def calc_comparison(logfile_mu_density, mosaiq_mu_density, normalisation=None):
if normalisation is None:
normalisation = np.sum(mosaiq_mu_density)
comparison = np.sum(np.abs(logfile_mu_density - mosaiq_mu_density)) / normalisation
return comparison
def _fraction_number(self, dicom_template, gantry_tol=3, meterset_tol=0.5):
fractions = dicom_template.FractionGroupSequence
if len(fractions) == 1:
return fractions[0].FractionGroupNumber
fraction_numbers = [
fraction.FractionGroupNumber for fraction in fractions
]
fraction_matches = np.array([
self._matches_fraction(
dicom_template,
fraction_number,
gantry_tol=gantry_tol,
meterset_tol=meterset_tol,
) for fraction_number in fraction_numbers
])
if np.sum(fraction_matches) < 1:
raise ValueError(
"A fraction group was not able to be found with the metersets "
"and gantry angles defined by the tolerances provided. "
"Please manually define the fraction group number.")
if np.sum(fraction_matches) > 1:
raise ValueError(
"More than one fraction group was found that had metersets "
"and gantry angles within the tolerances provided. "
"Please manually define the fraction group number.")
fraction_number = np.array(fraction_numbers)[fraction_matches]
return fraction_number
def create_bb_to_minimise(field, bb_diameter):
"""This is a numpy vectorised version of `create_bb_to_minimise_simple`
"""
points_to_check_edge_agreement, dist = interppoints.create_bb_points_function(
bb_diameter)
dist_mask = np.unique(dist)[:, None] == dist[None, :]
num_in_mask = np.sum(dist_mask, axis=1)
mask_count_per_item = np.sum(num_in_mask[:, None] * dist_mask, axis=0)
mask_mean_lookup = np.where(dist_mask)[0]
def to_minimise_edge_agreement(centre):
x, y = points_to_check_edge_agreement(centre)
results = field(x, y)
masked_results = results * dist_mask
mask_mean = np.sum(masked_results, axis=1) / num_in_mask
diff_to_mean_square = (results - mask_mean[mask_mean_lookup])**2
mean_of_layers = np.sum(
diff_to_mean_square[1::] /
mask_count_per_item[1::]) / (len(mask_mean) - 1)
return mean_of_layers
return to_minimise_edge_agreement
def to_minimise(inputs):
x_shift = inputs[0]
y_shift = inputs[1]
angle = inputs[2]
interpolated = shift_and_rotate_with_interp(moving_interp,
(ref_x, ref_y),
(x_shift, y_shift), angle)
return np.sum(
(interpolated - ref_edge_filtered)**2) - np.sum(interpolated)
def soft_surface_dice(reference, evaluation):
"""Non-TensorFlow implementation of a soft surface dice
"""
edge_reference = skimage.filters.scharr(reference)
edge_evaluation = skimage.filters.scharr(evaluation)
score = np.sum(np.abs(edge_evaluation - edge_reference)) / np.sum(
edge_evaluation + edge_reference
)
return 1 - score
def to_minimise_edge_agreement(centre):
x, y = points_to_check_edge_agreement(centre)
results = field(x, y)
masked_results = results * dist_mask
mask_mean = np.sum(masked_results, axis=1) / num_in_mask
diff_to_mean_square = (results - mask_mean[mask_mean_lookup])**2
mean_of_layers = np.sum(
diff_to_mean_square[1::] /
mask_count_per_item[1::]) / (len(mask_mean) - 1)
return mean_of_layers
def mephysto_absolute_profiles(
curvetype,
depth_test,
distance,
relative_dose,
scan_curvetype,
scan_depth,
mephysto_pdd_depth,
mephysto_pdd_dose,
):
choose_mephysto = (scan_curvetype == curvetype) & (scan_depth
== depth_test)
if np.sum(choose_mephysto) != 1:
raise ValueError(
"Can only handle exactly one scan type per mephysto file")
mephysto_distance = distance[choose_mephysto][0]
mephysto_normalised_dose = normalisation.normalise_profile(
mephysto_distance,
relative_dose[choose_mephysto][0],
scale_to_pdd=True,
pdd_distance=mephysto_pdd_depth,
pdd_relative_dose=mephysto_pdd_dose,
scan_depth=depth_test,
)
return mephysto_distance, mephysto_normalised_dose
def folder_analyze(volume):
for item in range(0, volume.shape[2]):
stack1 = np.sum(volume[:, :, item], axis=0)
maxstack1 = np.max(stack1)
stack2 = np.sum(volume[:, :, item], axis=1)
maxstack2 = np.max(stack2)
if maxstack2 / maxstack1 > 1.5: # It is a Y field folder
field = 2
elif maxstack2 / maxstack1 < 0.5: # It is a X field folder
field = 1
else:
field = 3 # It is a field rotation folder
return field
def calc_min_distance(cube_definition, contours):
vertices = cube_vertices(cube_definition)
vectors = cube_vectors(cube_definition)
unit_vectors = [vector / np.linalg.norm(vector) for vector in vectors]
plane_norms = np.array(
[
unit_vectors[1],
-unit_vectors[0],
-unit_vectors[1],
unit_vectors[0],
unit_vectors[2],
-unit_vectors[2],
]
)
plane_points = np.array(
[vertices[0], vertices[1], vertices[2], vertices[0], vertices[0], vertices[3]]
)
plane_origin_dist = -np.sum(plane_points * plane_norms, axis=1)
distance_to_planes = np.dot(plane_norms, contours) + plane_origin_dist[:, None]
min_dist_squared = np.min(distance_to_planes ** 2, axis=0)
return min_dist_squared
def to_minimise(cube):
cube_definition = cubify_cube_definition(
[tuple(cube[0:3]),
tuple(cube[3:6]),
tuple(cube[6::])])
min_dist_squared = calc_min_distance(cube_definition, contour_points)
return np.sum(min_dist_squared)
def distance_to(self, point):
"""Calculate the minimum distance from the line to a point.
Equations are from here: http://mathworld.wolfram.com/Point-LineDistance2-Dimensional.html #14
Parameters
----------
point : Point, iterable
The point to calculate distance to.
"""
point = Point(point).as_array()
lp1 = self.point1.as_array()
lp2 = self.point2.as_array()
numerator = np.sqrt(
np.sum(np.power(np.cross((lp2 - lp1), (lp1 - point)), 2)))
denominator = np.sqrt(np.sum(np.power(lp2 - lp1, 2)))
return numerator / denominator
def calc_normalisation(mosaiq_delivery_data):
all_gantry_angles = mosaiq_delivery_data.mudensity
mosaiq_gantry_angles = np.unique(mosaiq_delivery_data.gantry)
number_of_gantry_angles = len(mosaiq_gantry_angles)
normalisation = np.sum(all_gantry_angles) / number_of_gantry_angles
return normalisation
def filled_area_ratio(array) -> float:
"""Return the ratio of filled pixels to empty pixels in the ROI bounding box.
For example a solid square would be 1.0, while a sold circle would be ~0.785.
"""
ymin, ymax, xmin, xmax = bounding_box(array)
box_area = (ymax - ymin) * (xmax - xmin)
filled_area = np.sum(array)
return float(filled_area / box_area)
def plot_gamma_hist(gamma, percent, dist):
valid_gamma = gamma[~np.isnan(gamma)]
plt.hist(valid_gamma, 50, density=True)
pass_ratio = np.sum(valid_gamma <= 1) / len(valid_gamma)
plt.title(
"Local Gamma ({0}%/{1}mm) | Percent Pass: {2:.2f} % | Mean Gamma: {3:.2f} | Max Gamma: {4:.2f}"
.format(percent, dist, pass_ratio * 100, np.mean(valid_gamma),
np.max(valid_gamma)))
def _determine_leaf_centres(leaf_pair_widths):
total_leaf_widths = np.sum(leaf_pair_widths)
leaf_centres = (np.cumsum(leaf_pair_widths) - leaf_pair_widths / 2 -
total_leaf_widths / 2)
reference_leaf_index = len(leaf_centres) // 2
top_of_reference_leaf = (leaf_centres[reference_leaf_index] +
leaf_pair_widths[reference_leaf_index] / 2)
return leaf_centres, top_of_reference_leaf
def to_minimise(centre):
(
xx_left_right,
yy_left_right,
xx_top_bot,
yy_top_bot,
) = transform_penumbra_points(points_at_origin, centre, rotation)
left_right_interpolated = field(xx_left_right, yy_left_right)
top_bot_interpolated = field(xx_top_bot, yy_top_bot)
left_right_weighted_diff = (
2 * (left_right_interpolated - left_right_interpolated[:, ::-1]) /
(left_right_interpolated + left_right_interpolated[:, ::-1]))
top_bot_weighted_diff = (
2 * (top_bot_interpolated - top_bot_interpolated[::-1, :]) /
(top_bot_interpolated + top_bot_interpolated[::-1, :]))
return np.sum(left_right_weighted_diff**2) + np.sum(
top_bot_weighted_diff**2)
def _gantry_angle_masks(self,
gantry_angles,
gantry_tol,
allow_missing_angles=False):
masks = [
self._gantry_angle_mask(gantry_angle, gantry_tol)
for gantry_angle in gantry_angles
]
for mask in masks:
if np.all(mask == 0):
continue
# TODO: Apply mask by more than just gantry angle to appropriately
# extract beam index even when multiple beams have the same gantry
# angle
is_duplicate_gantry_angles = (np.sum(
np.abs(np.diff(np.concatenate([[0], mask, [0]])))) != 2)
if is_duplicate_gantry_angles:
raise ValueError("Duplicate gantry angles not yet supported")
try:
assert np.all(np.sum(masks, axis=0) == 1), (
"Not all beams were captured by the gantry tolerance of "
" {}".format(gantry_tol))
except AssertionError:
if not allow_missing_angles:
print("Allowable gantry angles = {}".format(gantry_angles))
gantry = np.array(self.gantry, copy=False)
out_of_tolerance = np.unique(
gantry[np.sum(masks, axis=0) == 0]).tolist()
print("The gantry angles out of tolerance were {}".format(
out_of_tolerance))
raise
return masks
def pull_mephysto_item(string, file_contents):
"""Steps through each scan region searching for a mephysto parameter that
matches the requested string. Returns an array filled with the results for
all scans that have a match. If a scan does not have a parameter matching
the request then np.nan is returned.
"""
scan_index = find_scan_index(file_contents)
# Format the input string for use in a regex search
string_test = re.escape(string)
result = []
# Loop over each scan index searching for requested parameter
for index in scan_index:
# See if any parameters match within this scan
match = np.array([
re.match(r"^\t\t" + string_test + "=(.*)$", item) is not None
for item in file_contents[index]
])
# If there is a single match then return the result
if np.sum(match) == 1:
relevant_line = file_contents[index][match][0]
# Return the value that is after the equal sign
# Example -- https://regex101.com/r/lR4pS2/7
result.append(
re.search(r"^\t\t" + string_test + "=(.*)$",
relevant_line).group(1))
# If there is no matches return np.nan
elif np.sum(match) == 0:
result.append(np.nan)
# If there is more than one match raise an error
else:
raise Exception("More than one item has this label")
return np.array(result)
def _calc_device_open(blocked_by_device):
device_open = {}
for device, value in blocked_by_device.items():
device_sum = np.sum(
np.concatenate(
[np.expand_dims(blocked, axis=0) for _, blocked in value.items()],
axis=0,
),
axis=0,
)
device_open[device] = 1 - device_sum
return device_open
def mephysto_absolute_depth_dose(absolute_dose, depth_of_absolute_dose_mm,
distance, relative_dose, scan_curvetype):
choose_mephysto = scan_curvetype == "PDD"
if np.sum(choose_mephysto) != 1:
raise ValueError("Can only handle one PDD per mephysto file")
mephysto_pdd_depth = distance[choose_mephysto][0]
mephysto_dose = relative_dose[choose_mephysto][0]
interpolation = scipy.interpolate.interp1d(mephysto_pdd_depth,
mephysto_dose)
mephysto_pdd_dose = (mephysto_dose /
interpolation(depth_of_absolute_dose_mm) *
absolute_dose)
return mephysto_pdd_depth, mephysto_pdd_dose
def get_grid(
max_leaf_gap=__DEFAULT_MAX_LEAF_GAP,
grid_resolution=__DEFAULT_GRID_RESOLUTION,
leaf_pair_widths=__DEFAULT_LEAF_PAIR_WIDTHS,
):
"""Get the MU Density grid for plotting purposes.
Examples
--------
See `pymedphys.mudensity.calculate`_.
"""
leaf_pair_widths = np.array(leaf_pair_widths)
grid = dict()
grid["mlc"] = np.arange(
-max_leaf_gap / 2, max_leaf_gap / 2 + grid_resolution, grid_resolution
).astype("float")
_, top_of_reference_leaf = _determine_leaf_centres(leaf_pair_widths)
grid_reference_position = _determine_reference_grid_position(
top_of_reference_leaf, grid_resolution
)
# It might be better to use round instead of ceil here.
total_leaf_widths = np.sum(leaf_pair_widths)
top_grid_pos = (
np.ceil((total_leaf_widths / 2 - grid_reference_position) / grid_resolution)
* grid_resolution
+ grid_reference_position
)
bot_grid_pos = (
grid_reference_position
- np.ceil((total_leaf_widths / 2 + grid_reference_position) / grid_resolution)
* grid_resolution
)
grid["jaw"] = np.arange(
bot_grid_pos, top_grid_pos + grid_resolution, grid_resolution
)
return grid
def calc_and_merge_logfile_mudensity(filepaths, grid_resolution=1):
logfile_results = []
for filepath in filepaths:
logfile_delivery_data = pymedphys.Delivery.from_logfile(filepath)
mu_density_results = mu_density_from_delivery_data(
logfile_delivery_data, grid_resolution=grid_resolution
)
logfile_results.append(mu_density_results)
grid_xx_list = [result[0] for result in logfile_results]
grid_yy_list = [result[1] for result in logfile_results]
# assert np.array_equal(*grid_xx_list)
# assert np.array_equal(*grid_yy_list)
grid_xx = grid_xx_list[0]
grid_yy = grid_yy_list[0]
mu_densities = [result[2] for result in logfile_results]
logfile_mu_density = np.sum(mu_densities, axis=0)
return grid_xx, grid_yy, logfile_mu_density
def image_analyze(volume, i_opt):
xfield = []
yfield = []
rotfield = []
if i_opt.startswith(("y", "yeah", "yes")):
kx = 0
ky = 0
krot = 0
for item in range(0, volume.shape[2]):
stack1 = np.sum(
volume[
int(
np.shape(volume)[0] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[0] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
int(
np.shape(volume)[1] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[1] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
item,
],
axis=0,
)
maxstack1 = np.amax(stack1)
# stack2 = np.sum(volume[:, :, item], axis=1)
stack2 = np.sum(
volume[
int(
np.shape(volume)[0] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[0] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
int(
np.shape(volume)[1] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[1] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
item,
],
axis=1,
)
maxstack2 = np.amax(stack2)
if maxstack2 / maxstack1 > 1.1: # It is a Y field folder
if ky == 0:
yfield = volume[:, :, item]
yfield = yfield[:, :, np.newaxis]
else:
volappend = volume[:, :, item]
yfield = np.append(yfield, volappend[:, :, np.newaxis], axis=2)
ky = ky + 1
elif maxstack2 / maxstack1 < 0.9: # It is a X field folder
if kx == 0:
xfield = volume[:, :, item]
xfield = xfield[:, :, np.newaxis]
else:
# xfield=xfield[:,:,np.newaxis]
volappend = volume[:, :, item]
xfield = np.append(xfield, volappend[:, :, np.newaxis], axis=2)
kx = kx + 1
else: # It is a field rotation folder
if krot == 0:
rotfield = volume[:, :, item]
rotfield = rotfield[:, :, np.newaxis]
else:
# rotfield = rotfield[:, :, np.newaxis]
volappend = volume[:, :, item]
rotfield = np.append(rotfield, volappend[:, :, np.newaxis], axis=2)
krot = krot + 1
else:
kx = 0
ky = 0
krot = 0
for item in range(0, volume.shape[2]):
stack1 = np.sum(
volume[
int(
np.shape(volume)[0] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[0] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
int(
np.shape(volume)[1] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[1] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
item,
],
axis=0,
)
maxstack1 = np.amax(stack1)
# stack2 = np.sum(volume[:, :, item], axis=1)
stack2 = np.sum(
volume[
int(
np.shape(volume)[0] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[0] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
int(
np.shape(volume)[1] / 2
- np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
) : int(
np.shape(volume)[1] / 2
+ np.amin([np.shape(volume)[0], np.shape(volume)[1]]) / 2
),
item,
],
axis=1,
)
maxstack2 = np.amax(stack2)
if maxstack2 / maxstack1 > 1.5: # It is a Y field folder
if ky == 0:
yfield = volume[:, :, item]
yfield = yfield[:, :, np.newaxis]
else:
volappend = volume[:, :, item]
yfield = np.append(yfield, volappend[:, :, np.newaxis], axis=2)
ky = ky + 1
elif maxstack2 / maxstack1 < 0.5: # It is a X field folder
if kx == 0:
xfield = volume[:, :, item]
xfield = xfield[:, :, np.newaxis]
else:
# xfield=xfield[:,:,np.newaxis]
volappend = volume[:, :, item]
xfield = np.append(xfield, volappend[:, :, np.newaxis], axis=2)
kx = kx + 1
else: # It is a field rotation folder
if krot == 0:
rotfield = volume[:, :, item]
rotfield = rotfield[:, :, np.newaxis]
else:
# rotfield = rotfield[:, :, np.newaxis]
volappend = volume[:, :, item]
rotfield = np.append(rotfield, volappend[:, :, np.newaxis], axis=2)
krot = krot + 1
return xfield, yfield, rotfield
def minimize_junction_X(amplitude, peaks, peak_type, dx):
print("Analyzing X jaws...")
amp_prev = 0
amp_filt_prev = 0
fig = plt.figure(figsize=(10, 6)) # create the plot
kk = 0 # counter for figure generation
for j in range(0, amplitude.shape[1] - 1):
for k in range(j + 1,
amplitude.shape[1]): # looping through remaining images
amp_base_res = signal.convolve(amplitude[:, j],
amplitude[:, j],
mode="full")
amp_base_res = signal.resample(
amp_base_res / np.amax(amp_base_res),
int(np.ceil(len(amp_base_res) / 2)),
)
amp_overlay_res = signal.convolve(amplitude[:, k],
amplitude[:, k],
mode="full")
amp_overlay_res = signal.resample(
amp_overlay_res / np.amax(amp_overlay_res),
int(np.ceil(len(amp_overlay_res) / 2)),
)
peak1, _ = find_peaks(amp_base_res, prominence=0.5)
peak2, _ = find_peaks(amp_overlay_res, prominence=0.5)
if (abs(peak2 - peak1) < 2500
): # if the two peaks are close together proceeed to analysis
kk = kk + 1 # incrementing the figure generator
cumsum_prev = 1e7
if peak2 < peak1: # this guarantee that we always slide the overlay
amp_base_res = amplitude[:, k]
amp_overlay_res = amplitude[:, j]
else:
amp_base_res = amplitude[:, j]
amp_overlay_res = amplitude[:, k]
if peak_type[j] == 0:
inc = -1
else:
inc = 1
for i in range(0, inc * 80, inc * 1):
# x = np.linspace(0, 0 + (len(amp_base_res) * dx), len(amplitude),
# endpoint=False) # definition of the distance axis
amp_overlay_res_roll = np.roll(amp_overlay_res, i)
# amplitude is the vector to analyze +-500 samples from the center
amp_tot = (
amp_base_res[peaks[j] - 1000:peaks[j] + 1000] +
amp_overlay_res_roll[peaks[j] - 1000:peaks[j] + 1000]
) # divided by 2 to normalize
# xsel = x[peaks[j] - 1000:peaks[j] + 1000]
amp_filt = rm.running_mean(amp_tot, 281)
cumsum = np.sum(np.abs(amp_tot - amp_filt))
if ( # pylint: disable = no-else-break
cumsum > cumsum_prev): # then we went too far
break
else:
amp_prev = amp_tot
amp_filt_prev = amp_filt
cumsum_prev = cumsum
ax = fig.add_subplot(amplitude.shape[1] - 1, 1, kk)
ax.plot(amp_prev)
ax.plot(amp_filt_prev)
if kk == 1:
ax.set_title("Minimization result", fontsize=16)
if (kk == amplitude.shape[1] - 1
): # if we reach the final plot the add the x axis label
ax.set_xlabel("distance [mm]")
ax.set_ylabel("amplitude")
# ax.annotate('delta=' + str(abs(i - inc * 1) * dx) + ' mm', xy=(2, 1), xycoords='axes fraction',
# xytext=(.35, .10))
if peaks[kk - 1] != 0:
ax.annotate(
"delta=" + str(abs(i - inc * 1) * dx) + " mm",
xy=(2, 1),
xycoords="axes fraction",
xytext=(0.35, 0.10),
)
else:
ax.annotate(
"delta= 0 mm (NO PEAK FOUND)",
xy=(2, 1),
xycoords="axes fraction",
xytext=(0.35, 0.10),
)
return fig
def _orientation_is_head_first(orientation_vector, is_decubitus):
if is_decubitus:
return np.abs(np.sum(orientation_vector)) != 2
return np.abs(np.sum(orientation_vector)) == 2
def main():
st.write("""
# Electron Insert Factors
""")
patient_id = st.text_input("Patient ID")
if patient_id == "":
st.stop()
rccc_string_search_pattern = r"\\monacoda\FocalData\RCCC\1~Clinical\*~{}\plan\*\*tel.1".format(
patient_id)
rccc_filepath_list = glob(rccc_string_search_pattern)
nbccc_string_search_pattern = r"\\tunnel-nbcc-monaco\FOCALDATA\NBCCC\1~Clinical\*~{}\plan\*\*tel.1".format(
patient_id)
nbccc_filepath_list = glob(nbccc_string_search_pattern)
sash_string_search_pattern = r"\\tunnel-sash-monaco\Users\Public\Documents\CMS\FocalData\SASH\1~Clinical\*~{}\plan\*\*tel.1".format(
patient_id)
sash_filepath_list = glob(sash_string_search_pattern)
filepath_list = np.concatenate(
[rccc_filepath_list, nbccc_filepath_list, sash_filepath_list])
electronmodel_regex = r"RiverinaAgility - (\d+)MeV"
applicator_regex = r"(\d+)X\d+"
insert_data = dict() # type: ignore
for telfilepath in filepath_list:
insert_data[telfilepath] = dict()
with open(telfilepath, "r") as file:
telfilecontents = np.array(file.read().splitlines())
insert_data[telfilepath]["reference_index"] = []
for i, item in enumerate(telfilecontents):
if re.search(electronmodel_regex, item):
insert_data[telfilepath]["reference_index"] += [i]
insert_data[telfilepath]["applicators"] = [
re.search(applicator_regex,
telfilecontents[i + 12]).group(1) # type: ignore
for i in insert_data[telfilepath]["reference_index"]
]
insert_data[telfilepath]["energies"] = [
re.search(electronmodel_regex,
telfilecontents[i]).group(1) # type: ignore
for i in insert_data[telfilepath]["reference_index"]
]
for telfilepath in filepath_list:
with open(telfilepath, "r") as file:
telfilecontents = np.array(file.read().splitlines())
insert_data[telfilepath]["x"] = []
insert_data[telfilepath]["y"] = []
for i, index in enumerate(insert_data[telfilepath]["reference_index"]):
insert_initial_range = telfilecontents[
index +
51::] # coords start 51 lines after electron model name
insert_stop = np.where(insert_initial_range == "0")[0][
0] # coords stop right before a line containing 0
insert_coords_string = insert_initial_range[:insert_stop]
insert_coords = np.fromstring(",".join(insert_coords_string),
sep=",")
insert_data[telfilepath]["x"].append(insert_coords[0::2] / 10)
insert_data[telfilepath]["y"].append(insert_coords[1::2] / 10)
for telfilepath in filepath_list:
insert_data[telfilepath]["width"] = []
insert_data[telfilepath]["length"] = []
insert_data[telfilepath]["circle_centre"] = []
insert_data[telfilepath]["P/A"] = []
for i in range(len(insert_data[telfilepath]["reference_index"])):
width, length, circle_centre = electronfactors.parameterise_insert(
insert_data[telfilepath]["x"][i],
insert_data[telfilepath]["y"][i])
insert_data[telfilepath]["width"].append(width)
insert_data[telfilepath]["length"].append(length)
insert_data[telfilepath]["circle_centre"].append(circle_centre)
insert_data[telfilepath]["P/A"].append(
electronfactors.convert2_ratio_perim_area(width, length))
data_filename = r"S:\Physics\RCCC Specific Files\Dosimetry\Elekta_EFacs\electron_factor_measured_data.csv"
data = pd.read_csv(data_filename)
width_data = data["Width (cm @ 100SSD)"]
length_data = data["Length (cm @ 100SSD)"]
factor_data = data["RCCC Inverse factor (dose open / dose cutout)"]
p_on_a_data = electronfactors.convert2_ratio_perim_area(
width_data, length_data)
for telfilepath in filepath_list:
insert_data[telfilepath]["model_factor"] = []
for i in range(len(insert_data[telfilepath]["reference_index"])):
applicator = float(insert_data[telfilepath]["applicators"][i])
energy = float(insert_data[telfilepath]["energies"][i])
ssd = 100
reference = ((data["Energy (MeV)"] == energy)
& (data["Applicator (cm)"] == applicator)
& (data["SSD (cm)"] == ssd))
number_of_measurements = np.sum(reference)
if number_of_measurements < 8:
insert_data[telfilepath]["model_factor"].append(np.nan)
else:
insert_data[telfilepath]["model_factor"].append(
electronfactors.spline_model_with_deformability(
insert_data[telfilepath]["width"],
insert_data[telfilepath]["P/A"],
width_data[reference],
p_on_a_data[reference],
factor_data[reference],
)[0])
for telfilepath in filepath_list:
st.write("---")
st.write("Filepath: `{}`".format(telfilepath))
for i in range(len(insert_data[telfilepath]["reference_index"])):
applicator = float(insert_data[telfilepath]["applicators"][i])
energy = float(insert_data[telfilepath]["energies"][i])
ssd = 100
st.write("Applicator: `{} cm` | Energy: `{} MeV`".format(
applicator, energy))
width = insert_data[telfilepath]["width"][i]
length = insert_data[telfilepath]["length"][i]
plt.figure()
plot_insert(
insert_data[telfilepath]["x"][i],
insert_data[telfilepath]["y"][i],
insert_data[telfilepath]["width"][i],
insert_data[telfilepath]["length"][i],
insert_data[telfilepath]["circle_centre"][i],
)
reference = ((data["Energy (MeV)"] == energy)
& (data["Applicator (cm)"] == applicator)
& (data["SSD (cm)"] == ssd))
number_of_measurements = np.sum(reference)
plt.figure()
if number_of_measurements < 8:
plt.scatter(
width_data[reference],
length_data[reference],
s=100,
c=factor_data[reference],
cmap="viridis",
zorder=2,
)
plt.colorbar()
else:
plot_model(
width_data[reference],
length_data[reference],
factor_data[reference],
)
reference_data_table = pd.concat(
[
width_data[reference], length_data[reference],
factor_data[reference]
],
axis=1,
)
reference_data_table.sort_values(
["RCCC Inverse factor (dose open / dose cutout)"],
ascending=False,
inplace=True,
)
st.write(reference_data_table)
st.pyplot()
factor = insert_data[telfilepath]["model_factor"][i]
st.write(
"Width: `{0:0.2f} cm` | Length: `{1:0.2f} cm` | Factor: `{2:0.3f}`"
.format(width, length, factor))
def minimize_junction_fieldrot(
amplitude, peaks, peak_type, dx, profilename
): # minimize junction for field rotations is done differently given the shape of the fields
print("Field rotation jaw analysis...")
# print('number of peaks=', peaks)
amp_prev = 0
amp_filt_prev = 0
fig = plt.figure(figsize=(10, 6)) # create the plot
kk = 1 # counter for figure generation
for j in range(0, amplitude.shape[1] - 1):
for k in range(j + 1,
amplitude.shape[1]): # looping through remaining images
amp_base_res = signal.convolve(amplitude[:, j],
amplitude[:, j],
mode="full")
amp_base_res = signal.resample(
amp_base_res / np.amax(amp_base_res),
int(np.ceil(len(amp_base_res) / 2)),
)
amp_overlay_res = signal.convolve(amplitude[:, k],
amplitude[:, k],
mode="full")
amp_overlay_res = signal.resample(
amp_overlay_res / np.amax(amp_overlay_res),
int(np.ceil(len(amp_overlay_res) / 2)),
)
# amp_base_res = signal.savgol_filter(amplitude[:, j], 1001, 3)
# amp_overlay_res = signal.savgol_filter(amplitude[:, k], 1001, 3)
# peak1, _ = find_peaks(amp_base_res, prominence=0.5)
# peak2, _ = find_peaks(amp_overlay_res, prominence=0.5)
cumsum_prev = 1e7
amp_base_res = amplitude[:, j]
amp_overlay_res = amplitude[:, k]
if peak_type[j] == 0:
inc = -1
else:
inc = 1
for i in range(0, inc * 80, inc * 1):
# x = np.linspace(0, 0 + (len(amp_base_res) * dx), len(amplitude),
# endpoint=False) # definition of the distance axis
amp_overlay_res_roll = np.roll(amp_overlay_res, i)
# amplitude is the vector to analyze +-500 samples from the center
amp_tot = (
amp_base_res[peaks[j] - 1000:peaks[j] + 1000] +
amp_overlay_res_roll[peaks[j] - 1000:peaks[j] + 1000]
) # divided by 2 to normalize
# xsel = x[peaks[j] - 1000:peaks[j] + 1000]
amp_filt = rm.running_mean(amp_tot, 281)
cumsum = np.sum(np.abs(amp_tot - amp_filt))
if ( # pylint: disable = no-else-break
cumsum > cumsum_prev): # then we went too far
ax = fig.add_subplot(amplitude.shape[1] - 1, 1, kk)
ax.plot(amp_prev)
ax.plot(amp_filt_prev)
if kk == 1:
ax.set_title("Minimization result - " + profilename,
fontsize=16)
if (
kk == amplitude.shape[1] - 1
): # if we reach the final plot the add the x axis label
ax.set_xlabel("distance [mm]")
ax.set_ylabel("amplitude")
ax.annotate(
"delta=" + str(abs(i - inc * 1) * dx) + " mm",
xy=(2, 1),
xycoords="axes fraction",
xytext=(0.35, 0.10),
)
# plt.show()
kk = kk + 1
break
else:
amp_prev = amp_tot
amp_filt_prev = amp_filt
cumsum_prev = cumsum
return fig
def to_minimise(x):
a, b, n = x
cal_fit = create_cal_fit(a, b, n)
return np.sum((cal_fit(net_od) - dose)**2)
def calculate_pass_rate(gamma_array):
valid_gamma = gamma_array[np.invert(np.isnan(gamma_array))]
percent_pass = 100 * np.sum(valid_gamma < 1) / len(valid_gamma)
return percent_pass
def calc_single_control_point(
mlc,
jaw,
delivered_mu=1,
leaf_pair_widths=__DEFAULT_LEAF_PAIR_WIDTHS,
grid_resolution=__DEFAULT_GRID_RESOLUTION,
min_step_per_pixel=__DEFAULT_MIN_STEP_PER_PIXEL,
):
"""Calculate the MU Density for a single control point.
Examples
--------
>>> from pymedphys._imports import numpy as np
>>> from pymedphys._mudensity.mudensity import (
... calc_single_control_point, display_mu_density)
>>>
>>> leaf_pair_widths = (2, 2)
>>> mlc = np.array([
... [
... [1, 1],
... [2, 2],
... ],
... [
... [2, 2],
... [3, 3],
... ]
... ])
>>> jaw = np.array([
... [1.5, 1.2],
... [1.5, 1.2]
... ])
>>> grid, mu_density = calc_single_control_point(
... mlc, jaw, leaf_pair_widths=leaf_pair_widths)
>>> display_mu_density(grid, mu_density)
>>>
>>> grid['mlc']
array([-3., -2., -1., 0., 1., 2., 3.])
>>>
>>> grid['jaw']
array([-1.5, -0.5, 0.5, 1.5])
>>>
>>> np.round(mu_density, 2)
array([[0. , 0.07, 0.43, 0.5 , 0.43, 0.07, 0. ],
[0. , 0.14, 0.86, 1. , 0.86, 0.14, 0. ],
[0.14, 0.86, 1. , 1. , 1. , 0.86, 0.14],
[0.03, 0.17, 0.2 , 0.2 , 0.2 , 0.17, 0.03]])
"""
leaf_pair_widths = np.array(leaf_pair_widths)
leaf_division = leaf_pair_widths / grid_resolution
if not np.all(leaf_division.astype(int) == leaf_division):
raise ValueError(
"The grid resolution needs to exactly divide every leaf pair width."
)
if (
not np.max(np.abs(jaw)) # pylint: disable = unneeded-not
<= np.sum(leaf_pair_widths) / 2
):
raise ValueError(
"The jaw should not travel further out than the maximum leaf limits. "
f"Max travel was {np.max(np.abs(jaw))}"
)
(grid, grid_leaf_map, mlc) = _determine_calc_grid_and_adjustments(
mlc, jaw, leaf_pair_widths, grid_resolution
)
positions = {
"mlc": {
1: (-mlc[0, :, 0], -mlc[1, :, 0]), # left
-1: (mlc[0, :, 1], mlc[1, :, 1]), # right
},
"jaw": {
1: (-jaw[0::-1, 0], -jaw[1::, 0]), # bot
-1: (jaw[0::-1, 1], jaw[1::, 1]), # top
},
}
time_steps = _calc_time_steps(positions, grid_resolution, min_step_per_pixel)
blocked_by_device = _calc_blocked_by_device(
grid, positions, grid_resolution, time_steps
)
device_open = _calc_device_open(blocked_by_device)
mlc_open, jaw_open = _remap_mlc_and_jaw(device_open, grid_leaf_map)
open_fraction = _calc_open_fraction(mlc_open, jaw_open)
mu_density = open_fraction * delivered_mu
return grid, mu_density
