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skytest.py
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from osgeo import gdal
import numpy as np
import os
import warnings
import csv
import math
import datetime
import numba
import sys
from memory_profiler import profile
import shadowing
# Notes:
# Shading is memory intensive (lots of copies of the array), Shadowing is processor intensive.
# Numba jit'ing the monolithic skymodel doesn't speed it up by much- just jit'ing shade is fine.
# putting it into a single loop slows it down even further- 34s vs 24s for non-monolithic
# The "return shaded*255" line holds onto a lot of memory- put the *255 in the body of the method.
def sizeof_fmt(num, suffix='B'):
'''
Quick-and-dirty method for formating file size, from Sridhar Ratnakumar,
https://stackoverflow.com/questions/1094841/reusable-library-to-get-human-readable-version-of-file-size.
'''
for unit in ['', 'Ki', 'Mi', 'Gi', 'Ti', 'Pi', 'Ei', 'Zi']:
if abs(num) < 1024.0:
return "%3.1f %s%s" % (num, unit, suffix)
num /= 1024.0
return "%.1f %s%s" % (num, 'Yi', suffix)
@numba.jit("f8[:,:](f4[:,:],f8,f8,f8,f8)", nopython=True)
def hillshade_numba(in_array, az, alt, res, nodata):
'''
Custom implmentation of hillshading, using the algorithm from the source
code for gdaldem. The inputs and outputs are the same as in gdal or ArcGIS.
in_array: The input array, should be read using the supper_array
technique from below.
az: The sun's azimuth, in degrees.
alt: The sun's altitude, in degrees.
scale: When true, stretches the result to 1-255. CAUTION: If using
as part of a parallel or multi-chunk process, each chunk
has different min and max values, which leads to different
stretching for each chunk.
'''
# Create new array with s_nodata values set to np.nan (for edges)
nan_array = np.where(in_array == nodata, np.nan, in_array)
# Initialize shaded array to 0s
shaded = np.zeros(nan_array.shape)
# Conversion between mathematical and nautical azimuth
az = 90. - az
azrad = az * np.pi / 180.
altrad = alt * np.pi / 180.
sinalt = np.sin(altrad)
cosaz = np.cos(azrad)
cosalt = np.cos(altrad)
sinaz = np.sin(azrad)
rows = nan_array.shape[0]
cols = nan_array.shape[1]
for i in range(1, rows-1): # ignoring edges right now by subsetting
for j in range(1, cols-1):
window = nan_array[i-1:i+2, j-1:j+2].flatten()
x = ((window[2] + 2. * window[5] + window[8]) -
(window[0] + 2. * window[3] + window[6])) / (8. * res)
y = ((window[6] + 2. * window[7] + window[8]) -
(window[0] + 2. * window[1] + window[2])) / (8. * res)
xx_plus_yy = x * x + y * y
alpha = y * cosaz * cosalt - x * sinaz * cosalt
shade = (sinalt - alpha) / np.sqrt(1 + xx_plus_yy)
shaded[i,j] = shade * 255
# scale from 0-1 to 0-255
return shaded
#@profile
def hillshade(in_array, az, alt, res, nodata):
'''
Custom implmentation of hillshading, using the algorithm from the source
code for gdaldem. The inputs and outputs are the same as in gdal or ArcGIS.
in_array: The input array, should be read using the supper_array
technique from below.
az: The sun's azimuth, in degrees.
alt: The sun's altitude, in degrees.
scale: When true, stretches the result to 1-255. CAUTION: If using
as part of a parallel or multi-chunk process, each chunk
has different min and max values, which leads to different
stretching for each chunk.
'''
# Create new array wsith s_nodata values set to np.nan (for edges)
nan_array = np.where(in_array == nodata, np.nan, in_array)
# x = np.zeros(nan_array.shape)
# y = np.zeros(nan_array.shape)
# Conversion between mathematical and nautical azimuth
az = 90. - az
azrad = az * np.pi / 180.
altrad = alt * np.pi / 180.
x, y = np.gradient(nan_array, res, res, edge_order=2)
nan_array = None
sinalt = np.sin(altrad)
cosaz = np.cos(azrad)
cosalt = np.cos(altrad)
sinaz = np.sin(azrad)
xx_plus_yy = x * x + y * y
alpha = y * cosaz * cosalt - x * sinaz * cosalt
x = None
y = None
shaded = (sinalt - alpha) / np.sqrt(1 + xx_plus_yy) * 255
# print('')
# print("Locals")
# for var, obj in locals().items():
# print(var, sizeof_fmt(sys.getsizeof(obj)))
# print("\nGlobals")
# for var, obj in globals().items():
# print(var, sizeof_fmt(sys.getsizeof(obj)))
# scale from 0-1 to 0-255
return shaded# * 255
@numba.jit(nopython=True)
def skymodel_numba(in_array, lum_lines, res, nodata):#, cell_size):
'''
Creates a unique hillshade based on a skymodel, implmenting the method
defined in Kennelly and Stewart (2014), A Uniform Sky Illumination Model to
Enhance Shading of Terrain and Urban Areas.
in_array: The input array, should be read using the supper_array
technique from below.
lum_lines: The azimuth, altitude, and weight for each iteration of the
hillshade. Stored as an array lines, with each line being
an array of [az, alt, weight].
'''
# initialize skyshade as 0's
skyshade = np.zeros((in_array.shape))
# If it's all NoData, just return an array of 0's
if in_array.mean() == nodata:
return skyshade
# Multiply by 5 per K & S
in_array *= 5
# Loop through luminance file lines to calculate multiple hillshades
for l in range(0, lum_lines.shape[0]):
#for line in lum_lines:
az = lum_lines[l, 0]
alt = lum_lines[l, 1]
weight = lum_lines[l, 2]
# print("shading...")
# Hillshade variables
nan_array = np.where(in_array == nodata, np.nan, in_array)
# Initialize shaded array to 0s
shaded = np.zeros(nan_array.shape)
# Conversion between mathematical and nautical azimuth
az = 90. - az
azrad = az * np.pi / 180.
altrad = alt * np.pi / 180.
sinalt = math.sin(altrad)
cosaz = math.cos(azrad)
cosalt = math.cos(altrad)
sinaz = math.sin(azrad)
rows = nan_array.shape[0]
cols = nan_array.shape[1]
# Shadow variables
delta_j = math.cos(azrad)
delta_i = -1. * math.sin(azrad)
tanaltrad = math.tan(altrad)
mult_size = 1
max_steps = 200
shadow_array = np.ones(in_array.shape) # init to 1 (not shadowed), change to 0 if shadowed
max_elev = np.max(in_array)
# Just loop once, doing both hillshade and shadow
for i in range(1, rows-1): # ignoring edges right now by subsetting
for j in range(1, cols-1):
# ===================
# Hillshade algorithm
window = nan_array[i-1:i+2, j-1:j+2].flatten()
x = ((window[2] + 2. * window[5] + window[8]) -
(window[0] + 2. * window[3] + window[6])) / (8. * res)
y = ((window[6] + 2. * window[7] + window[8]) -
(window[0] + 2. * window[1] + window[2])) / (8. * res)
xx_plus_yy = x * x + y * y
alpha = y * cosaz * cosalt - x * sinaz * cosalt
shade = (sinalt - alpha) / np.sqrt(1 + xx_plus_yy)
shaded[i,j] = shade * 255
# ================
# Shadow algorithm
point_elev = in_array[i, j] # the point we want to determine if in shadow
# start calculating next point from the source point
prev_i = i
prev_j = j
# shadow = 1 # 0 if shadowed, 1 if not
for p in range(0, max_steps):
# Figure out next point along the path
next_i = prev_i + delta_i * p * mult_size
next_j = prev_j + delta_j * p * mult_size
# Update prev_i/j for next go-around
prev_i = next_i
prev_j = next_j
# We need integar indexes for the array
idx_i = int(round(next_i))
idx_j = int(round(next_j))
# distance for elevation check is distance in cells (idx_i/j), not distance along the path
# critical height is the elevation that is directly in the path of the sun at given alt/az
idx_distance = math.sqrt((i - idx_i)**2 + (j - idx_j)**2)
# path_distance = math.sqrt((i - next_i)**2 + (j - next_j)**2)
critical_height = idx_distance * tanaltrad * res + point_elev
in_bounds = idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols
in_height = critical_height < max_elev
# in_distance = path_distance * res < max_distance
if in_bounds and in_height: # and in_distance:
next_elev = in_array[idx_i, idx_j]
if next_elev > point_elev and next_elev > critical_height:
shadow_array[i, j] = 0
# print(p)
break # We're done with this point, move on to the next
# weight the shaded array (mult is cummutative, same as (shadow*shade)*weight)
shaded *= weight
# # print("shadowing...")
# #--- SHADOWS ---
# shadow_array = np.ones(in_array.shape) # init to 1 (not shadowed), change to 0 if shadowed
# max_elev = np.max(in_array)
# # max_distance = 500.
#
# az = 90. - az # convert from 0 = north, cw to 0 = east, ccw
#
# azrad = az * np.pi / 180.
# altrad = alt * np.pi / 180.
# delta_j = math.cos(azrad)
# delta_i = -1. * math.sin(azrad)
# tanaltrad = math.tan(altrad)
#
# mult_size = 1
# max_steps = 200
# for i in range(0, rows):
# for j in range(0, cols):
# point_elev = in_array[i, j] # the point we want to determine if in shadow
# # start calculating next point from the source point
# prev_i = i
# prev_j = j
#
# # shadow = 1 # 0 if shadowed, 1 if not
#
# for p in range(0, max_steps):
# # Figure out next point along the path
# next_i = prev_i + delta_i * p * mult_size
# next_j = prev_j + delta_j * p * mult_size
# # Update prev_i/j for next go-around
# prev_i = next_i
# prev_j = next_j
#
# # We need integar indexes for the array
# idx_i = int(round(next_i))
# idx_j = int(round(next_j))
#
# # distance for elevation check is distance in cells (idx_i/j), not distance along the path
# # critical height is the elevation that is directly in the path of the sun at given alt/az
# idx_distance = math.sqrt((i - idx_i)**2 + (j - idx_j)**2)
# # path_distance = math.sqrt((i - next_i)**2 + (j - next_j)**2)
# critical_height = idx_distance * tanaltrad * res + point_elev
#
# in_bounds = idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols
# in_height = critical_height < max_elev
# # in_distance = path_distance * res < max_distance
#
# if in_bounds and in_height: # and in_distance:
# next_elev = in_array[idx_i, idx_j]
# if next_elev > point_elev and next_elev > critical_height:
# shadow_array[i, j] = 0
# # print(p)
# break # We're done with this point, move on to the next
#shadowed = shadows(in_array, az, alt, res, nodata)
print("combining...")
skyshade = skyshade + shaded * shadow_array
return skyshade
def skymodel(in_array, lum_lines, res, nodata):#, cell_size):
'''
Creates a unique hillshade based on a skymodel, implmenting the method
defined in Kennelly and Stewart (2014), A Uniform Sky Illumination Model to
Enhance Shading of Terrain and Urban Areas.
in_array: The input array, should be read using the supper_array
technique from below.
lum_lines: The azimuth, altitude, and weight for each iteration of the
hillshade. Stored as an array lines, with each line being
an array of [az, alt, weight].
'''
# initialize skyshade as 0's
skyshade = np.zeros((in_array.shape), dtype=np.float32)
# If it's all NoData, just return an array of 0's
if in_array.mean() == nodata:
return skyshade
# Multiply by 5 per K & S
in_array *= 5
i = 1
# Loop through luminance file lines to calculate multiple hillshades
for line in lum_lines:
print(i)
az = line[0]
alt = line[1]
weight = line[2]
# print("shading...")
# shade = hillshade_numba(in_array, az, alt, res, nodata) * weight
shade = hillshade(in_array[:], az, alt, res, nodata) * weight
# print("shadowing...")
shadowed = shadows(in_array, az, alt, res, nodata*5)
# shadowed = shadowing.shadows(in_array, az, alt, res, 0, nodata*5)
# print("combining...")
skyshade += (shade * shadowed)
# print(np.nanmean(skyshade))
# for var, obj in locals().items():
# print(var, sizeof_fmt(sys.getsizeof(obj)))
shade = None
shadowed = None
i += 1
return skyshade
@numba.jit("u1[:,:](f4[:,:],f8,f8,f8,u4,f8)", nopython=True)
def shadows(in_array, az, alt, res, overlap, nodata):
# Rows = i = y values, cols = j = x values
rows = in_array.shape[0]
cols = in_array.shape[1]
shadow_array = np.ones(in_array.shape, dtype=np.uint8) # init to 1 (not shadowed), change to 0 if shadowed
max_elev = np.max(in_array)
# max_distance = 500.
az = 90. - az # convert from 0 = north, cw to 0 = east, ccw
azrad = az * np.pi / 180.
altrad = alt * np.pi / 180.
delta_j = math.cos(azrad) # these are switched sin for cos because of 90-az above
delta_i = -1. * math.sin(azrad) # these are switched sin for cos because of 90-az above
tanaltrad = math.tan(altrad)
oneoverres = 1. / res
# Mult size is in array units, not georef units
mult_size = .5
max_steps = 600
counter = 0
max = rows * cols
# numba jit w/for loop is faster than nditer
# # https://docs.scipy.org/doc/numpy/reference/arrays.nditer.html
# it = np.nditer(in_array, flags=['multi_index'])
# while not it.finished:
# i = it.multi_index[0]
# j = it.multi_index[1]
#
# point_elev = it[0] # the point we want to determine if in shadow
# # start calculating next point from the source point
# prev_i = i
# prev_j = j
#
# for p in range(0, max_steps):
# # Figure out next point along the path
# next_i = prev_i + delta_i * p * mult_size
# next_j = prev_j + delta_j * p * mult_size
# # Update prev_i/j for next go-around
# prev_i = next_i
# prev_j = next_j
#
# # We need integar indexes for the array
# idx_i = int(round(next_i))
# idx_j = int(round(next_j))
#
# # distance for elevation check is distance in cells (idx_i/j), not distance along the path
# # critical height is the elevation that is directly in the path of the sun at given alt/az
# idx_distance = math.sqrt((i - idx_i)**2 + (j - idx_j)**2)
# # path_distance = math.sqrt((i - next_i)**2 + (j - next_j)**2)
# critical_height = idx_distance * tanaltrad * res + point_elev
#
# in_bounds = idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols
# in_height = critical_height < max_elev
# # in_distance = path_distance * res < max_distance
#
# if in_bounds and in_height: # and in_distance:
# next_elev = in_array[idx_i, idx_j]
# if next_elev > point_elev and next_elev > critical_height:
# shadow_array[i, j] = 0
# # print(p)
# break # We're done with this point, move on to the next
# it.iternext()
# return shadow_array
iterations = 0
already_shadowed = 0
# precompute idx distances
distances = []
for d in range(1, max_steps):
# # Figure out next point along the path
# # use i/j + delta_i/j instead of prev_i/j + delta_i/j because step takes care of progression for us
# next_i = (d-1) + delta_i * d * mult_size
# next_j = (d-1) + delta_j * d * mult_size
#
# # We need integar indexes for the array
# idx_i = int(round(next_i))
# idx_j = int(round(next_j))
#
# # distance for elevation check is distance in cells (idx_i/j), not distance along the path
# # critical height is the elevation that is directly in the path of the sun at given alt/az
#
# idx_distance = math.sqrt((idx_i)**2 + (idx_j)**2)
# ids.append(idx_distance)
# distance is just d * resolution (only going in 1-array-unit steps)
distance = d * res
step_height = distance * tanaltrad
i_distance = delta_i * d
j_distance = delta_j * d
distances.append((step_height, i_distance, j_distance))
# # calculate distance in georeff units, i, and j values in array units
# i_distance = delta_i * d * mult_size
# j_distance = delta_j * d * mult_size
# y_distance = i_distance * res
# x_distance = j_distance * res
# y_dist_sq = y_distance**2
# x_dist_sq = x_distance**2
#
# # total_distance = math.sqrt((j_distance*res)**2 + (i_distance*res)**2) * tanaltrad
# total_distance = math.sqrt(x_dist_sq + y_dist_sq) * tanaltrad
# distances.append((total_distance, i_distance, j_distance))
if overlap > 0:
y_start = overlap - 1
y_end = rows - overlap
x_start = overlap - 1
x_end = cols - overlap
else:
y_start = 0
y_end = rows
x_start = 0
x_end = cols
for i in range(y_start, y_end):
for j in range(x_start, x_end):
# keep_going = True
# counter += 1
# elapsed = datetime.datetime.now() - start
# print("{}, {} {}".format(i, j, elapsed))
point_elev = in_array[i, j] # the point we want to determine if in shadow
# start calculating next point from the source point
# shadow = 1 # 0 if shadowed, 1 if not
for step in range(1, max_steps): # start at a step of 1- a point cannot be shadowed by itself
iterations += 1
# No need to continue if it's already shadowed
if shadow_array[i, j] == 0:
already_shadowed += 1
# print("shadow break")
break
# # Figure out next point along the path
# # use i/j + delta_i/j instead of prev_i/j + delta_i/j because step takes care of progression for us
# next_i = i + delta_i * step * mult_size
# next_j = j + delta_j * step * mult_size
#
# # We need integar indexes for the array
# idx_i = int(round(next_i))
# idx_j = int(round(next_j))
#
# # distance for elevation check is distance in cells (idx_i/j), not distance along the path
# # critical height is the elevation that is directly in the path of the sun at given alt/az
# idx_distance = math.sqrt((i - idx_i)**2 + (j - idx_j)**2)
# # path_distance = math.sqrt((i - next_i)**2 + (j - next_j)**2)
# critical_height = idx_distance * tanaltrad * res + point_elev
# critical height, distances[][0] is already in georeffed units
# [step-1] because distance[0] is already one step away from the start
critical_height = distances[step-1][0] + point_elev
# idx_i/j are indices of array corresponding to current position + y/x distances
idx_i = int(round(i + distances[step-1][1]))
idx_j = int(round(j + distances[step-1][2]))
in_bounds = idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols
in_height = critical_height < max_elev
# in_distance = path_distance * res < max_distance
#print(in_bounds)
# set to shaded if out of bounds
# if in_bounds is False:
# shadow_array[i,j] = 0
# break
if in_bounds and in_height: # and in_distance:
next_elev = in_array[idx_i, idx_j]
# Bail out if we hit a nodata area
if next_elev == nodata:
break
if next_elev > point_elev and next_elev > critical_height:
shadow_array[i, j] = 0
# set all array indices in between our found shadowing index and the source index to shadowed
for step2 in range(1, step):
i2 = int(round(i + distances[step2-1][1]))
j2 = int(round(j + distances[step2-1][2]))
shadow_array[i2, j2] = 0
# #print(step)
break # We're done with this point, move on to the next
print(max)
print(iterations)
print(already_shadowed)
return shadow_array
# while keep_going: # this inner loop loops through the possible values for each path
# # Figure out next point along the path
# # delta_j = math.cos(azrad) * res
# # delta_i = math.sin(azrad) * res
# next_i = prev_i + delta_i
# next_j = prev_j + delta_j
# # Update prev_i/j for next go-around
# prev_i = next_i
# prev_j = next_j
#
# # We need integar indexes for the array
# idx_i = int(round(next_i))
# idx_j = int(round(next_j))
#
# shadow = 1 # 0 if shadowed, 1 if not
#
# # distance for elevation check is distance from cell centers (idx_i/j), not distance along the path
# # critical height is the elevation that is directly in the path of the sun at given alt/az
# idx_distance = math.sqrt((i - idx_i)**2 + (j - idx_j)**2)
# path_distance = math.sqrt((i - next_i)**2 + (j - next_j)**2)
# critical_height = idx_distance * tanaltrad * res + point_elev
#
#
# in_bounds = idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols
# in_height = critical_height < max_elev
# in_distance = path_distance * res < max_distance
# #print("{}, {}, {}".format(in_bounds, in_height, in_distance))
#
# if in_bounds and in_height and in_distance:
# # bounds check (array bounds, elevation check)
# # if idx_i >= 0 and idx_i < rows and idx_j >= 0 and idx_j < cols and critical_height < max_elev:
# next_elev = in_array[idx_i, idx_j]
# if next_elev > point_elev: # only check if the next elev is greater than the point elev
# if next_elev > critical_height:
# shadow = 0
# keep_going = False # don't bother continuing to check
#
# else:
# keep_going = False # our next index would be out of bounds, we've reached the edge of the array
#
#
# #print("i:{}, j:{}; idx_i:{}, idx_j:{}; idx_distance:{}, critical_height:{}, delta_i:{}, delta_j:{}".format(i, j, idx_i, idx_j, idx_distance, critical_height, delta_i, delta_j))
#
# shadow_array[i, j] = shadow # assign shadow value to output array
# #print("{}, {}: {}".format(i, j, shadow))
# return shadow_array
# variables
csv_path = r'C:\GIS\Data\Elevation\Uintahs\test2_nohdr.csv'
in_dem_path = r'C:\GIS\Data\Elevation\Uintahs\utest.tif'
# in_dem_path = r'C:\GIS\Data\Elevation\Uintahs\uintahs_fft60_sub.tif'
out_dem_path = r'C:\GIS\Data\Elevation\Uintahs\utest_sky_1x600_test2_jit_old.tif'
alt = 45.
az = 315.
start = datetime.datetime.now()
gdal.UseExceptions()
lines = []
with open(csv_path, 'r') as l:
reader = csv.reader(l)
for line in reader:
lines.append([float(line[0]), float(line[1]), float(line[2])])
nplines = np.zeros((len(lines), 3))
for i in range(0, len(lines)):
for j in range(0,3):
nplines[i,j] = lines[i][j]
# Get source file metadata (dimensions, driver, proj, cell size, nodata)
print("Processing {0:s}...".format(in_dem_path))
s_fh = gdal.Open(in_dem_path, gdal.GA_ReadOnly)
rows = s_fh.RasterYSize
cols = s_fh.RasterXSize
driver = s_fh.GetDriver()
bands = s_fh.RasterCount
s_band = s_fh.GetRasterBand(1)
# Get source georeference info
transform = s_fh.GetGeoTransform()
projection = s_fh.GetProjection()
cell_size = abs(transform[5]) # Assumes square pixels where height=width
s_nodata = s_band.GetNoDataValue()
if os.path.exists(out_dem_path):
raise IOError("Output file {} already exists.".format(out_dem_path))
print("Reading array")
s_data = s_band.ReadAsArray()
print("s_data: {}".format(sizeof_fmt(sys.getsizeof(s_data))))
# Close source file handle
s_band = None
s_fh = None
print("Processing array")
#shade = hillshade_numba(s_data, az, alt, cell_size)
# shadowed = shadows(s_data, az, alt, cell_size)
# mult = shade * shadowed
#sky = skymodel_numba(s_data, nplines, cell_size, s_nodata)
sky = skymodel(s_data[:], lines, cell_size, s_nodata)
# Test is 225 az, 25 alt
# shad = shadows(s_data, az, alt, cell_size)
out_array = sky
print("Writing output array")
# Set up target file in preparation for future writes
# If we've been given a vrt as a source, force the output to be geotiff
if driver.LongName == 'Virtual Raster':
driver = gdal.GetDriverByName('gtiff')
# if os.path.exists(out_dem_path):
# raise IOError("Output file {} already exists.".format(out_dem_path))
lzw_opts = ["compress=lzw", "tiled=yes", "bigtiff=yes"]
t_fh = driver.Create(out_dem_path, cols, rows, bands, gdal.GDT_Float32, options=lzw_opts)
t_fh.SetGeoTransform(transform)
t_fh.SetProjection(projection)
t_band = t_fh.GetRasterBand(1)
if bands == 1:
t_band.SetNoDataValue(s_nodata)
t_band.WriteArray(out_array)
t_band = None
t_fh = None
end = datetime.datetime.now()
print(end - start)