
if params['dataset_is_blender']:
shutil.copyfile(os.path.join(params['dataset_directory'], 'trajectory_nominal.txt'),
os.path.join(params['trace_dir'], 'groundtruth_matched.txt'))
else:
shutil.copyfile(os.path.join(params['dataset_directory'], 'groundtruth_matched.txt'),
os.path.join(params['trace_dir'], 'groundtruth_matched.txt'))
# execute ros node
node = ros_node.RosNode(args.version, args.executable)
node.run(params)
if __name__=="__main__":
# parse command line
parser = argparse.ArgumentParser(description='''
Runs SVO with the dataset and parameters specified in the provided experiment file.
''')
parser.add_argument('experiment_file', help='experiment file in svo_analysis/experiments folder')
parser.add_argument('--evaluate', help='evaluate tracefile after running SVO', action='store_true')
parser.add_argument('--version', help='version of svo to evaluate', default='svo_ros')
parser.add_argument('--executable', help='the executable to be called', default='benchmark')
args = parser.parse_args()
# load experiment parameters
args.experiment_file = args.experiment_file.replace('.yaml','')
experiment_params_file = os.path.join(rospkg.RosPack().get_path('svo_analysis'),
'experiments', args.experiment_file+'.yaml')
if os.path.exists(experiment_params_file):
experiment_params = yaml.load(open(experiment_params_file, 'r'))
else:
print('experiment file does not exist. run with default setttings')
experiment_params = dict({'experiment_label':'default','param_settings':'vo_fast',
'datasets':list([args.experiment_file])})
params = dict()
params['experiment_label'] = experiment_params['experiment_label']
params['param_settings'] = experiment_params['param_settings']
params['time'] = time.strftime("%Y%m%d_%H%M", time.localtime())
params['platform'] = cpu_info.get_cpu_info()
params['trace_name'] = 'trace'
trace_dirs = list()
for dataset in experiment_params['datasets']:
params['experiment_name'] = params['time']+'_'+args.version+'_'+args.experiment_file+'_'+dataset
params['trace_dir'] = os.path.join(rospkg.RosPack().get_path('svo_analysis'),
'results', params['experiment_name'])
if not os.path.exists(params['trace_dir']):
os.makedirs(params['trace_dir'])
trace_dirs.append(params['trace_dir'])
run_experiment(dataset, params)
# TODO: check if it is a synthetic dataset
for trace in trace_dirs:
evaluate.evaluate_dataset(trace)
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#!/usr/bin/python
import os
import sys
import time
import rospkg
import numpy as np
import matplotlib.pyplot as plt
import yaml
import argparse
from matplotlib import rc
# tell matplotlib to use latex font
rc('font',**{'family':'serif','serif':['Cardo']})
rc('text', usetex=True)
from mpl_toolkits.axes_grid1.inset_locator import zoomed_inset_axes
from mpl_toolkits.axes_grid1.inset_locator import mark_inset
def plot_trajectory(ax, filename, label, color, linewidth):
file = open(filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
trajectory = np.array([[v.strip() for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"], dtype=np.float64)
ax.plot(trajectory[:,1], trajectory[:,2], label=label, color=color, linewidth=linewidth)
def compare_results(experiments, results_dir, comparison_dir,
plot_scale_drift = False):
# ------------------------------------------------------------------------------
# position error
fig_poserr = plt.figure(figsize=(8,6))
ax_poserr_x = fig_poserr.add_subplot(311, ylabel='x-error [m]')
ax_poserr_y = fig_poserr.add_subplot(312, ylabel='y-error [m]')
ax_poserr_z = fig_poserr.add_subplot(313, ylabel='z-error [m]', xlabel='time [s]')
for exp in experiments:
# load dataset parameters
params_stream = open(os.path.join(results_dir, exp, 'params.yaml'))
params = yaml.load(params_stream)
# plot translation error
trans_error = np.loadtxt(os.path.join(results_dir, exp, 'translation_error.txt'))
trans_error[:,0] = trans_error[:,0]-trans_error[0,0]
ax_poserr_x.plot(trans_error[:,0], trans_error[:,1], label=params['experiment_label'])
ax_poserr_y.plot(trans_error[:,0], trans_error[:,2])
ax_poserr_z.plot(trans_error[:,0], trans_error[:,3])
ax_poserr_x.set_xlim([0, trans_error[-1,0]+4])
ax_poserr_y.set_xlim([0, trans_error[-1,0]+4])
ax_poserr_z.set_xlim([0, trans_error[-1,0]+4])
ax_poserr_x.legend(bbox_to_anchor=[0, 0], loc='lower left', ncol=3)
ax_poserr_x.grid()
ax_poserr_y.grid()
ax_poserr_z.grid()
fig_poserr.tight_layout()
fig_poserr.savefig(os.path.join(comparison_dir, 'translation_error.pdf'))
# ------------------------------------------------------------------------------
# orientation error
fig_roterr = plt.figure(figsize=(8,6))
ax_roterr_r = fig_roterr.add_subplot(311, ylabel='roll-error [rad]')
ax_roterr_p = fig_roterr.add_subplot(312, ylabel='pitch-error [rad]')
ax_roterr_y = fig_roterr.add_subplot(313, ylabel='yaw-error [rad]', xlabel='time [s]')
for exp in experiments:
# load dataset parameters
params_stream = open(os.path.join(results_dir, exp, 'params.yaml'))
params = yaml.load(params_stream)
# plot translation error
rot_error = np.loadtxt(os.path.join(results_dir, exp, 'orientation_error.txt'))
rot_error[:,0] = rot_error[:,0]-rot_error[0,0]
ax_roterr_r.plot(rot_error[:,0], rot_error[:,3], label=params['experiment_label'])
ax_roterr_p.plot(rot_error[:,0], rot_error[:,2])
ax_roterr_y.plot(rot_error[:,0], rot_error[:,1])
ax_roterr_r.set_xlim([0, rot_error[-1,0]+4])
ax_roterr_p.set_xlim([0, rot_error[-1,0]+4])
ax_roterr_y.set_xlim([0, rot_error[-1,0]+4])
ax_roterr_r.legend(bbox_to_anchor=[0, 1], loc='upper left', ncol=3)
ax_roterr_r.grid()
ax_roterr_p.grid()
ax_roterr_y.grid()
fig_roterr.tight_layout()
fig_roterr.savefig(os.path.join(comparison_dir, 'orientation_error.pdf'))
# ------------------------------------------------------------------------------
# scale error
if plot_scale_drift:
fig_scale = plt.figure(figsize=(8,2.5))
ax_scale = fig_scale.add_subplot(111, xlabel='time [s]', ylabel='scale change [\%]')
for exp in experiments:
# load dataset parameters
params = yaml.load(open(os.path.join(results_dir, exp, 'params.yaml')))
# plot translation error
scale_drift = open(os.path.join(results_dir, exp, 'scale_drift.txt'))
scale_drift[:,0] = scale_drift[:,0]-scale_drift[0,0]
ax_scale.plot(scale_drift[:,0], scale_drift[:,1], label=params['experiment_label'])
ax_scale.set_xlim([0, rot_error[-1,0]+4])
ax_scale.legend(bbox_to_anchor=[0, 1], loc='upper left', ncol=3)
ax_scale.grid()
fig_scale.tight_layout()
fig_scale.savefig(os.path.join(comparison_dir, 'scale_drift.pdf'))
# ------------------------------------------------------------------------------
# trajectory
# fig_traj = plt.figure(figsize=(8,4.8))
# ax_traj = fig_traj.add_subplot(111, xlabel='x [m]', ylabel='y [m]', aspect='equal', xlim=[-3.1, 4], ylim=[-1.5, 2.6])
#
# plotTrajectory(ax_traj, '/home/cforster/Datasets/asl_vicon_d2/groundtruth_filtered.txt', 'Groundtruth', 'k', 1.5)
# plotTrajectory(ax_traj, results_dir+'/20130911_2229_nslam_i7_asl2_fast/traj_estimate_rotated.txt', 'Fast', 'g', 1)
# plotTrajectory(ax_traj, results_dir+'/20130906_2149_ptam_i7_asl2/traj_estimate_rotated.txt', 'PTAM', 'r', 1)
#
# mark_inset(ax_traj, axins, loc1=2, loc2=4, fc="none", ec='b')
# plt.draw()
# plt.show()
# ax_traj.legend(bbox_to_anchor=[1, 0], loc='lower right', ncol=3)
# ax_traj.grid()
# fig_traj.tight_layout()
# fig_traj.savefig('../results/trajectory_asl.pdf')
if __name__ == '__main__':
default_name = time.strftime("%Y%m%d_%H%M", time.localtime())+'_comparison'
parser = argparse.ArgumentParser(description='Compare results.')
parser.add_argument('result_directories', nargs='+', help='list of result directories to compare')
parser.add_argument('--name', help='name of the comparison', default=default_name)
args = parser.parse_args()
# create folder for comparison results
results_dir = os.path.join(rospkg.RosPack().get_path('svo_analysis'), 'results')
comparison_dir = os.path.join(results_dir, args.name)
if not os.path.exists(comparison_dir):
os.makedirs(comparison_dir)
# run comparison
compare_results(args.result_directories, results_dir, comparison_dir)
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#!/usr/bin/python
import os
import sys
import time
import rospkg
import numpy as np
import matplotlib.pyplot as plt
import yaml
import argparse
import svo_analysis.analyse_depth as analyse_depth
from matplotlib import rc
# tell matplotlib to use latex font
rc('font',**{'family':'serif','serif':['Cardo']})
rc('text', usetex=True)
from mpl_toolkits.axes_grid1.inset_locator import zoomed_inset_axes
from mpl_toolkits.axes_grid1.inset_locator import mark_inset
def plot_trajectory(ax, filename, label, color, linewidth):
file = open(filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
trajectory = np.array([[v.strip() for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"], dtype=np.float64)
ax.plot(trajectory[:,1], trajectory[:,2], label=label, color=color, linewidth=linewidth)
def save_figure(fig, name, directory):
fig.tight_layout()
fig.savefig(os.path.join(directory, name+'.pdf'), bbox_inches="tight")
def distances_along_trajectory(traj):
keys = traj.keys()
keys.sort()
motion = [ominus(traj[keys[i+1]],traj[keys[i]]) for i in range(len(keys)-1)]
distances = [0]
sum = 0
for t in motion:
sum += compute_distance(t)
distances.append(sum)
return distances
def get_distance_from_start(gt):
distances = np.diff(gt[:,1:4],axis=0)
distances = np.sqrt(np.sum(np.multiply(distances,distances),1))
distances = np.cumsum(distances)
distances = np.concatenate(([0], distances))
return distances
def compare_results(comp_params, results_dir, comparison_dir):
print('run comparison: '+comp_params['comparison_name'])
line_styles = ['-','--',':']
line_colors = ['b','g','r','m','c']
# -------------------------------------------------------------------------
# plot trajectory:
fig = plt.figure(figsize=(6,2))
ax = fig.add_subplot(111, xlabel='x [m]', ylabel='y [m]')
for exp_set in comp_params['experiment_sets']:
print('processing experiment set: ' + exp_set['label'])
for i, exp in enumerate(exp_set['experiments']):
data = np.loadtxt(os.path.join(results_dir, exp, 'traj_estimate.txt'))
if i == 0:
base_plot, = ax.plot(data[:,1], data[:,2], label=exp_set['label'], linestyle=line_styles[np.mod(i, len(line_styles))])
else:
ax.plot(data[:,1], data[:,2], color=base_plot.get_color(), linestyle= line_styles[np.mod(i, len(line_styles))])
ax.legend(loc='upper left', ncol=3)
save_figure(fig, 'trajectory', comparison_dir)
# -------------------------------------------------------------------------
# plot translation error:
fig = plt.figure(figsize=(6,2))
ax = fig.add_subplot(111, xlabel='distance [m]', ylabel='translation drift [mm]')
for exp_set in comp_params['experiment_sets']:
print('processing experiment set: ' + exp_set['label'])
for i, exp in enumerate(exp_set['experiments']):
gt = np.loadtxt(os.path.join(results_dir, exp, 'groundtruth_matched.txt'))
distances = get_distance_from_start(gt)
data = np.loadtxt(os.path.join(results_dir, exp, 'translation_error.txt'))
e = np.sqrt(np.sum(np.multiply(data[:,1:4],data[:,1:4]),1))
if np.shape(e)[0] > np.shape(distances)[0]:
print('WARNING: estimate has more measurement than groundtruth: '
+str(np.shape(e)[0]-np.shape(distances)[0]))
e = e[0:np.shape(distances)[0]]
distances = distances[0:np.shape(e)[0]]
print '--'
print np.shape(e)
print np.shape(distances)
if i == 0:
base_plot, = ax.plot(distances, e*1000, label=exp_set['label'], linestyle= line_styles[np.mod(i, len(line_styles))])
else:
ax.plot(distances, e*1000, color=base_plot.get_color(), linestyle= line_styles[np.mod(i, len(line_styles))])
ax.legend(loc='upper left', ncol=3)
save_figure(fig, 'translation_error', comparison_dir)
# -------------------------------------------------------------------------
# plot depth estimation error:
fig = plt.figure(figsize=(6,5))
ax = fig.add_subplot(111, xlabel='Travelled distance [m]', ylabel='Error [m]')
for k, exp_set in enumerate(comp_params['experiment_sets']):
print('plot depth error for experiment: ' + exp)
exp = exp_set['experiments'][0]
gt = np.loadtxt(os.path.join(results_dir, exp, 'groundtruth_matched.txt'))
x_axis_data = get_distance_from_start(gt)
analyse_depth.plot_depth_over_time(os.path.join(results_dir, exp), ax,
x_axis_data[1:], line_colors[k], exp_set['label'])
ax.legend(loc='upper left', ncol=3)
save_figure(fig, 'depth_error_textures', comparison_dir)
fig = plt.figure(figsize=(6,5))
ax = fig.add_subplot(111, xlabel='Travelled distance [m]', ylabel='Error [m]')
exp_set = comp_params['experiment_sets'][0]
for i, exp in enumerate(exp_set['experiments']):
print('plot depth error for speed: ' + exp)
gt = np.loadtxt(os.path.join(results_dir, exp, 'groundtruth_matched.txt'))
x_axis_data = get_distance_from_start(gt)
params = yaml.load(open(os.path.join(results_dir, exp, 'dataset_params.yaml')))
analyse_depth.plot_depth_over_time(os.path.join(results_dir, exp), ax,
x_axis_data[1:], line_colors[i],
str(params['trajectory_modifiers']['speed'])+' m/s')
ax.legend(loc='upper left', ncol=3)
save_figure(fig, 'depth_error_speed', comparison_dir)
if __name__ == '__main__':
parser = argparse.ArgumentParser(description='Compare results of a VO pipeline.')
parser.add_argument('comparison_file', help='A YAML file that contains the details of the comparison')
args = parser.parse_args()
# load comparison file
args.experiment_file = args.comparison_file.replace('.yaml','')
comparison_params_file = os.path.join(rospkg.RosPack().get_path('svo_analysis'),
'comparisons', args.comparison_file+'.yaml')
if os.path.exists(comparison_params_file):
comp_params = yaml.load(open(comparison_params_file, 'r'))
else:
raise Exception("Provided comparison file does not exist.")
# create folder for comparison results
comparison_dir = os.path.join(rospkg.RosPack().get_path('svo_analysis'),
'comparisons', comp_params['comparison_name'])
if not os.path.exists(comparison_dir):
os.makedirs(comparison_dir)
# folder where the results of previous experiments are saved
results_dir = os.path.join(rospkg.RosPack().get_path('svo_analysis'), 'results')
# run comparison
compare_results(comp_params, results_dir, comparison_dir)
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#!/usr/bin/python
"""
Created on Sat Aug 10 18:21:47 2013
@author: Christian Forster
"""
import os
import csv
import numpy as np
import rospkg
import argparse
import yaml
import svo_analysis.analyse_logs as analyse_logs
import svo_analysis.analyse_timing as analyse_timing
import svo_analysis.analyse_trajectory as analyse_trajectory
import svo_analysis.analyse_depth as analyse_depth
def evaluate_dataset(trace_dir):
# read tracefile
data = csv.reader(open(os.path.join(trace_dir, 'trace.csv')))
fields = data.next()
D = dict()
for field in fields:
D[field] = list()
# fill dictionary with column values
for row in data:
for (field, value) in zip(fields, row):
D[field].append(float(value))
# change dictionary values from list to numpy array for easier manipulation
for field, value in D.items():
D[field] = np.array(D[field])
# generate plots
analyse_logs.analyse_logs(D, trace_dir)
analyse_timing.analyse_timing(D, trace_dir)
analyse_trajectory.analyse_trajectory(trace_dir)
param = yaml.load(open(os.path.join(trace_dir, 'dataset_params.yaml'), 'r'))
if param['dataset_is_blender']:
analyse_depth.analyse_depth(trace_dir)
analyse_depth.analyse_depth_over_time(trace_dir)
if __name__=="__main__":
parser = argparse.ArgumentParser(description='''
Evaluates tracefiles of SVO and generates the plots.
''')
parser.add_argument('experiment_name', help='directory name of the tracefiles')
args = parser.parse_args()
trace_dir = os.path.join(rospkg.RosPack().get_path('svo_analysis'),
'results',
args.experiment_name)
evaluate_dataset(trace_dir)
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#!/usr/bin/env python
from distutils.core import setup
from catkin_pkg.python_setup import generate_distutils_setup
d = generate_distutils_setup(
packages=['svo_analysis'],
package_dir={'': 'src'},
install_requires=['rospkg', 'yaml'],
)
setup(**d)
@@ -0,0 +1,41 @@
# -*- coding: utf-8 -*-
import associate
import numpy as np
import matplotlib.pyplot as plt
import yaml
def loadDataset(filename):
file = open(filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
D = np.array([[v.strip() for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"], dtype=np.float64)
return D
dataset_dir = '/home/cforster/Datasets/SlamBenchmark/px4_r2'
trajectory_data = dataset_dir+'/groundtruth.txt'
stepsize = 10
# load dataset
data = loadDataset(trajectory_data)
n = data.shape[0]
steps = np.arange(0,n,stepsize)
# compute trajectory length
last_pos = data[0,1:4]
trajectory_length = 0
for i in steps[1:]:
new_pos = data[i,1:4]
trajectory_length += np.linalg.norm(new_pos-last_pos)
last_pos = new_pos
print 'trajectory lenght = ' + str(trajectory_length) + 'm'
print 'height mean = ' + str(np.mean(data[:,3])) + 'm'
print 'height median = ' + str(np.median(data[:,3])) + 'm'
print 'height std = ' + str(np.std(data[:,3])) + 'm'
print 'duration = ' + str(data[-1,0]-data[0,0]) + 's'
print 'speed = ' + str(trajectory_length/(data[-1,0]-data[0,0])) + 'm/s'
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#!/usr/bin/python
import os
import argparse
import numpy as np
import matplotlib.pyplot as plt
from matplotlib import rc
rc('font',**{'family':'serif','serif':['Cardo']})
rc('text', usetex=True)
def precision_plot(ax, errors, max_error, color, linestyle):
number_of_error_ranges = 500
error_step = max_error / number_of_error_ranges
precision_array = np.zeros(number_of_error_ranges)
error_array = np.zeros(number_of_error_ranges)
n_measurements = len(errors)
for error_ind in range(0, number_of_error_ranges):
precision_array[error_ind] = np.sum(errors < error_step*error_ind) / float(n_measurements) * 100.0
error_array[error_ind] = error_step*error_ind
plot_obj, = ax.plot(error_array, precision_array, label='error', linestyle=linestyle, color=color)
return plot_obj
def analyse_depth(results_dir):
D = np.loadtxt(os.path.join(results_dir, 'depth_error.txt'), delimiter=' ')
D = D[D[:,0] > 1,:]
fig = plt.figure(figsize=(6,5))
ax = fig.add_subplot(111, xlabel='depth error [m]', ylabel='Precision [\%]')
errors = np.abs(D[:,1])
precision_plot(ax, errors, 0.05, 'r', '-')
fig.tight_layout()
fig.savefig(os.path.join(results_dir,'depth_error.pdf'), bbox_inches="tight")
def plot_depth_over_time(results_dir, ax, x_axis_data, color, label=''):
D = np.loadtxt(os.path.join(results_dir, 'depth_error.txt'), delimiter=' ')
D = D[D[:,0] > 1,:]
idxs = np.unique(D[:,0])
percentile_10 = np.zeros(len(idxs))
percentile_50 = np.zeros(len(idxs))
percentile_90 = np.zeros(len(idxs))
for i in range(len(idxs)):
errors = np.abs(D[D[:,0]==idxs[i],1])
percentile_10[i] = np.percentile(errors, 10)
percentile_50[i] = np.percentile(errors, 50)
percentile_90[i] = np.percentile(errors, 90)
if len(x_axis_data) == 0:
x_axis_data = idxs
print np.shape(x_axis_data)
print np.shape(idxs)
print '--'
ax.plot(x_axis_data, percentile_50, linewidth=2, color=color, label=label)
ax.plot(x_axis_data, percentile_10, linewidth=0.5, color=color, alpha=0.5)
ax.plot(x_axis_data, percentile_90, linewidth=0.5, color=color, alpha=0.5)
ax.fill_between(x_axis_data, percentile_10, percentile_90, color=color, alpha=0.1)
if __name__ == '__main__':
parser = argparse.ArgumentParser(description='Analyse depth estimate')
parser.add_argument('results_dir', help='folder with the results')
args = parser.parse_args()
analyse_depth(args.results_dir)
fig = plt.figure(figsize=(6,5))
ax = fig.add_subplot(111, xlabel='Measurement', ylabel='Scale-Drift')
plot_depth_over_time(args.results_dir, [], ax)
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#!/usr/bin/python
import os
import yaml
import numpy as np
import matplotlib.pyplot as plt
def analyse_logs(D, trace_dir):
# identify measurements which result from normal frames and which from keyframes
is_kf = np.argwhere( (D['dropout'] == 1) & (D['repr_n_mps'] >= 0))
is_frame = np.argwhere(D['repr_n_mps'] >= 0)
is_nokf = np.argwhere( (D['dropout'] == 0) & (D['repr_n_mps'] >= 0))
# set initial time to zero
D['timestamp'] = D['timestamp'] - D['timestamp'][0]
# ----------------------------------------------------------------------------
# plot number of reprojected points
mean_n_reproj_points = np.mean(D['repr_n_mps'][is_frame]);
mean_n_reproj_matches = np.mean(D['repr_n_new_references'][is_frame]);
mean_n_edges_final = np.mean(D['sfba_n_edges_final'][is_frame]);
fig = plt.figure(figsize=(8,3))
ax = fig.add_subplot(111, xlabel='time [s]')
ax.plot(D['timestamp'][is_frame], D['repr_n_mps'][is_frame], 'r-',
label='Reprojected Points, avg = %.2f'%mean_n_reproj_points)
ax.plot(D['timestamp'][is_frame], D['repr_n_new_references'][is_frame], 'b-',
label='Feature Matches, avg = %.2f'%mean_n_reproj_matches)
ax.plot(D['timestamp'][is_frame], D['sfba_n_edges_final'][is_frame], 'g-',
label='Points after Optimization, avg = %.2f'%mean_n_edges_final)
ax.set_ylim(bottom=0)
ax.legend(loc='lower right')
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'num_reprojected.pdf'), bbox_inches="tight")
# ----------------------------------------------------------------------------
# plot median error before and after pose-optimzation and bundle adjustment
init_error_avg = np.mean(D['sfba_error_init'][is_frame])
opt1_avg = np.mean(D['sfba_error_final'][is_frame])
fig = plt.figure(figsize=(8,2))
ax = fig.add_subplot(111, xlabel='time [s]', ylabel='error [px]')
ax.plot(D['timestamp'][is_frame], D['sfba_error_init'][is_frame], 'r-', label='Initial error')
ax.plot(D['timestamp'][is_frame], D['sfba_error_final'][is_frame], 'b-', label='Final error')
ax.legend(ncol=2)
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'reprojection_error.pdf'), bbox_inches="tight")
print 'average reprojection error improvement: ' + str(init_error_avg - opt1_avg)
# ----------------------------------------------------------------------------
# plot number of candidate points
fig = plt.figure(figsize=(8,3))
ax = fig.add_subplot(111, xlabel='time [s]')
ax.plot(D['timestamp'][is_frame], D['n_candidates'][is_frame], 'r-', label='Candidate Points')
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'candidate_points.pdf'), bbox_inches="tight")
# ----------------------------------------------------------------------------
# plot number of candidate points
fig = plt.figure(figsize=(8,2))
ax = fig.add_subplot(111, xlabel='time [s]', ylabel='px')
ax.plot(D['timestamp'][is_frame], D['sfba_thresh'][is_frame], 'r-', label='Threshold')
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'optimization_thresh.pdf'), bbox_inches="tight")
# ----------------------------------------------------------------------------
# write other statistics to file
stat = {'num_frames': len(is_frame),
'num_kfs': len(is_kf),
'reproj_error_avg_improvement': float(init_error_avg - opt1_avg)}
with open(os.path.join(trace_dir,'dataset_stats.yaml'),'w') as outfile:
outfile.write(yaml.dump(stat, default_flow_style=False))
@@ -0,0 +1,68 @@
#!/usr/bin/python
import os
import numpy as np
import matplotlib.pyplot as plt
def analyse_timing(D, trace_dir):
# identify measurements which result from normal frames and which from keyframes
is_frame = np.argwhere(D['repr_n_mps'] >= 0)
n_frames = len(is_frame)
# set initial time to zero
D['timestamp'] = D['timestamp'] - D['timestamp'][0]
# ----------------------------------------------------------------------------
# plot total time for frame processing
avg_time = np.mean(D['tot_time'][is_frame])*1000;
fig = plt.figure(figsize=(8, 3))
ax = fig.add_subplot(111, ylabel='processing time [ms]', xlabel='time [s]')
ax.plot(D['timestamp'][is_frame], D['tot_time'][is_frame]*1000, 'g-', label='total time [ms]')
ax.plot(D['timestamp'][is_frame], np.ones(n_frames)*avg_time, 'b--', label=str('%(time).1fms mean time' % {'time': avg_time}))
ax.legend()
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'timing.pdf'), bbox_inches="tight")
# ----------------------------------------------------------------------------
# plot boxplot
fig = plt.figure(figsize=(6,2))
ax = fig.add_subplot(111, xlabel='Processing time [ms]')
ax.boxplot([
D['tot_time'][is_frame]*1000,
# D['t_local_ba'][is_kf]*1000,
D['pose_optimizer'][is_frame]*1000 + D['point_optimizer'][is_frame]*1000,
D['reproject'][is_frame]*1000,
D['sparse_img_align'][is_frame]*1000,
D['pyramid_creation'][is_frame]*1000
], 0,'', vert=0)
boxplot_labels = [
r'\textbf{Total Motion Estimation: %2.2fms}' % np.median(D['tot_time'][is_frame]*1000),
# 'Local BA (KF only): %.2fms ' % np.median(D['local_ba'][is_kf]*1000),
'Refinement: %2.2fms' % np.median(D['pose_optimizer'][is_frame]*1000 + D['point_optimizer'][is_frame]*1000),
'Feature Alignment: %2.2fms' % np.median(D['reproject'][is_frame]*1000),
'Sparse Image Alignment: %2.2fms' % np.median(D['sparse_img_align'][is_frame]*1000),
'Pyramid Creation: %2.2fms' % np.median(D['pyramid_creation'][is_frame]*1000) ]
ax.set_yticks(np.arange(len(boxplot_labels))+1)
ax.set_yticklabels(boxplot_labels)
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'timing_boxplot.pdf'), bbox_inches="tight")
# ----------------------------------------------------------------------------
# plot boxplot reprojection
fig = plt.figure(figsize=(6,2))
ax = fig.add_subplot(111, xlabel='Processing time [ms]')
ax.boxplot([ D['reproject'][is_frame]*1000,
D['feature_align'][is_frame]*1000,
D['reproject_candidates'][is_frame]*1000,
D['reproject_kfs'][is_frame]*1000 ], 0, '', vert=0)
boxplot_labels = [r'\textbf{Total Reprojection: %2.2fms}' % np.median(D['reproject'][is_frame]*1000),
'Feature Alignment: %2.2fms' % np.median(D['feature_align'][is_frame]*1000),
'Reproject Candidates: %2.2fms' % np.median(D['reproject_candidates'][is_frame]*1000),
'Reproject Keyframes: %2.2fms' % np.median(D['reproject_kfs'][is_frame]*1000) ]
ax.set_yticks(np.arange(len(boxplot_labels))+1)
ax.set_yticklabels(boxplot_labels)
fig.tight_layout()
fig.savefig(os.path.join(trace_dir,'timing_reprojection.pdf'), bbox_inches="tight")
@@ -0,0 +1,185 @@
#!/usr/bin/python
import os
import yaml
import argparse
import numpy as np
import matplotlib.pyplot as plt
import svo_analysis.tum_benchmark_tools.associate as associate
import vikit_py.transformations as transformations
import vikit_py.align_trajectory as align_trajectory
from matplotlib import rc
rc('font',**{'family':'serif','serif':['Cardo']})
rc('text', usetex=True)
def plot_translation_error(timestamps, translation_error, results_dir):
fig = plt.figure(figsize=(8, 2.5))
ax = fig.add_subplot(111, xlabel='time [s]', ylabel='position drift [mm]', xlim=[0,timestamps[-1]-timestamps[0]+4])
ax.plot(timestamps-timestamps[0], translation_error[:,0]*1000, 'r-', label='x')
ax.plot(timestamps-timestamps[0], translation_error[:,1]*1000, 'g-', label='y')
ax.plot(timestamps-timestamps[0], translation_error[:,2]*1000, 'b-', label='z')
ax.legend()
fig.tight_layout()
fig.savefig(results_dir+'/translation_error.pdf')
def plot_rotation_error(timestamps, rotation_error, results_dir):
fig = plt.figure(figsize=(8, 2.5))
ax = fig.add_subplot(111, xlabel='time [s]', ylabel='orientation drift [rad]', xlim=[0,timestamps[-1]-timestamps[0]+4])
ax.plot(timestamps-timestamps[0], rotation_error[:,0], 'r-', label='yaw')
ax.plot(timestamps-timestamps[0], rotation_error[:,1], 'g-', label='pitch')
ax.plot(timestamps-timestamps[0], rotation_error[:,2], 'b-', label='roll')
ax.legend()
fig.tight_layout()
fig.savefig(results_dir+'/orientation_error.pdf')
def analyse_synthetic_trajectory(results_dir):
data = np.loadtxt(os.path.join(results_dir, 'translation_error.txt'))
timestamps = data[:,0]
translation_error = data[:,1:4]
plot_translation_error(timestamps, translation_error, results_dir)
# plot orientation error
data = np.loadtxt(os.path.join(results_dir, 'orientation_error.txt'))
timestamps = data[:,0]
orientation_error = data[:,1:4]
plot_rotation_error(timestamps, orientation_error, results_dir)
def analyse_optitrack_trajectory_with_hand_eye_calib(results_dir, params, n_align_frames = 200):
print('loading hand-eye-calib')
T_cm_quat = np.array([params['hand_eye_calib']['Tcm_qx'],
params['hand_eye_calib']['Tcm_qy'],
params['hand_eye_calib']['Tcm_qz'],
params['hand_eye_calib']['Tcm_qw']])
T_cm_tran = np.array([params['hand_eye_calib']['Tcm_tx'],
params['hand_eye_calib']['Tcm_ty'],
params['hand_eye_calib']['Tcm_tz']])
T_cm = get_rigid_body_trafo(T_cm_quat, T_cm_tran)
T_mc = transformations.inverse_matrix(T_cm)
t_es, p_es, q_es, t_gt, p_gt, q_gt = load_dataset(results_dir, params['cam_delay'])
# align Sim3 to get scale
print('align Sim3 using '+str(n_align_frames)+' first frames.')
scale,rot,trans = align_trajectory.align_sim3(p_gt[0:n_align_frames,:], p_es[0:n_align_frames,:])
print 'scale = '+str(scale)
# get trafo between (v)ision and (o)ptitrack frame
print q_gt[0,:]
print p_gt[0,:]
T_om = get_rigid_body_trafo(q_gt[0,:], p_gt[0,:])
T_vc = get_rigid_body_trafo(q_es[0,:], scale*p_es[0,:])
T_cv = transformations.inverse_matrix(T_vc)
T_ov = np.dot(T_om, np.dot(T_mc, T_cv))
print 'T_ov = ' + str(T_ov)
# apply transformation to estimated trajectory
q_es_aligned = np.zeros(np.shape(q_es))
rpy_es_aligned = np.zeros(np.shape(p_es))
rpy_gt = np.zeros(np.shape(p_es))
p_es_aligned = np.zeros(np.shape(p_es))
for i in range(np.shape(p_es)[0]):
T_vc = get_rigid_body_trafo(q_es[i,:],p_es[i,:])
T_vc[0:3,3] *= scale
T_om = np.dot(T_ov, np.dot(T_vc, T_cm))
p_es_aligned[i,:] = T_om[0:3,3]
q_es_aligned[i,:] = transformations.quaternion_from_matrix(T_om)
rpy_es_aligned[i,:] = transformations.euler_from_quaternion(q_es_aligned[i,:], 'rzyx')
rpy_gt[i,:] = transformations.euler_from_quaternion(q_gt[i,:], 'rzyx')
# plot position error (drift)
translation_error = (p_gt-p_es_aligned)
plot_translation_error(t_es, translation_error, results_dir)
# plot orientation error (drift)
orientation_error = (rpy_gt - rpy_es_aligned)
plot_rotation_error(t_es, orientation_error, results_dir)
# plot scale drift
motion_gt = np.diff(p_gt, 0)
motion_es = np.diff(p_es_aligned, 0)
dist_gt = np.sqrt(np.sum(np.multiply(motion_gt,motion_gt),1))
dist_es = np.sqrt(np.sum(np.multiply(motion_es,motion_es),1))
fig = plt.figure(figsize=(8,2.5))
ax = fig.add_subplot(111, xlabel='time [s]', ylabel='scale change [\%]', xlim=[0,t_es[-1]+4])
scale_drift = np.divide(dist_es,dist_gt)*100-100
ax.plot(t_es, scale_drift, 'b-')
fig.tight_layout()
fig.savefig(results_dir+'/scale_drift.pdf')
# plot trajectory
fig = plt.figure()
ax = fig.add_subplot(111, title='trajectory', aspect='equal', xlabel='x [m]', ylabel='y [m]')
ax.plot(p_es_aligned[:,0], p_es_aligned[:,1], 'b-', label='estimate')
ax.plot(p_gt[:,0], p_gt[:,1], 'r-', label='groundtruth')
ax.plot(p_es_aligned[0:n_align_frames,0], p_es_aligned[0:n_align_frames,1], 'g-', linewidth=2, label='aligned')
ax.legend()
fig.tight_layout()
fig.savefig(results_dir+'/trajectory.pdf')
def analyse_trajectory(results_dir, n_align_frames = 200, use_hand_eye_calib = True):
params = yaml.load(open(os.path.join(results_dir, 'dataset_params.yaml'),'r'))
if params['dataset_is_blender']:
analyse_synthetic_trajectory(results_dir)
elif use_hand_eye_calib:
analyse_optitrack_trajectory_with_hand_eye_calib(results_dir, params, n_align_frames)
else:
t_es, p_es, q_es, t_gt, p_gt, q_gt = load_dataset(results_dir, params['cam_delay'])
scale,rot,trans = align_trajectory.align_sim3(p_gt[0:n_align_frames,:], p_es[0:n_align_frames,:])
p_es_aligned = np.zeros(np.shape(p_es))
for i in range(np.shape(p_es)[0]):
p_es_aligned[i,:] = scale*rot.dot(p_es[i,:]) + trans
# plot position error (drift)
translation_error = (p_gt-p_es_aligned)
plot_translation_error(t_es, translation_error, results_dir)
def get_rigid_body_trafo(quat,trans):
T = transformations.quaternion_matrix(quat)
T[0:3,3] = trans
return T
def load_dataset(results_dir, cam_delay):
print('loading dataset in '+results_dir)
print('cam_delay = '+str(cam_delay))
data_gt = open(os.path.join(results_dir, 'groundtruth.txt')).read()
lines = data_gt.replace(","," ").replace("\t"," ").split("\n")
data_gt = np.array([[np.float(v.strip()) for i,v in enumerate(line.split(" ")) if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"])
#data_gt = np.array([[np.float(v.strip()) for i,v in enumerate(line.split(" ")) if i != 1 and v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"])
data_gt = [(float(l[0]),l[1:]) for l in data_gt]
data_gt = dict(data_gt)
data_es = open(os.path.join(results_dir, 'traj_estimate.txt')).read()
lines = data_es.replace(","," ").replace("\t"," ").split("\n")
data_es = np.array([[np.float(v.strip()) for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"])
data_es = [(float(l[0]),l[1:]) for l in data_es]
data_es = dict(data_es)
matches = associate.associate(data_gt, data_es, -cam_delay, 0.02)
p_gt = np.array([[np.float(value) for value in data_gt[a][0:3]] for a,b in matches])
q_gt = np.array([[np.float(value) for value in data_gt[a][3:7]] for a,b in matches])
p_es = np.array([[np.float(value) for value in data_es[b][0:3]] for a,b in matches])
q_es = np.array([[np.float(value) for value in data_es[b][3:7]] for a,b in matches])
t_gt = np.array([np.float(a) for a,b in matches])
t_es = np.array([np.float(b) for a,b in matches])
# set start time to zero
start_time = min(t_es[0], t_gt[0])
t_es -= start_time
t_gt -= start_time
return t_es, p_es, q_es, t_gt, p_gt, q_gt
if __name__ == '__main__':
# parse command line
parser = argparse.ArgumentParser(description='''
Analyse trajectory
''')
parser.add_argument('results_dir', help='folder with the results')
parser.add_argument('--use_hand_eye_calib', help='', action='store_true')
parser.add_argument('--n_align_frames', help='', default=200)
args = parser.parse_args()
print('analyse trajectory for dataset: '+str(args.results_dir))
analyse_trajectory(args.results_dir,
n_align_frames = int(args.n_align_frames),
use_hand_eye_calib = args.use_hand_eye_calib)
@@ -0,0 +1,60 @@
#!/usr/bin/python
import numpy as np
import matplotlib.pyplot as plt
import transformations
from scipy import signal
save = True
data_filename = '/home/cforster/Datasets/SlamBenchmark/asl_vicon_d2/groundtruth.txt'
filtered_data_filename = '/home/cforster/Datasets/SlamBenchmark/asl_vicon_d2/groundtruth_filtered.txt'
file = open(data_filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
D = np.array([[v.strip() for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"], dtype=np.float64)
n = np.shape(D)[0]
rpy = np.empty([n,3])
for i in range(n):
quat = D[i,4:8]
rpy[i,:] = transformations.euler_from_quaternion(quat, axes='sxyz')
# filter rpy
f_sensor = 200.0; # sampling frequency in hz
f_cut = 15.0; # cutoff frequency in hz
b,a = signal.butter(5,f_cut/(f_sensor/2));
print a
print b
rpy_filt = np.empty([n,3])
rpy_filt[:,0] = signal.filtfilt(b, a, rpy[:,0])
rpy_filt[:,1] = signal.filtfilt(b, a, rpy[:,1])
rpy_filt[:,2] = signal.filtfilt(b, a, rpy[:,2])
fig = plt.figure()
ax = fig.add_subplot(111, title='orientation filtered')
ax.plot(rpy[:,0], 'r-')
ax.plot(rpy[:,1], 'g-')
ax.plot(rpy[:,2], 'b-')
ax.plot(rpy_filt[:,0], 'k-', linewidth=2)
ax.plot(rpy_filt[:,1], 'k-', linewidth=2)
ax.plot(rpy_filt[:,2], 'k-', linewidth=2)
fig = plt.figure()
ax = fig.add_subplot(111, title='position')
ax.plot(D[:,1], 'r')
ax.plot(D[:,2], 'g')
ax.plot(D[:,3], 'b')
fig = plt.figure()
ax = fig.add_subplot(111, title='trajectory from top')
ax.plot(D[:,1], D[:,2])
if save:
f = open(filtered_data_filename,'w')
for i in range(np.shape(D)[0]):
quat = transformations.quaternion_from_euler(rpy_filt[i,0], rpy_filt[i,1], rpy_filt[i,2], axes='sxyz')
f.write('%.7f %.5f %.5f %.5f %.5f %.5f %.5f %.5f\n' % (D[i,0], D[i,1], D[i,2], D[i,3], quat[0], quat[1], quat[2], quat[3]))
f.close()
@@ -0,0 +1,227 @@
# -*- coding: utf-8 -*-
"""
Created on Sun Aug 4 15:47:55 2013
@author: cforster
"""
import os
import yaml
import numpy as np
import svo_analysis.tum_benchmark_tools.associate as associate
import vikit_py.align_trajectory as align_trajectory
import vikit_py.transformations as transformations
import matplotlib.pyplot as plt
# user config
display = True
dataset_dir = '/home/cforster/catkin_ws/src/rpg_svo/svo_analysis/results/rpg_circle_1'
n_measurements = 400
n_align_sim3 = 600
delta = 50
# load dataset parameters
params = yaml.load(open(os.path.join(dataset_dir, 'dataset_params.yaml')))
# set trajectory groundtruth and estimate file
traj_groundtruth = os.path.join(dataset_dir, 'groundtruth.txt')
traj_estimate = os.path.join(dataset_dir,'traj_estimate.txt')
# load data
data_gt = associate.read_file_list(traj_groundtruth)
data_es = associate.read_file_list(traj_estimate)
# select matches
offset = -params['cam_delay']
print ('offset = '+str(offset))
matches = associate.associate(data_gt, data_es, offset, 0.02)
#matches = matches[500:]
p_gt = np.array([[float(value) for value in data_gt[a][0:3]] for a,b in matches])
q_gt = np.array([[float(value) for value in data_gt[a][3:7]] for a,b in matches])
p_es = np.array([[float(value) for value in data_es[b][0:3]] for a,b in matches])
q_es = np.array([[float(value) for value in data_es[b][3:7]] for a,b in matches])
# --------------------------------------------------------------------------------
# align Sim3 to get scale
scale,rot,trans = align_trajectory.align_sim3(p_gt[0:n_align_sim3,:], p_es[0:n_align_sim3,:])
#model_aligned = s * R * model + t
#alignment_error = model_aligned - data
#t_error = np.sqrt(np.sum(np.multiply(alignment_error,alignment_error),0)).A[0]
p_es_aligned = np.transpose(scale*np.dot(rot,np.transpose(p_es)))+trans
p_es = scale*p_es
print 's='+str(scale)
print 't='+str(trans)
print 'R='+str(rot)
# plot sim3 aligned trajectory
fig = plt.figure()
ax = fig.add_subplot(111, aspect='equal')
ax.plot(p_es_aligned[:,0], p_es_aligned[:,1], 'r-', label='estimate', alpha=0.2)
ax.plot(p_gt[:,0], p_gt[:,1], 'b-', label='groundtruth', alpha=0.2)
ax.plot(p_es_aligned[:n_align_sim3,0], p_es_aligned[:n_align_sim3,1], 'g-', label='aligned', linewidth=2)
ax.plot(p_gt[:n_align_sim3,0], p_gt[:n_align_sim3,1], 'm-', label='aligned', linewidth=2)
ax.legend()
for (x1,y1,z1),(x2,y2,z2) in zip(p_es_aligned[:n_align_sim3:10],p_gt[:n_align_sim3:10]):
ax.plot([x1,x2],[y1,y2],'-',color="red")
fig = plt.figure()
ax = fig.add_subplot(111)
ax.plot(p_gt[:,0], 'r-')
ax.plot(p_gt[:,1], 'g-')
ax.plot(p_gt[:,2], 'b-')
ax.plot(p_es_aligned[:,0], 'r--')
ax.plot(p_es_aligned[:,1], 'g--')
ax.plot(p_es_aligned[:,2], 'b--')
# --------------------------------------------------------------------------------
# hand-eye-calib
# select random measurements
I = np.array(np.random.rand(n_measurements,1)*(np.shape(matches)[0]-delta), dtype=int)[:,0]
R,b = align_trajectory.hand_eye_calib(q_gt, q_es, p_gt, p_es, I, delta, True)
print 'quat = ' + str(transformations.quaternion_from_matrix(transformations.convert_3x3_to_4x4(R)))
print 'b = ' + str(b)
rpy_es = np.zeros([q_es.shape[0]-1, 3])
rpy_gt = np.zeros([q_gt.shape[0]-1, 3])
t_gt = np.zeros([q_es.shape[0]-1,3])
t_es = np.zeros([q_es.shape[0]-1,3])
for i in range(delta,np.shape(q_es)[0]):
A1 = transformations.quaternion_matrix(q_es[i-delta,:])[:3,:3]
A2 = transformations.quaternion_matrix(q_es[i,:])[:3,:3]
A = np.dot(A1.transpose(), A2)
B1 = transformations.quaternion_matrix(q_gt[i-delta,:])[:3,:3]
B2 = transformations.quaternion_matrix(q_gt[i,:])[:3,:3]
B = np.dot(B1.transpose(), B2)
B_es = np.dot(np.transpose(R), np.dot(A, R))
rpy_gt[i-delta,:] = transformations.euler_from_matrix(B, 'rzyx')
rpy_es[i-delta,:] = transformations.euler_from_matrix(B_es, 'rzyx')
t_B = np.dot(np.transpose(B1),(p_gt[i,:]-p_gt[i-delta,:]))
t_A = np.dot(np.transpose(A1),(p_es[i,:]-p_es[i-delta,:]))
t_gt[i-delta,:] = t_B
t_es[i-delta,:] = np.dot(np.transpose(R), np.dot(A,b[:,0]) + t_A - b[:,0])
alignment_error = (t_gt-t_es)
error = np.sqrt(np.sum(np.multiply(alignment_error,alignment_error),1))
I_accurate = np.argwhere(error < np.percentile(error, 90))[:,0]
if display:
plt.figure()
plt.plot(rpy_es[:,0], 'r-', label='es roll')
plt.plot(rpy_es[:,1], 'g-', label='es pitch')
plt.plot(rpy_es[:,2], 'b-', label='es yaw')
plt.plot(rpy_gt[:,0], 'r--', label='gt roll')
plt.plot(rpy_gt[:,1], 'g--', label='gt pitch')
plt.plot(rpy_gt[:,2], 'b--', label='gt yaw')
plt.legend()
plt.figure()
plt.plot(t_gt[:,0], 'r-', label='gt x')
plt.plot(t_gt[:,1], 'g-', label='gt y')
plt.plot(t_gt[:,2], 'b-', label='gt z')
plt.plot(t_es[:,0], 'r--', label='es x')
plt.plot(t_es[:,1], 'g--', label='es y')
plt.plot(t_es[:,2], 'b--', label='es z')
plt.legend()
plt.figure()
plt.plot(error,'-g')
print 'e_rms = ' + str(np.sqrt(np.dot(error,error) / len(error)))
print 'e_mean = ' + str(np.mean(error))
print 'e_median = ' + str(np.median(error))
print 'e_std = ' + str(np.std(error))
# now sample again from the filtered list:
N = 10
display = False
n_acc_meas = I_accurate.size
n_measurements = 500
#for i in range(5):
# print '-------------------------------------'
# i0 = np.array(rand(n_measurements,1)*np.shape(I_accurate)[0], dtype=int)[:,0]
# i1 = np.minimum(i0+N, n_acc_meas-1)
# I = np.empty(i0.size*2, dtype=int)
# I[0::2] = I_accurate[i0]
# I[1::2] = I_accurate[i1]
# R,b = handEyeCalib(q_gt[I,:], q_es[I,:], p_gt[I,:], p_es[I,:], True)
# print 'quat = ' + str(ru.dcm2quat(R))
# print 'b = ' + str(b)
# rpy_es = np.zeros([q_es.shape[0]-1, 3])
# rpy_gt = np.zeros([q_gt.shape[0]-1, 3])
# t_gt = np.zeros([q_es.shape[0]-1,3])
# t_es = np.zeros([q_es.shape[0]-1,3])
#
# delta = 10
# for i in range(delta,np.shape(q_es)[0]):
# A1 = ru.quat2dcm(q_es[i-delta,:])
# A2 = ru.quat2dcm(q_es[i,:])
# A = np.dot(A1.transpose(), A2)
# B1 = ru.quat2dcm(q_gt[i-delta,:])
# B2 = ru.quat2dcm(q_gt[i,:])
# B = np.dot(B1.transpose(), B2)
# B_es = np.dot(np.transpose(R), np.dot(A, R))
# rpy_gt[i-delta,:] = ru.dcm2rpy(B)
# rpy_es[i-delta,:] = ru.dcm2rpy(B_es)
# t_B = np.dot(np.transpose(B1),(p_gt[i,:]-p_gt[i-delta,:]))
# t_A = np.dot(np.transpose(A1),(p_es[i,:]-p_es[i-delta,:]))
# t_gt[i-delta,:] = t_B
# t_es[i-delta,:] = np.dot(np.transpose(R), np.dot(A,b[:,0]) + t_A - b[:,0])
# alignment_error = (t_gt-t_es)
# error = np.sqrt(np.sum(np.multiply(alignment_error,alignment_error),1))
#
# if display:
# plt.figure()
# plt.plot(rpy_es[:,0], 'r-', label='es roll')
# plt.plot(rpy_es[:,1], 'g-', label='es pitch')
# plt.plot(rpy_es[:,2], 'b-', label='es yaw')
# plt.plot(rpy_gt[:,0], 'r--', label='gt roll')
# plt.plot(rpy_gt[:,1], 'g--', label='gt pitch')
# plt.plot(rpy_gt[:,2], 'b--', label='gt yaw')
# plt.legend()
# plt.figure()
# plt.plot(t_gt[:,0], 'r-', label='es x')
# plt.plot(t_gt[:,1], 'g-', label='es y')
# plt.plot(t_gt[:,2], 'b-', label='es z')
# plt.plot(t_es[:,0], 'r--', label='gt x')
# plt.plot(t_es[:,1], 'g--', label='gt y')
# plt.plot(t_es[:,2], 'b--', label='gt z')
# plt.legend()
# plt.figure()
# plt.plot(error,'-g')
#
# print 'e_rms = ' + str(np.sqrt(np.dot(error,error) / len(error)))
# print 'e_mean = ' + str(np.mean(error))
# print 'e_median = ' + str(np.median(error))
# print 'e_std = ' + str(np.std(error))
@@ -0,0 +1,2 @@
# -*- coding: utf-8 -*-
@@ -0,0 +1,130 @@
#!/usr/bin/python
# Software License Agreement (BSD License)
#
# Copyright (c) 2013, Juergen Sturm, TUM
# All rights reserved.
#
# Redistribution and use in source and binary forms, with or without
# modification, are permitted provided that the following conditions
# are met:
#
# * Redistributions of source code must retain the above copyright
# notice, this list of conditions and the following disclaimer.
# * Redistributions in binary form must reproduce the above
# copyright notice, this list of conditions and the following
# disclaimer in the documentation and/or other materials provided
# with the distribution.
# * Neither the name of TUM nor the names of its
# contributors may be used to endorse or promote products derived
# from this software without specific prior written permission.
#
# THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
# "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
# LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
# FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
# COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
# INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
# BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
# LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
# CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
# LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
# ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
# POSSIBILITY OF SUCH DAMAGE.
#
# Requirements:
# sudo apt-get install python-argparse
"""
The Kinect provides the color and depth images in an un-synchronized way. This means that the set of time stamps from the color images do not intersect with those of the depth images. Therefore, we need some way of associating color images to depth images.
For this purpose, you can use the ''associate.py'' script. It reads the time stamps from the rgb.txt file and the depth.txt file, and joins them by finding the best matches.
"""
import argparse
import sys
import os
import numpy
def read_file_list(filename):
"""
Reads a trajectory from a text file.
File format:
The file format is "stamp d1 d2 d3 ...", where stamp denotes the time stamp (to be matched)
and "d1 d2 d3.." is arbitary data (e.g., a 3D position and 3D orientation) associated to this timestamp.
Input:
filename -- File name
Output:
dict -- dictionary of (stamp,data) tuples
"""
file = open(filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
list = [[v.strip() for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"]
list = [(float(l[0]),l[1:]) for l in list if len(l)>1]
return dict(list)
def associate(first_list, second_list,offset,max_difference):
"""
Associate two dictionaries of (stamp,data). As the time stamps never match exactly, we aim
to find the closest match for every input tuple.
Input:
first_list -- first dictionary of (stamp,data) tuples
second_list -- second dictionary of (stamp,data) tuples
offset -- time offset between both dictionaries (e.g., to model the delay between the sensors)
max_difference -- search radius for candidate generation
Output:
matches -- list of matched tuples ((stamp1,data1),(stamp2,data2))
"""
first_keys = first_list.keys()
second_keys = second_list.keys()
potential_matches = [(abs(a - (b + offset)), a, b)
for a in first_keys
for b in second_keys
if abs(a - (b + offset)) < max_difference]
potential_matches.sort()
matches = []
for diff, a, b in potential_matches:
if a in first_keys and b in second_keys:
first_keys.remove(a)
second_keys.remove(b)
matches.append((a, b))
matches.sort()
return matches
if __name__ == '__main__':
# parse command line
parser = argparse.ArgumentParser(description='''
This script takes two data files with timestamps and associates them
''')
parser.add_argument('first_file', help='estimated trajectory (format: timestamp data)')
parser.add_argument('second_file', help='groundtruth (format: timestamp data)')
parser.add_argument('--offset', help='time offset added to the timestamps of the second file (default: 0.0)',default=0.0)
parser.add_argument('--max_difference', help='maximally allowed time difference for matching entries (default: 0.02)',default=0.02)
args = parser.parse_args()
first_list = read_file_list(args.first_file)
second_list = read_file_list(args.second_file)
matches = associate(first_list, second_list,float(args.offset),float(args.max_difference))
filename = 'groundtruth_matched.txt'
associates_file = open(filename, 'w')
for a,b in matches:
img = first_list[a]
pos = second_list[b]
associates_file.write('%.6f %s %s %s %s %s %s %s %s\n' %
(a, img[0],
pos[0], pos[1], pos[2],
pos[3], pos[4], pos[5], pos[6]))
print('Wrote matches to file: ' + filename)
@@ -0,0 +1,194 @@
#!/usr/bin/python
# Software License Agreement (BSD License)
#
# Copyright (c) 2013, Juergen Sturm, TUM
# All rights reserved.
#
# Redistribution and use in source and binary forms, with or without
# modification, are permitted provided that the following conditions
# are met:
#
# * Redistributions of source code must retain the above copyright
# notice, this list of conditions and the following disclaimer.
# * Redistributions in binary form must reproduce the above
# copyright notice, this list of conditions and the following
# disclaimer in the documentation and/or other materials provided
# with the distribution.
# * Neither the name of TUM nor the names of its
# contributors may be used to endorse or promote products derived
# from this software without specific prior written permission.
#
# THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
# "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
# LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
# FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
# COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
# INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
# BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
# LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
# CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
# LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
# ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
# POSSIBILITY OF SUCH DAMAGE.
#
# Requirements:
# sudo apt-get install python-argparse
"""
This script computes the absolute trajectory error from the ground truth
trajectory and the estimated trajectory.
"""
import sys
import numpy
import argparse
import associate
def align(model,data):
"""Align two trajectories using the method of Horn (closed-form).
Input:
model -- first trajectory (3xn)
data -- second trajectory (3xn)
Output:
rot -- rotation matrix (3x3)
trans -- translation vector (3x1)
trans_error -- translational error per point (1xn)
"""
numpy.set_printoptions(precision=3,suppress=True)
model_zerocentered = model - model.mean(1)
data_zerocentered = data - data.mean(1)
W = numpy.zeros( (3,3) )
for column in range(model.shape[1]):
W += numpy.outer(model_zerocentered[:,column],data_zerocentered[:,column])
U,d,Vh = numpy.linalg.linalg.svd(W.transpose())
S = numpy.matrix(numpy.identity( 3 ))
if(numpy.linalg.det(U) * numpy.linalg.det(Vh)<0):
S[2,2] = -1
rot = U*S*Vh
trans = data.mean(1) - rot * model.mean(1)
model_aligned = rot * model + trans
alignment_error = model_aligned - data
trans_error = numpy.sqrt(numpy.sum(numpy.multiply(alignment_error,alignment_error),0)).A[0]
return rot,trans,trans_error
def plot_traj(ax,stamps,traj,style,color,label):
"""
Plot a trajectory using matplotlib.
Input:
ax -- the plot
stamps -- time stamps (1xn)
traj -- trajectory (3xn)
style -- line style
color -- line color
label -- plot legend
"""
stamps.sort()
interval = numpy.median([s-t for s,t in zip(stamps[1:],stamps[:-1])])
x = []
y = []
last = stamps[0]
for i in range(len(stamps)):
if stamps[i]-last < 2*interval:
x.append(traj[i][0])
y.append(traj[i][1])
elif len(x)>0:
ax.plot(x,y,style,color=color,label=label)
label=""
x=[]
y=[]
last= stamps[i]
if len(x)>0:
ax.plot(x,y,style,color=color,label=label)
if __name__=="__main__":
# parse command line
parser = argparse.ArgumentParser(description='''
This script computes the absolute trajectory error from the ground truth trajectory and the estimated trajectory.
''')
parser.add_argument('first_file', help='ground truth trajectory (format: timestamp tx ty tz qx qy qz qw)')
parser.add_argument('second_file', help='estimated trajectory (format: timestamp tx ty tz qx qy qz qw)')
parser.add_argument('--offset', help='time offset added to the timestamps of the second file (default: 0.0)',default=0.0)
parser.add_argument('--scale', help='scaling factor for the second trajectory (default: 1.0)',default=1.0)
parser.add_argument('--max_difference', help='maximally allowed time difference for matching entries (default: 0.02)',default=0.02)
parser.add_argument('--save', help='save aligned second trajectory to disk (format: stamp2 x2 y2 z2)')
parser.add_argument('--save_associations', help='save associated first and aligned second trajectory to disk (format: stamp1 x1 y1 z1 stamp2 x2 y2 z2)')
parser.add_argument('--plot', help='plot the first and the aligned second trajectory to an image (format: png)')
parser.add_argument('--verbose', help='print all evaluation data (otherwise, only the RMSE absolute translational error in meters after alignment will be printed)', action='store_true')
args = parser.parse_args()
first_list = associate.read_file_list(args.first_file)
second_list = associate.read_file_list(args.second_file)
matches = associate.associate(first_list, second_list, float(args.offset), float(args.max_difference))
if len(matches)<2:
sys.exit("Couldn't find matching timestamp pairs between groundtruth and estimated trajectory! Did you choose the correct sequence?")
first_xyz = numpy.matrix([[float(value) for value in first_list[a][0:3]] for a,b in matches]).transpose()
second_xyz = numpy.matrix([[float(value)*float(args.scale) for value in second_list[b][0:3]] for a,b in matches]).transpose()
rot,trans,trans_error = align(second_xyz,first_xyz)
second_xyz_aligned = rot * second_xyz + trans
first_stamps = first_list.keys()
first_stamps.sort()
first_xyz_full = numpy.matrix([[float(value) for value in first_list[b][0:3]] for b in first_stamps]).transpose()
second_stamps = second_list.keys()
second_stamps.sort()
second_xyz_full = numpy.matrix([[float(value)*float(args.scale) for value in second_list[b][0:3]] for b in second_stamps]).transpose()
second_xyz_full_aligned = rot * second_xyz_full + trans
if args.verbose:
print "compared_pose_pairs %d pairs"%(len(trans_error))
print "absolute_translational_error.rmse %f m"%numpy.sqrt(numpy.dot(trans_error,trans_error) / len(trans_error))
print "absolute_translational_error.mean %f m"%numpy.mean(trans_error)
print "absolute_translational_error.median %f m"%numpy.median(trans_error)
print "absolute_translational_error.std %f m"%numpy.std(trans_error)
print "absolute_translational_error.min %f m"%numpy.min(trans_error)
print "absolute_translational_error.max %f m"%numpy.max(trans_error)
else:
print "%f"%numpy.sqrt(numpy.dot(trans_error,trans_error) / len(trans_error))
if args.save_associations:
file = open(args.save_associations,"w")
file.write("\n".join(["%f %f %f %f %f %f %f %f"%(a,x1,y1,z1,b,x2,y2,z2) for (a,b),(x1,y1,z1),(x2,y2,z2) in zip(matches,first_xyz.transpose().A,second_xyz_aligned.transpose().A)]))
file.close()
if args.save:
file = open(args.save,"w")
file.write("\n".join(["%f "%stamp+" ".join(["%f"%d for d in line]) for stamp,line in zip(second_stamps,second_xyz_full_aligned.transpose().A)]))
file.close()
if args.plot:
import matplotlib
matplotlib.use('Agg')
import matplotlib.pyplot as plt
fig = plt.figure()
ax = fig.add_subplot(111)
plot_traj(ax,first_stamps,first_xyz_full.transpose().A,'-',"black","ground truth")
plot_traj(ax,second_stamps,second_xyz_full_aligned.transpose().A,'-',"blue","estimated")
label="difference"
for (a,b),(x1,y1,z1),(x2,y2,z2) in zip(matches,first_xyz.transpose().A,second_xyz_aligned.transpose().A):
ax.plot([x1,x2],[y1,y2],'-',color="red",label=label)
label=""
ax.legend()
ax.set_xlabel('x [m]')
ax.set_ylabel('y [m]')
plt.savefig(args.plot,dpi=90)
@@ -0,0 +1,382 @@
#!/usr/bin/python
# Software License Agreement (BSD License)
#
# Copyright (c) 2013, Juergen Sturm, TUM
# All rights reserved.
#
# Redistribution and use in source and binary forms, with or without
# modification, are permitted provided that the following conditions
# are met:
#
# * Redistributions of source code must retain the above copyright
# notice, this list of conditions and the following disclaimer.
# * Redistributions in binary form must reproduce the above
# copyright notice, this list of conditions and the following
# disclaimer in the documentation and/or other materials provided
# with the distribution.
# * Neither the name of TUM nor the names of its
# contributors may be used to endorse or promote products derived
# from this software without specific prior written permission.
#
# THIS SOFTWARE IS PROVIDED BY THE COPYRIGHT HOLDERS AND CONTRIBUTORS
# "AS IS" AND ANY EXPRESS OR IMPLIED WARRANTIES, INCLUDING, BUT NOT
# LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS
# FOR A PARTICULAR PURPOSE ARE DISCLAIMED. IN NO EVENT SHALL THE
# COPYRIGHT OWNER OR CONTRIBUTORS BE LIABLE FOR ANY DIRECT, INDIRECT,
# INCIDENTAL, SPECIAL, EXEMPLARY, OR CONSEQUENTIAL DAMAGES (INCLUDING,
# BUT NOT LIMITED TO, PROCUREMENT OF SUBSTITUTE GOODS OR SERVICES;
# LOSS OF USE, DATA, OR PROFITS; OR BUSINESS INTERRUPTION) HOWEVER
# CAUSED AND ON ANY THEORY OF LIABILITY, WHETHER IN CONTRACT, STRICT
# LIABILITY, OR TORT (INCLUDING NEGLIGENCE OR OTHERWISE) ARISING IN
# ANY WAY OUT OF THE USE OF THIS SOFTWARE, EVEN IF ADVISED OF THE
# POSSIBILITY OF SUCH DAMAGE.
"""
This script computes the relative pose error from the ground truth trajectory
and the estimated trajectory.
"""
import argparse
import random
import numpy
import sys
_EPS = numpy.finfo(float).eps * 4.0
def transform44(l):
"""
Generate a 4x4 homogeneous transformation matrix from a 3D point and unit quaternion.
Input:
l -- tuple consisting of (stamp,tx,ty,tz,qx,qy,qz,qw) where
(tx,ty,tz) is the 3D position and (qx,qy,qz,qw) is the unit quaternion.
Output:
matrix -- 4x4 homogeneous transformation matrix
"""
t = l[1:4]
q = numpy.array(l[4:8], dtype=numpy.float64, copy=True)
nq = numpy.dot(q, q)
if nq < _EPS:
return numpy.array((
( 1.0, 0.0, 0.0, t[0])
( 0.0, 1.0, 0.0, t[1])
( 0.0, 0.0, 1.0, t[2])
( 0.0, 0.0, 0.0, 1.0)
), dtype=numpy.float64)
q *= numpy.sqrt(2.0 / nq)
q = numpy.outer(q, q)
return numpy.array((
(1.0-q[1, 1]-q[2, 2], q[0, 1]-q[2, 3], q[0, 2]+q[1, 3], t[0]),
( q[0, 1]+q[2, 3], 1.0-q[0, 0]-q[2, 2], q[1, 2]-q[0, 3], t[1]),
( q[0, 2]-q[1, 3], q[1, 2]+q[0, 3], 1.0-q[0, 0]-q[1, 1], t[2]),
( 0.0, 0.0, 0.0, 1.0)
), dtype=numpy.float64)
def read_trajectory(filename, matrix=True):
"""
Read a trajectory from a text file.
Input:
filename -- file to be read
matrix -- convert poses to 4x4 matrices
Output:
dictionary of stamped 3D poses
"""
file = open(filename)
data = file.read()
lines = data.replace(","," ").replace("\t"," ").split("\n")
list = [[float(v.strip()) for v in line.split(" ") if v.strip()!=""] for line in lines if len(line)>0 and line[0]!="#"]
list_ok = []
for i,l in enumerate(list):
if l[4:8]==[0,0,0,0]:
continue
isnan = False
for v in l:
if numpy.isnan(v):
isnan = True
break
if isnan:
sys.stderr.write("Warning: line %d of file '%s' has NaNs, skipping line\n"%(i,filename))
continue
list_ok.append(l)
if matrix :
traj = dict([(l[0],transform44(l[0:])) for l in list_ok])
else:
traj = dict([(l[0],l[1:8]) for l in list_ok])
return traj
def find_closest_index(L,t):
"""
Find the index of the closest value in a list.
Input:
L -- the list
t -- value to be found
Output:
index of the closest element
"""
beginning = 0
difference = abs(L[0] - t)
best = 0
end = len(L)
while beginning < end:
middle = int((end+beginning)/2)
if abs(L[middle] - t) < difference:
difference = abs(L[middle] - t)
best = middle
if t == L[middle]:
return middle
elif L[middle] > t:
end = middle
else:
beginning = middle + 1
return best
def ominus(a,b):
"""
Compute the relative 3D transformation between a and b.
Input:
a -- first pose (homogeneous 4x4 matrix)
b -- second pose (homogeneous 4x4 matrix)
Output:
Relative 3D transformation from a to b.
"""
return numpy.dot(numpy.linalg.inv(a),b)
def scale(a,scalar):
"""
Scale the translational components of a 4x4 homogeneous matrix by a scale factor.
"""
return numpy.array(
[[a[0,0], a[0,1], a[0,2], a[0,3]*scalar],
[a[1,0], a[1,1], a[1,2], a[1,3]*scalar],
[a[2,0], a[2,1], a[2,2], a[2,3]*scalar],
[a[3,0], a[3,1], a[3,2], a[3,3]]]
)
def compute_distance(transform):
"""
Compute the distance of the translational component of a 4x4 homogeneous matrix.
"""
return numpy.linalg.norm(transform[0:3,3])
def compute_angle(transform):
"""
Compute the rotation angle from a 4x4 homogeneous matrix.
"""
# an invitation to 3-d vision, p 27
return numpy.arccos( min(1,max(-1, (numpy.trace(transform[0:3,0:3]) - 1)/2) ))
def distances_along_trajectory(traj):
"""
Compute the translational distances along a trajectory.
"""
keys = traj.keys()
keys.sort()
motion = [ominus(traj[keys[i+1]],traj[keys[i]]) for i in range(len(keys)-1)]
distances = [0]
sum = 0
for t in motion:
sum += compute_distance(t)
distances.append(sum)
return distances
def rotations_along_trajectory(traj,scale):
"""
Compute the angular rotations along a trajectory.
"""
keys = traj.keys()
keys.sort()
motion = [ominus(traj[keys[i+1]],traj[keys[i]]) for i in range(len(keys)-1)]
distances = [0]
sum = 0
for t in motion:
sum += compute_angle(t)*scale
distances.append(sum)
return distances
def evaluate_trajectory(traj_gt,traj_est,param_max_pairs=10000,param_fixed_delta=False,param_delta=1.00,param_delta_unit="s",param_offset=0.00,param_scale=1.00):
"""
Compute the relative pose error between two trajectories.
Input:
traj_gt -- the first trajectory (ground truth)
traj_est -- the second trajectory (estimated trajectory)
param_max_pairs -- number of relative poses to be evaluated
param_fixed_delta -- false: evaluate over all possible pairs
true: only evaluate over pairs with a given distance (delta)
param_delta -- distance between the evaluated pairs
param_delta_unit -- unit for comparison:
"s": seconds
"m": meters
"rad": radians
"deg": degrees
"f": frames
param_offset -- time offset between two trajectories (to model the delay)
param_scale -- scale to be applied to the second trajectory
Output:
list of compared poses and the resulting translation and rotation error
"""
stamps_gt = list(traj_gt.keys())
stamps_est = list(traj_est.keys())
stamps_gt.sort()
stamps_est.sort()
stamps_est_return = []
for t_est in stamps_est:
t_gt = stamps_gt[find_closest_index(stamps_gt,t_est + param_offset)]
t_est_return = stamps_est[find_closest_index(stamps_est,t_gt - param_offset)]
t_gt_return = stamps_gt[find_closest_index(stamps_gt,t_est_return + param_offset)]
if not t_est_return in stamps_est_return:
stamps_est_return.append(t_est_return)
if(len(stamps_est_return)<2):
raise Exception("Number of overlap in the timestamps is too small. Did you run the evaluation on the right files?")
if param_delta_unit=="s":
index_est = list(traj_est.keys())
index_est.sort()
elif param_delta_unit=="m":
index_est = distances_along_trajectory(traj_est)
elif param_delta_unit=="rad":
index_est = rotations_along_trajectory(traj_est,1)
elif param_delta_unit=="deg":
index_est = rotations_along_trajectory(traj_est,180/numpy.pi)
elif param_delta_unit=="f":
index_est = range(len(traj_est))
else:
raise Exception("Unknown unit for delta: '%s'"%param_delta_unit)
if not param_fixed_delta:
if(param_max_pairs==0 or len(traj_est)<numpy.sqrt(param_max_pairs)):
pairs = [(i,j) for i in range(len(traj_est)) for j in range(len(traj_est))]
else:
pairs = [(random.randint(0,len(traj_est)-1),random.randint(0,len(traj_est)-1)) for i in range(param_max_pairs)]
else:
pairs = []
for i in range(len(traj_est)):
j = find_closest_index(index_est,index_est[i] + param_delta)
if j!=len(traj_est)-1:
pairs.append((i,j))
if(param_max_pairs!=0 and len(pairs)>param_max_pairs):
pairs = random.sample(pairs,param_max_pairs)
gt_interval = numpy.median([s-t for s,t in zip(stamps_gt[1:],stamps_gt[:-1])])
gt_max_time_difference = 2*gt_interval
result = []
for i,j in pairs:
stamp_est_0 = stamps_est[i]
stamp_est_1 = stamps_est[j]
stamp_gt_0 = stamps_gt[ find_closest_index(stamps_gt,stamp_est_0 + param_offset) ]
stamp_gt_1 = stamps_gt[ find_closest_index(stamps_gt,stamp_est_1 + param_offset) ]
if(abs(stamp_gt_0 - (stamp_est_0 + param_offset)) > gt_max_time_difference or
abs(stamp_gt_1 - (stamp_est_1 + param_offset)) > gt_max_time_difference):
continue
error44 = ominus( scale(
ominus( traj_est[stamp_est_1], traj_est[stamp_est_0] ),param_scale),
ominus( traj_gt[stamp_gt_1], traj_gt[stamp_gt_0] ) )
trans = compute_distance(error44)
rot = compute_angle(error44)
result.append([stamp_est_0,stamp_est_1,stamp_gt_0,stamp_gt_1,trans,rot])
if len(result)<2:
raise Exception("Couldn't find matching timestamp pairs between groundtruth and estimated trajectory!")
return result
def percentile(seq,q):
"""
Return the q-percentile of a list
"""
seq_sorted = list(seq)
seq_sorted.sort()
return seq_sorted[int((len(seq_sorted)-1)*q)]
if __name__ == '__main__':
random.seed(0)
parser = argparse.ArgumentParser(description='''
This script computes the relative pose error from the ground truth trajectory and the estimated trajectory.
''')
parser.add_argument('groundtruth_file', help='ground-truth trajectory file (format: "timestamp tx ty tz qx qy qz qw")')
parser.add_argument('estimated_file', help='estimated trajectory file (format: "timestamp tx ty tz qx qy qz qw")')
parser.add_argument('--max_pairs', help='maximum number of pose comparisons (default: 10000, set to zero to disable downsampling)', default=10000)
parser.add_argument('--fixed_delta', help='only consider pose pairs that have a distance of delta delta_unit (e.g., for evaluating the drift per second/meter/radian)', action='store_true')
parser.add_argument('--delta', help='delta for evaluation (default: 1.0)',default=1.0)
parser.add_argument('--delta_unit', help='unit of delta (options: \'s\' for seconds, \'m\' for meters, \'rad\' for radians, \'f\' for frames; default: \'s\')',default='s')
parser.add_argument('--offset', help='time offset between ground-truth and estimated trajectory (default: 0.0)',default=0.0)
parser.add_argument('--scale', help='scaling factor for the estimated trajectory (default: 1.0)',default=1.0)
parser.add_argument('--save', help='text file to which the evaluation will be saved (format: stamp_est0 stamp_est1 stamp_gt0 stamp_gt1 trans_error rot_error)')
parser.add_argument('--plot', help='plot the result to a file (requires --fixed_delta, output format: png)')
parser.add_argument('--verbose', help='print all evaluation data (otherwise, only the mean translational error measured in meters will be printed)', action='store_true')
args = parser.parse_args()
if args.plot and not args.fixed_delta:
sys.exit("The '--plot' option can only be used in combination with '--fixed_delta'")
traj_gt = read_trajectory(args.groundtruth_file)
traj_est = read_trajectory(args.estimated_file)
result = evaluate_trajectory(traj_gt,
traj_est,
int(args.max_pairs),
args.fixed_delta,
float(args.delta),
args.delta_unit,
float(args.offset),
float(args.scale))
stamps = numpy.array(result)[:,0]
trans_error = numpy.array(result)[:,4]
rot_error = numpy.array(result)[:,5]
if args.save:
f = open(args.save,"w")
f.write("\n".join([" ".join(["%f"%v for v in line]) for line in result]))
f.close()
if args.verbose:
print "compared_pose_pairs %d pairs"%(len(trans_error))
print "translational_error.rmse %f m"%numpy.sqrt(numpy.dot(trans_error,trans_error) / len(trans_error))
print "translational_error.mean %f m"%numpy.mean(trans_error)
print "translational_error.median %f m"%numpy.median(trans_error)
print "translational_error.std %f m"%numpy.std(trans_error)
print "translational_error.min %f m"%numpy.min(trans_error)
print "translational_error.max %f m"%numpy.max(trans_error)
print "rotational_error.rmse %f deg"%(numpy.sqrt(numpy.dot(rot_error,rot_error) / len(rot_error)) * 180.0 / numpy.pi)
print "rotational_error.mean %f deg"%(numpy.mean(rot_error) * 180.0 / numpy.pi)
print "rotational_error.median %f deg"%numpy.median(rot_error)
print "rotational_error.std %f deg"%(numpy.std(rot_error) * 180.0 / numpy.pi)
print "rotational_error.min %f deg"%(numpy.min(rot_error) * 180.0 / numpy.pi)
print "rotational_error.max %f deg"%(numpy.max(rot_error) * 180.0 / numpy.pi)
else:
print numpy.mean(trans_error)
if args.plot:
import matplotlib
matplotlib.use('Agg')
import matplotlib.pyplot as plt
import matplotlib.pylab as pylab
fig = plt.figure()
ax = fig.add_subplot(111)
ax.plot(stamps - stamps[0],trans_error,'-',color="blue")
#ax.plot([t for t,e in err_rot],[e for t,e in err_rot],'-',color="red")
ax.set_xlabel('time [s]')
ax.set_ylabel('translational error [m]')
plt.savefig(args.plot,dpi=300)