-
Notifications
You must be signed in to change notification settings - Fork 133
/
postprocessor.py
883 lines (742 loc) · 48.1 KB
/
postprocessor.py
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
236
237
238
239
240
241
242
243
244
245
246
247
248
249
250
251
252
253
254
255
256
257
258
259
260
261
262
263
264
265
266
267
268
269
270
271
272
273
274
275
276
277
278
279
280
281
282
283
284
285
286
287
288
289
290
291
292
293
294
295
296
297
298
299
300
301
302
303
304
305
306
307
308
309
310
311
312
313
314
315
316
317
318
319
320
321
322
323
324
325
326
327
328
329
330
331
332
333
334
335
336
337
338
339
340
341
342
343
344
345
346
347
348
349
350
351
352
353
354
355
356
357
358
359
360
361
362
363
364
365
366
367
368
369
370
371
372
373
374
375
376
377
378
379
380
381
382
383
384
385
386
387
388
389
390
391
392
393
394
395
396
397
398
399
400
401
402
403
404
405
406
407
408
409
410
411
412
413
414
415
416
417
418
419
420
421
422
423
424
425
426
427
428
429
430
431
432
433
434
435
436
437
438
439
440
441
442
443
444
445
446
447
448
449
450
451
452
453
454
455
456
457
458
459
460
461
462
463
464
465
466
467
468
469
470
471
472
473
474
475
476
477
478
479
480
481
482
483
484
485
486
487
488
489
490
491
492
493
494
495
496
497
498
499
500
501
502
503
504
505
506
507
508
509
510
511
512
513
514
515
516
517
518
519
520
521
522
523
524
525
526
527
528
529
530
531
532
533
534
535
536
537
538
539
540
541
542
543
544
545
546
547
548
549
550
551
552
553
554
555
556
557
558
559
560
561
562
563
564
565
566
567
568
569
570
571
572
573
574
575
576
577
578
579
580
581
582
583
584
585
586
587
588
589
590
591
592
593
594
595
596
597
598
599
600
601
602
603
604
605
606
607
608
609
610
611
612
613
614
615
616
617
618
619
620
621
622
623
624
625
626
627
628
629
630
631
632
633
634
635
636
637
638
639
640
641
642
643
644
645
646
647
648
649
650
651
652
653
654
655
656
657
658
659
660
661
662
663
664
665
666
667
668
669
670
671
672
673
674
675
676
677
678
679
680
681
682
683
684
685
686
687
688
689
690
691
692
693
694
695
696
697
698
699
700
701
702
703
704
705
706
707
708
709
710
711
712
713
714
715
716
717
718
719
720
721
722
723
724
725
726
727
728
729
730
731
732
733
734
735
736
737
738
739
740
741
742
743
744
745
746
747
748
749
750
751
752
753
754
755
756
757
758
759
760
761
762
763
764
765
766
767
768
769
770
771
772
773
774
775
776
777
778
779
780
781
782
783
784
785
786
787
788
789
790
791
792
793
794
795
796
797
798
799
800
801
802
803
804
805
806
807
808
809
810
811
812
813
814
815
816
817
818
819
820
821
822
823
824
825
826
827
828
829
830
831
832
833
834
835
836
837
838
839
840
841
842
843
844
845
846
847
848
849
850
851
852
853
854
855
856
857
858
859
860
861
862
863
864
865
866
867
868
869
870
871
872
873
874
875
876
877
878
879
880
881
882
883
"""Smoke and mirrors. Glitch artistry. Pixel-space postprocessing effects.
These effects work in linear intensity space, before gamma correction.
"""
__all__ = ["Postprocessor"]
from collections import defaultdict
import logging
import math
import time
from typing import Dict, List, Optional, Tuple, TypeVar, Union
import torch
import torchvision
from tha3.app.util import RunningAverage, luminance, rgb_to_yuv, yuv_to_rgb
logging.basicConfig(level=logging.INFO)
logger = logging.getLogger(__name__)
# # Default configuration for the postprocessor.
# # This documents the correct ordering of the filters.
# # Feel free to improvise, but make sure to understand why your filter chain makes sense.
# default_chain = [
# # physical input signal
# ("bloom", {}),
# # video camera
# ("chromatic_aberration", {}),
# ("vignetting", {}),
# # scifi hologram output
# ("translucency", {}),
# ("alphanoise", {"magnitude": 0.1, "sigma": 0.0}),
# # # lo-fi analog video
# # ("analog_lowres", {}),
# # ("alphanoise", {"magnitude": 0.2, "sigma": 2.0}),
# # ("analog_badhsync", {}),
# # # ("analog_vhsglitches", {}),
# # ("analog_vhstracking", {}),
# # CRT TV output
# ("banding", {}),
# ("scanlines", {})
# ]
default_chain = [] # Overridden by the animator, which sends us the chain.
T = TypeVar("T")
Atom = Union[str, bool, int, float]
MaybeContained = Union[T, List[T], Dict[str, T]]
VHS_GLITCH_BLANK = object() # nonce value, see `analog_vhsglitches`
class Postprocessor:
"""
`chain`: Postprocessor filter chain configuration.
Don't mind the complicated type signature; the format is just::
[(filter_name0, {param0: value0, ...}),
...]
The filter name must be a method of `Postprocessor`, taking in an image, and any number of named parameters.
To use a filter's default parameter values, supply an empty dictionary for the parameters.
The outer `Optional[List[Tuple[...]]]` just formalizes that `chain` may be omitted (to use the built-in
default chain, for testing), and the top-level format that it's an ordered list of filters. The filters
are applied in order, first to last.
The auxiliary type definitions are::
MaybeContained = Union[T, List[T], Dict[str: T]]
Atom = Union[str, bool, int, float]
The leaf value (atom) types are restricted so that filter chain configurations JSON easily.
The leaf values may actually be contained inside arbitrarily nested lists and dicts (with str keys),
which is currently not captured by the type signature (the definition should be recursive).
The chain is stored as `self.chain`. Any modifications to that attribute modify the chain,
taking effect immediately. It is recommended to update the chain atomically, by::
my_postprocessor.chain = my_new_chain
In filter descriptions:
[static] := depends only on input image, no explicit time dependence.
[dynamic] := beside input image, also depends on time. In other words,
produces animation even for a stationary input image.
"""
def __init__(self, device: torch.device, chain: Optional[List[Tuple[str, Dict[str, MaybeContained[Atom]]]]] = None):
# We intentionally keep very little state in this class, for a more FP/REST approach with less bugs.
# Filters for static effects are stateless.
#
# We deviate from FP in that:
# - The filters MUTATE, i.e. they overwrite the image being processed.
# This is to allow optimizing their implementations for memory usage and speed.
# - The filter for a dynamic effect may store state, if needed for performing FPS correction.
self.device = device
if chain is None:
chain = default_chain
self.chain = chain
# Meshgrid cache for geometric position of each pixel
self._yy = None
self._xx = None
self._meshy = None
self._meshx = None
self._prev_h = None
self._prev_w = None
# FPS correction
self.CALIBRATION_FPS = 25 # design FPS for dynamic effects (for automatic FPS correction)
self.stream_start_timestamp = time.time_ns() # for updating frame counter reliably (no accumulation)
self.frame_no = -1 # float, frame counter for *normalized* frame number *at CALIBRATION_FPS*
self.last_frame_no = -1
# Performance measurement
self.render_duration_statistics = RunningAverage()
self.last_report_time = None
# Caches for individual dynamic effects
self.alphanoise_last_image = defaultdict(lambda: None)
self.lumanoise_last_image = defaultdict(lambda: None)
self.vhs_glitch_interval = defaultdict(lambda: 0.0)
self.vhs_glitch_last_frame_no = defaultdict(lambda: 0.0)
self.vhs_glitch_last_image = defaultdict(lambda: None)
self.vhs_glitch_last_mask = defaultdict(lambda: None)
self.shift_distort_interval = defaultdict(lambda: 0.0)
self.shift_distort_last_frame_no = defaultdict(lambda: 0.0)
self.shift_distort_grid = defaultdict(lambda: None)
def render_into(self, image):
"""Apply current postprocess chain, modifying `image` in-place."""
time_render_start = time.time_ns()
c, h, w = image.shape
if h != self._prev_h or w != self._prev_w:
logger.info(f"render_into: Computing pixel position tensors for image size {w}x{h}")
# Compute base meshgrid for the geometric position of each pixel.
# This is needed by filters that either vary by geometric position (e.g. `vignetting`),
# or deform the image (e.g. `analog_badhsync`).
#
# This postprocessor is typically applied to a video stream. As long as
# the image dimensions stay constant, we can re-use the previous meshgrid.
#
# We don't strictly keep state here - we just cache. :P
# Seems the deformation geometry must be float32 no matter the image data type.
self._yy = torch.linspace(-1.0, 1.0, h, dtype=torch.float32, device=self.device)
self._xx = torch.linspace(-1.0, 1.0, w, dtype=torch.float32, device=self.device)
self._meshy, self._meshx = torch.meshgrid((self._yy, self._xx), indexing="ij")
self._prev_h = h
self._prev_w = w
logger.info("render_into: Pixel position tensors cached")
# Update the frame counter.
#
# We consider the frame number to be a float, so that dynamic filters can decide what
# to do at fractional frame positions. For continuously animated effects (e.g. banding)
# it makes sense to interpolate continuously, whereas other effects (e.g. scanlines)
# can make their decisions based on the integer part.
#
# As always with floats, we must be careful. Note that we operate in a mindset of robust
# engineering. Since doing the Right Thing here does not cost significantly more engineering
# effort than doing the intuitive but Wrong Thing, it is preferable to go for the proper solution,
# regardless of whether it would take a centuries-long session to actually trigger a failure
# in the less robust approach.
#
# So, floating point accuracy considerations? First, we note that accumulation invites
# disaster in two ways:
#
# - Accumulating the result accumulates also representation error and roundoff error.
# - When accumulating small positive numbers to a sum total, the update eventually
# becomes too small to add, causing the counter to get stuck. (For floats, `x + ϵ = x`
# for sufficiently small ϵ dependent on the magnitude of `x`.)
#
# Fortunately, frame number is a linear function of time, and time diffs can be measured
# precisely. Thus, we can freshly compute the current frame number at each frame, completely
# bypassing the need for accumulation:
#
seconds_since_stream_start = (time_render_start - self.stream_start_timestamp) / 10**9
self.last_frame_no = self.frame_no
self.frame_no = self.CALIBRATION_FPS * seconds_since_stream_start # float!
# That leaves just the questions of how accurate the calculation is, and for how long.
# As to the first question:
#
# - Timestamps are an integer number of nanoseconds, so they are exact.
# - Dividing by 10**9, we move the decimal point. But floats are base-2, so 0.1
# is not representable in IEEE-754. So there will be some small representation error,
# which for float64 likely appears in the ~15th significant digit.
# - Basic arithmetic, such as multiplication, is guaranteed by IEEE-754
# to be accurate to the ULP.
#
# Thus, as the result, we obtain the closest number that is representable in IEEE-754,
# and the strategy works for the whole range of float64.
#
# As for the second question, floats are logarithmically spaced. So if this is left running
# "for long enough" during the same session, accuracy will eventually suffer. Instead of the
# counter getting stuck, however, this will manifest as the frame number updating by more
# than `1.0` each time it updates (i.e. whenever the elapsed number of frames reaches the
# next representable float).
#
# This could be fixed by resetting `stream_start_timestamp` once the frame number
# becomes too large. But in practice, how long does it take for this issue to occur?
# The ULP becomes 1.0 at ~5e15. To reach frame number 5e15, at the reference 25 FPS,
# the time required is 2e14 seconds, i.e. 2.31e9 days, or 6.34 million years.
# While I can almost imagine the eventual bug report, I think it's safe to ignore this.
# Apply the current filter chain.
chain = self.chain # read just once; other threads might reassign it while we're rendering
for filter_name, settings in chain:
apply_filter = getattr(self, filter_name)
apply_filter(image, **settings)
# Measure the performance of the postprocessor.
time_now = time.time_ns()
render_elapsed_sec = (time_now - time_render_start) / 10**9
self.render_duration_statistics.add_datapoint(render_elapsed_sec)
# Log the FPS counter in 5-second intervals.
if (self.last_report_time is None or time_now - self.last_report_time > 5e9):
avg_render_sec = self.render_duration_statistics.average()
msec = round(1000 * avg_render_sec, 1)
fps = round(1 / avg_render_sec, 1) if avg_render_sec > 0.0 else 0.0
logger.info(f"postproc: {msec:.1f}ms [{fps} FPS available]")
self.last_report_time = time_now
# --------------------------------------------------------------------------------
# Physical input signal
def bloom(self, image: torch.tensor, *,
luma_threshold: float = 0.8,
hdr_exposure: float = 0.7) -> None:
"""[static] Bloom effect (fake HDR). Popular in early 2000s anime.
Makes bright parts of the image bleed light into their surroundings, enhancing perceived contrast.
Only makes sense when the talkinghead is rendered on a dark-ish background.
`luma_threshold`: How bright is bright. 0.0 is full black, 1.0 is full white.
(Technically, true relative luminance, not luma, since we work in linear RGB space.)
`hdr_exposure`: Controls the overall brightness of the output. Like in photography,
higher exposure means brighter image (saturating toward white).
"""
# There are online tutorials for how to create this effect, see e.g.:
# https://learnopengl.com/Advanced-Lighting/Bloom
# Find the bright parts.
Y = luminance(image[:3, :, :])
mask = torch.ge(Y, luma_threshold) # [h, w]
# Make a copy of the image with just the bright parts.
mask = torch.unsqueeze(mask, 0) # -> [1, h, w]
brights = image * mask # [c, h, w]
# Blur the bright parts. Two-pass blur to save compute, since we need a very large blur kernel.
# It seems that in Torch, one large 1D blur is faster than looping with a smaller one.
#
# Although everything else in Torch takes (height, width), kernel size is given as (size_x, size_y);
# see `gaussian_blur_image` in https://pytorch.org/vision/main/_modules/torchvision/transforms/v2/functional/_misc.html
# for a hint (the part where it computes the padding).
brights = torchvision.transforms.GaussianBlur((21, 1), sigma=7.0)(brights) # blur along x
brights = torchvision.transforms.GaussianBlur((1, 21), sigma=7.0)(brights) # blur along y
# Additively blend the images. Note we are working in linear intensity space, and we will now go over 1.0 intensity.
image.add_(brights)
# We now have a fake HDR image. Tonemap it back to LDR.
image[:3, :, :] = 1.0 - torch.exp(-image[:3, :, :] * hdr_exposure) # RGB: tonemap
image[3, :, :] = torch.maximum(image[3, :, :], brights[3, :, :]) # alpha: max-combine
torch.clamp_(image, min=0.0, max=1.0)
# --------------------------------------------------------------------------------
# Video camera
def chromatic_aberration(self, image: torch.tensor, *,
transverse_sigma: float = 0.5,
axial_scale: float = 0.005) -> None:
"""[static] Simulate the two types of chromatic aberration in a camera lens.
Like everything else here, this is of course made of smoke and mirrors. We simulate the axial effect
(index of refraction varying w.r.t. wavelength) by geometrically scaling the RGB channels individually,
and the transverse effect (focal distance varying w.r.t. wavelength) by a gaussian blur.
Note that in a real lens:
- Axial CA is typical at long focal lengths (e.g. tele/zoom lens)
- Axial CA increases at high F-stops (low depth of field, i.e. sharp focus at all distances)
- Transverse CA is typical at short focal lengths (e.g. macro lens)
However, in an RGB postproc effect, it is useful to apply both together, to help hide the clear-cut red/blue bands
resulting from the different geometric scalings of just three wavelengths (instead of a continuous spectrum, like
a scene lit with natural light would have).
See:
https://en.wikipedia.org/wiki/Chromatic_aberration
"""
# Axial: Shrink R (deflected less), pass G through (lens reference wavelength), enlarge B (deflected more).
grid_R = torch.stack((self._meshx * (1.0 + axial_scale), self._meshy * (1.0 + axial_scale)), 2)
grid_R = grid_R.unsqueeze(0)
grid_B = torch.stack((self._meshx * (1.0 - axial_scale), self._meshy * (1.0 - axial_scale)), 2)
grid_B = grid_B.unsqueeze(0)
image_batch_R = image[0, :, :].unsqueeze(0).unsqueeze(0) # [h, w] -> [c, h, w] -> [n, c, h, w]
warped_R = torch.nn.functional.grid_sample(image_batch_R, grid_R, mode="bilinear", padding_mode="border", align_corners=False)
warped_R = warped_R.squeeze(0) # [1, c, h, w] -> [c, h, w]
image_batch_B = image[2, :, :].unsqueeze(0).unsqueeze(0)
warped_B = torch.nn.functional.grid_sample(image_batch_B, grid_B, mode="bilinear", padding_mode="border", align_corners=False)
warped_B = warped_B.squeeze(0) # [1, c, h, w] -> [c, h, w]
# Transverse (blur to simulate wrong focal distance for R and B)
warped_R[:, :, :] = torchvision.transforms.GaussianBlur((5, 5), sigma=transverse_sigma)(warped_R)
warped_B[:, :, :] = torchvision.transforms.GaussianBlur((5, 5), sigma=transverse_sigma)(warped_B)
# Alpha channel: treat similarly to each of R,G,B and average the three resulting alpha channels
image_batch_A = image[3, :, :].unsqueeze(0).unsqueeze(0)
warped_A1 = torch.nn.functional.grid_sample(image_batch_A, grid_R, mode="bilinear", padding_mode="border", align_corners=False)
warped_A1[:, :, :] = torchvision.transforms.GaussianBlur((5, 5), sigma=transverse_sigma)(warped_A1)
warped_A2 = torch.nn.functional.grid_sample(image_batch_A, grid_B, mode="bilinear", padding_mode="border", align_corners=False)
warped_A2[:, :, :] = torchvision.transforms.GaussianBlur((5, 5), sigma=transverse_sigma)(warped_A2)
averaged_alpha = (warped_A1 + image[3, :, :] + warped_A2) / 3.0
image[0, :, :] = warped_R
# image[1, :, :] passed through as-is
image[2, :, :] = warped_B
image[3, :, :] = averaged_alpha
def vignetting(self, image: torch.tensor, *,
strength: float = 0.42) -> None:
"""[static] Simulate vignetting (less light hitting the corners of a film frame or CCD sensor).
The profile used here is [cos(strength * d * pi)]**2, where `d` is the distance
from the center, scaled such that `d = 1.0` is reached at the corners.
Thus, at the midpoints of the frame edges, `d = 1 / sqrt(2) ~ 0.707`.
"""
euclidean_distance_from_center = (self._meshy**2 + self._meshx**2)**0.5 / 2**0.5 # [h, w]
brightness = torch.cos(strength * euclidean_distance_from_center * math.pi)**2 # [h, w]
brightness = torch.unsqueeze(brightness, 0) # -> [1, h, w]
image[:3, :, :] *= brightness
# --------------------------------------------------------------------------------
# Scifi hologram
def translucency(self, image: torch.tensor, *,
alpha: float = 0.9) -> None:
"""[static] A simple translucency filter for a hologram look.
Multiplicatively adjusts the alpha channel.
"""
image[3, :, :].mul_(alpha)
# --------------------------------------------------------------------------------
# General use
def alphanoise(self, image: torch.tensor, *,
magnitude: float = 0.1,
sigma: float = 0.0,
name: str = "alphanoise0") -> None:
"""[dynamic] Dynamic noise to alpha channel.
`magnitude`: How much noise to apply. 0 is off, 1 is as much noise as possible.
`sigma`: If nonzero, apply a Gaussian blur to the noise, thus reducing its spatial frequency
(i.e. making larger and smoother "noise blobs").
The blur kernel size is fixed to 5, so `sigma = 1.0` is the largest that will be
somewhat accurate. Nevertheless, `sigma = 2.0` looks acceptable, too, producing
square blobs.
`name`: Optional name for this filter instance in the chain. Used as cache key.
If you have more than one `alphanoise` in the chain, they should have
different names so that each one gets its own cache.
Suggested settings:
Scifi hologram: magnitude=0.1, sigma=0.0
Analog VHS tape: magnitude=0.2, sigma=2.0
"""
# Re-randomize the noise image whenever the normalized frame changes
if self.alphanoise_last_image[name] is None or int(self.frame_no) > int(self.last_frame_no):
c, h, w = image.shape
noise_image = torch.rand(h, w, device=self.device, dtype=image.dtype)
if sigma > 0.0:
noise_image = noise_image.unsqueeze(0) # [h, w] -> [c, h, w] (where c=1)
noise_image = torchvision.transforms.GaussianBlur((5, 5), sigma=sigma)(noise_image)
noise_image = noise_image.squeeze(0) # -> [h, w]
self.alphanoise_last_image[name] = noise_image
else:
noise_image = self.alphanoise_last_image[name]
base_magnitude = 1.0 - magnitude
image[3, :, :].mul_(base_magnitude + magnitude * noise_image)
def lumanoise(self, image: torch.tensor, *,
magnitude: float = 0.1,
sigma: float = 0.0,
name: str = "lumanoise0") -> None:
"""[dynamic] Dynamic noise to luminance, without touching colors or alpha.
Based on converting `image` from RGB to YUV, noising it there, and converting back.
`magnitude`: How much noise to apply. 0 is off, 1 is as much noise as possible.
`sigma`: If nonzero, apply a Gaussian blur to the noise, thus reducing its spatial frequency
(i.e. making larger and smoother "noise blobs").
The blur kernel size is fixed to 5, so `sigma = 1.0` is the largest that will be
somewhat accurate. Nevertheless, `sigma = 2.0` looks acceptable, too, producing
square blobs.
`name`: Optional name for this filter instance in the chain. Used as cache key.
If you have more than one `alphanoise` in the chain, they should have
different names so that each one gets its own cache.
Suggested settings:
Scifi hologram: magnitude=0.1, sigma=0.0
Analog VHS tape: magnitude=0.2, sigma=2.0
"""
# Re-randomize the noise image whenever the normalized frame changes
if self.lumanoise_last_image[name] is None or int(self.frame_no) > int(self.last_frame_no):
c, h, w = image.shape
noise_image = torch.rand(h, w, device=self.device, dtype=image.dtype)
if sigma > 0.0:
noise_image = noise_image.unsqueeze(0) # [h, w] -> [c, h, w] (where c=1)
noise_image = torchvision.transforms.GaussianBlur((5, 5), sigma=sigma)(noise_image)
noise_image = noise_image.squeeze(0) # -> [h, w]
self.lumanoise_last_image[name] = noise_image
else:
noise_image = self.lumanoise_last_image[name]
base_magnitude = 1.0 - magnitude
image_yuv = rgb_to_yuv(image[:3, :, :])
image_yuv[0, :, :].mul_(base_magnitude + magnitude * noise_image)
image_rgb = yuv_to_rgb(image_yuv)
image[:3, :, :] = image_rgb
# --------------------------------------------------------------------------------
# Lo-fi analog video
def analog_lowres(self, image: torch.tensor, *,
kernel_size: int = 5,
sigma: float = 0.75) -> None:
"""[static] Low-resolution analog video signal, simulated by blurring.
`kernel_size`: size of the Gaussian blur kernel, in pixels.
`sigma`: standard deviation of the Gaussian blur kernel, in pixels.
Ideally, `kernel_size` should be `2 * (3 * sigma) + 1`, so that the kernel
reaches its "3 sigma" (99.7% mass) point where the finitely sized kernel
cuts the tail. "2 sigma" (95% mass) is also acceptable, to save some compute.
The default settings create a slight blur without destroying much detail.
"""
image[:, :, :] = torchvision.transforms.GaussianBlur((kernel_size, kernel_size), sigma=sigma)(image)
def analog_badhsync(self, image: torch.tensor, *,
speed: float = 8.0,
amplitude1: float = 0.001, density1: float = 4.0,
amplitude2: Optional[float] = 0.001, density2: Optional[float] = 13.0,
amplitude3: Optional[float] = 0.001, density3: Optional[float] = 27.0) -> None:
"""[dynamic] Analog video signal with fluctuating hsync.
In practice, this looks like a rippling effect added to the outline of the character.
We superpose three waves with different densities (1 / cycle length)
to make the pattern look more irregular.
E.g. density of 2.0 means that two full waves fit into the image height.
Amplitudes are given in units where the height and width of the image
are both 2.0.
`speed`: At speed 1.0, a wave of `density = 1.0` completes a full cycle every
`image_height` frames. So effectively the cycle position updates by
`speed * (1 / image_height)` at each frame.
Note that "frame" here refers to the normalized frame number, at a reference of 25 FPS.
"""
c, h, w = image.shape
# Animation
# FPS correction happens automatically, because `frame_no` is normalized to CALIBRATION_FPS.
cycle_pos = (self.frame_no / h) * speed
cycle_pos = cycle_pos - float(int(cycle_pos)) # fractional part
cycle_pos = 1.0 - cycle_pos # -> motion from top toward bottom
cycle_pos *= 2.0 # full cycle = 2 units
# Deformation
meshy = self._meshy
meshx = self._meshx + amplitude1 * torch.sin((density1 * (self._meshy + cycle_pos)) * math.pi)
if amplitude2 and density2:
meshx = self._meshx + amplitude2 * torch.sin((density2 * (self._meshy + cycle_pos)) * math.pi)
if amplitude3 and density3:
meshx = self._meshx + amplitude3 * torch.sin((density3 * (self._meshy + cycle_pos)) * math.pi)
grid = torch.stack((meshx, meshy), 2)
grid = grid.unsqueeze(0) # batch of one
image_batch = image.unsqueeze(0) # batch of one -> [1, c, h, w]
warped = torch.nn.functional.grid_sample(image_batch, grid, mode="bilinear", padding_mode="border", align_corners=False)
warped = warped.squeeze(0) # [1, c, h, w] -> [c, h, w]
image[:, :, :] = warped
def analog_distort(self, image: torch.tensor, *,
speed: float = 8.0,
strength: float = 0.1,
ripple_amplitude: float = 0.05,
ripple_density1: float = 4.0,
ripple_density2: Optional[float] = 13.0,
ripple_density3: Optional[float] = 27.0,
edge: str = "top") -> None:
"""[dynamic] Analog video signal distorted by a runaway hsync near the top or bottom edge.
A bad video cable connection can do this, e.g. when connecting a game console to a display
with an analog YPbPr component cable 10m in length. In reality, when I ran into this phenomenon,
the distortion only occurred for near-white images, but as glitch art, it looks better if it's
always applied at full strength.
`speed`: At speed 1.0, a full cycle of the rippling effect completes every `image_height` frames.
So effectively the cycle position updates by `speed * (1 / image_height)` at each frame.
`strength`: Base strength for maximum distortion at the edge of the image.
In units where the height and width of the image are both 2.0.
`ripple_amplitude`: Variation on top of `strength`.
`ripple_density1`: Like `density` in `analog_badhsync`, but in time. How many cycles the first
component wave completes per one cycle of the ripple effect.
`ripple_density2`: Like `ripple_density1`, but for the second component wave.
Set to `None` or to 0.0 to disable the second component wave.
`ripple_density3`: Like `ripple_density1`, but for the third component wave.
Set to `None` or to 0.0 to disable the third component wave.
`edge`: one of "top", "bottom". Near which edge of the image to apply the maximal distortion.
The distortion then decays to zero, with a quadratic profile, in 1/8 of the image height.
Note that "frame" here refers to the normalized frame number, at a reference of 25 FPS.
"""
c, h, w = image.shape
# Animation
# FPS correction happens automatically, because `frame_no` is normalized to CALIBRATION_FPS.
cycle_pos = (self.frame_no / h) * speed
cycle_pos = cycle_pos - float(int(cycle_pos)) # fractional part
cycle_pos *= 2.0 # full cycle = 2 units
# Deformation
# The spatial distort profile is a quadratic curve [0, 1], for 1/8 of the image height.
meshy = self._meshy
if edge == "top":
spatial_distort_profile = (torch.clamp(meshy + 0.75, max=0.0) * 4.0)**2 # distort near y = -1
else: # edge == "bottom":
spatial_distort_profile = (torch.clamp(meshy - 0.75, min=0.0) * 4.0)**2 # distort near y = +1
ripple_amplitude = ripple_amplitude
ripple = math.sin(ripple_density1 * cycle_pos * math.pi)
if ripple_density2:
ripple += math.sin(ripple_density2 * cycle_pos * math.pi)
if ripple_density3:
ripple += math.sin(ripple_density3 * cycle_pos * math.pi)
instantaneous_strength = (1.0 - ripple_amplitude) * strength + ripple_amplitude * ripple
# The minus sign: read coordinates toward the left -> shift the image toward the right.
meshx = self._meshx - instantaneous_strength * spatial_distort_profile
# Then just the usual incantation for applying a geometric distortion in Torch:
grid = torch.stack((meshx, meshy), 2)
grid = grid.unsqueeze(0) # batch of one
image_batch = image.unsqueeze(0) # batch of one -> [1, c, h, w]
warped = torch.nn.functional.grid_sample(image_batch, grid, mode="bilinear", padding_mode="border", align_corners=False)
warped = warped.squeeze(0) # [1, c, h, w] -> [c, h, w]
image[:, :, :] = warped
def _vhs_noise(self, image: torch.tensor, *,
height: int) -> torch.tensor:
"""Generate a horizontal band of noise that looks as if it came from a blank VHS tape.
`height`: desired height of noise band, in pixels.
Output is a tensor of shape `[1, height, w]`, where `w` is the width of `image`.
"""
c, h, w = image.shape
# This looks best if we randomize the alpha channel, too.
noise_image = torch.rand(height, w, device=self.device, dtype=image.dtype).unsqueeze(0) # [1, h, w]
# Real VHS noise has horizontal runs of the same color, and the transitions between black and white are smooth.
noise_image = torchvision.transforms.GaussianBlur((5, 1), sigma=2.0)(noise_image)
return noise_image
def analog_vhsglitches(self, image: torch.tensor, *,
strength: float = 0.1,
unboost: float = 4.0,
max_glitches: int = 3,
min_glitch_height: int = 3, max_glitch_height: int = 6,
hold_min: int = 1, hold_max: int = 3,
name: str = "analog_vhsglitches0") -> None:
"""[dynamic] Damaged 1980s VHS video tape, with transient (per-frame) glitching lines.
This leaves the alpha channel alone, so the effect only affects parts that already show something.
This is an artistic interpretation that makes the effect less distracting when used with RGBA data.
`strength`: How much to blend in noise.
`unboost`: Use this to adjust the probability profile for the appearance of glitches.
The higher `unboost` is, the less probable it is for glitches to appear at all,
and there will be fewer of them (in the same video frame) when they do appear.
`max_glitches`: Maximum number of glitches in the video frame.
`min_glitch_height`, `max_glitch_height`: in pixels. The height is randomized separately for each glitch.
`hold_min`, `hold_max`: in frames (at a reference of 25 FPS). Limits for the random time that the
filter holds one glitch pattern before randomizing the next one.
`name`: Optional name for this filter instance in the chain. Used as cache key.
If you have more than one `analog_vhsglitches` in the chain, they should have
different names so that each one gets its own cache.
"""
# Re-randomize the glitch noise image whenever enough frames have elapsed after last randomization
if self.vhs_glitch_last_image[name] is None or (int(self.frame_no) - int(self.vhs_glitch_last_frame_no[name])) >= self.vhs_glitch_interval[name]:
n_glitches = torch.rand(1, device="cpu")**unboost # unboost: increase probability of having none or few glitching lines
n_glitches = int(max_glitches * n_glitches[0])
if not n_glitches:
vhs_glitch_image = VHS_GLITCH_BLANK # use a nonce value instead of None to distinguish between "uninitialized" and "no glitches during current glitch interval"
vhs_glitch_mask = None
else:
c, h, w = image.shape
vhs_glitch_image = torch.zeros(1, h, w, dtype=image.dtype, device=self.device) # monochrome
vhs_glitch_mask = torch.zeros(1, h, w, dtype=image.dtype, device=self.device) # alpha only
glitch_start_lines = torch.rand(n_glitches, device="cpu")
glitch_start_lines = [int((h - (max_glitch_height - 1)) * x) for x in glitch_start_lines]
for line in glitch_start_lines:
glitch_height = torch.rand(1, device="cpu")
glitch_height = int(min_glitch_height + (max_glitch_height - min_glitch_height) * glitch_height[0])
vhs_glitch_image[0, line:(line + glitch_height), :] = self._vhs_noise(image, height=glitch_height) # [1, h, w]
vhs_glitch_mask[0, line:(line + glitch_height), :] = 1.0 # mark the glitching lines for blending
self.vhs_glitch_last_image[name] = vhs_glitch_image
self.vhs_glitch_last_mask[name] = vhs_glitch_mask
# Randomize time until next change of glitch pattern
self.vhs_glitch_interval[name] = round(hold_min + float(torch.rand(1, device="cpu")[0]) * (hold_max - hold_min))
self.vhs_glitch_last_frame_no[name] = self.frame_no
else:
vhs_glitch_image = self.vhs_glitch_last_image[name]
vhs_glitch_mask = self.vhs_glitch_last_mask[name]
if vhs_glitch_image is not VHS_GLITCH_BLANK:
# Apply glitch to RGB only, so fully transparent parts stay transparent (important to make the effect less distracting).
strength_field = strength * vhs_glitch_mask # "field" as in physics, NOT as in CRT TV
image[:3, :, :] = (1.0 - strength_field) * image[:3, :, :] + strength_field * vhs_glitch_image
def analog_vhstracking(self, image: torch.tensor, *,
base_offset: float = 0.03,
max_dynamic_offset: float = 0.01,
speed: float = 2.5) -> None:
"""[dynamic] 1980s VHS tape with bad tracking.
Image floats up and down, and a band of black and white noise appears at the bottom.
Units like in `analog_badhsync`:
Offsets are given in units where the height of the image is 2.0.
`speed`: At speed 1.0, the floating motion completes a full cycle every
`image_height` frames. So effectively the cycle position updates by
`speed * (1 / image_height)` at each frame.
Note that "frame" here refers to the normalized frame number, at a reference of 25 FPS.
"""
c, h, w = image.shape
# Animation
# FPS correction happens automatically, because `frame_no` is normalized to CALIBRATION_FPS.
cycle_pos = (self.frame_no / h) * speed
cycle_pos = cycle_pos - float(int(cycle_pos)) # fractional part
cycle_pos *= 2.0 # full cycle = 2 units
# Deformation - move image up/down
yoffs = max_dynamic_offset * math.sin(cycle_pos * math.pi)
meshy = self._meshy + yoffs
meshx = self._meshx
grid = torch.stack((meshx, meshy), 2)
grid = grid.unsqueeze(0) # batch of one
image_batch = image.unsqueeze(0) # batch of one -> [1, c, h, w]
warped = torch.nn.functional.grid_sample(image_batch, grid, mode="bilinear", padding_mode="border", align_corners=False)
warped = warped.squeeze(0) # [1, c, h, w] -> [c, h, w]
image[:, :, :] = warped
# Noise from bad VHS tracking at bottom
yoffs_pixels = int((yoffs / 2.0) * h)
base_offset_pixels = int((base_offset / 2.0) * h)
noise_pixels = yoffs_pixels + base_offset_pixels
if noise_pixels > 0:
image[:, -noise_pixels:, :] = self._vhs_noise(image, height=noise_pixels)
# # Fade out toward left/right, since the character does not take up the full width.
# # Works, but fails at reaching the iconic VHS look.
# xx = torch.linspace(0, math.pi, w, dtype=image.dtype, device=self.device)
# fade = torch.sin(xx)**2 # [w]
# fade = fade.unsqueeze(0) # [1, w]
# image[3, -noise_pixels:, :] = fade
def shift_distort(self, image: torch.tensor, *,
strength: float = 0.05,
unboost: float = 4.0,
max_glitches: int = 3,
min_glitch_height: int = 20, max_glitch_height: int = 30,
hold_min: int = 1, hold_max: int = 3,
name: str = "shift_distort0") -> None:
"""[dynamic] Glitchy digital video transport, with transient (per-frame) blocks of lines shifted left or right.
`strength`: Amount of the horizontal shift, in units where 2.0 is the width of the full image.
Positive values shift toward the right.
For shifting both left and right, use two copies of the filter in your chain,
one with `strength > 0` and one with `strength < 0`.
`unboost`: Use this to adjust the probability profile for the appearance of glitches.
The higher `unboost` is, the less probable it is for glitches to appear at all,
and there will be fewer of them (in the same video frame) when they do appear.
`max_glitches`: Maximum number of glitches in the video frame.
`min_glitch_height`, `max_glitch_height`: in pixels. The height is randomized separately for each glitch.
`hold_min`, `hold_max`: in frames (at a reference of 25 FPS). Limits for the random time that the
filter holds one glitch pattern before randomizing the next one.
`name`: Optional name for this filter instance in the chain. Used as cache key.
If you have more than one `shift_distort` in the chain, they should have
different names so that each one gets its own cache.
"""
# Re-randomize the glitch pattern whenever enough frames have elapsed after last randomization
if self.shift_distort_grid[name] is None or (int(self.frame_no) - int(self.shift_distort_last_frame_no[name])) >= self.shift_distort_interval[name]:
n_glitches = torch.rand(1, device="cpu")**unboost # unboost: increase probability of having none or few glitching lines
n_glitches = int(max_glitches * n_glitches[0])
meshy = self._meshy
meshx = self._meshx.clone() # don't modify the original; also, make sure each element has a unique memory address
if n_glitches:
c, h, w = image.shape
glitch_start_lines = torch.rand(n_glitches, device="cpu")
glitch_start_lines = [int((h - (max_glitch_height - 1)) * x) for x in glitch_start_lines]
for line in glitch_start_lines:
glitch_height = torch.rand(1, device="cpu")
glitch_height = int(min_glitch_height + (max_glitch_height - min_glitch_height) * glitch_height[0])
meshx[line:(line + glitch_height), :] -= strength
shift_distort_grid = torch.stack((meshx, meshy), 2)
shift_distort_grid = shift_distort_grid.unsqueeze(0) # batch of one
self.shift_distort_grid[name] = shift_distort_grid
# Randomize time until next change of glitch pattern
self.shift_distort_interval[name] = round(hold_min + float(torch.rand(1, device="cpu")[0]) * (hold_max - hold_min))
self.shift_distort_last_frame_no[name] = self.frame_no
else:
shift_distort_grid = self.shift_distort_grid[name]
image_batch = image.unsqueeze(0) # batch of one -> [1, c, h, w]
warped = torch.nn.functional.grid_sample(image_batch, shift_distort_grid, mode="bilinear", padding_mode="border", align_corners=False)
warped = warped.squeeze(0) # [1, c, h, w] -> [c, h, w]
image[:, :, :] = warped
# --------------------------------------------------------------------------------
# CRT TV output
def _rgb_to_hue(rgb: List[float]) -> float:
"""Convert an RGB color to an HSL hue, for use as `bandpass_hue` in `desaturate`.
This uses a cartesian-to-polar approximation of the HSL representation,
which is fine for hue detection, but should not be taken as an authoritative
H component of an accurate RGB->HSL conversion.
"""
R, G, B = rgb
alpha = 0.5 * (2.0 * R - G - B)
beta = 3.0**0.5 / 2.0 * (G - B)
hue = math.atan2(beta, alpha) / (2.0 * math.pi) # note atan2(0, 0) := 0
return hue
# This filter is adapted from an old GLSL code I made for Panda3D 1.8 back in 2014.
def desaturate(self, image: torch.tensor, *,
strength: float = 1.0,
tint_rgb: List[float] = [1.0, 1.0, 1.0],
bandpass_reference_rgb: List[float] = [1.0, 0.0, 0.0], bandpass_q: float = 0.0) -> None:
"""[static] Desaturation with bells and whistles.
Does not touch the alpha channel.
`strength`: Overall blending strength of the filter (0 is off, 1 is fully applied).
`tint_rgb`: Color to multiplicatively tint the image with. Applied after desaturation.
Some example tint values:
Green monochrome computer monitor: [0.5, 1.0, 0.5]
Amber monochrome computer monitor: [1.0, 0.5, 0.2]
Sepia effect: [0.8039, 0.6588, 0.5098]
No tint (off; default): [1.0, 1.0, 1.0]
`bandpass_reference_rgb`: Reference color for hue to let through the bandpass.
Use this to let e.g. red things bypass the desaturation.
The hue is extracted automatically from the given color.
`bandpass_q`: Hue bandpass band half-width, in (0, 1]. Hues farther away from `bandpass_hue`
than `bandpass_q` will be fully desaturated. The opposite colors on the color
circle are defined as having the largest possible hue difference, 1.0.
The shape of the filter is a quadratic spike centered on the reference hue,
and smoothly decaying to zero at `bandpass_q` away from the center.
The special value 0 (default) switches the hue bandpass code off,
saving some compute.
"""
R = image[0, :, :]
G = image[1, :, :]
B = image[2, :, :]
if bandpass_q > 0.0: # hue bandpass enabled?
# Calculate hue of each pixel, using a cartesian-to-polar approximation of the HSL representation.
# An approximation is fine here, because we only use this for a hue detector.
# This is faster and requires less branching than the exact hexagonal representation.
desat_alpha = 0.5 * (2.0 * R - G - B)
desat_beta = 3.0**0.5 / 2.0 * (G - B)
desat_hue = torch.atan2(desat_beta, desat_alpha) / (2.0 * math.pi) # note atan2(0, 0) := 0
desat_hue = desat_hue + torch.where(torch.lt(desat_hue, 0.0), 0.5, 0.0) # convert from `[-0.5, 0.5)` to `[0, 1)`
# -> [h, w]
# Determine whether to keep this pixel or desaturate (and by how much).
#
# Calculate distance of each pixel from reference hue, accounting for wrap-around.
bandpass_hue = self._rgb_to_hue(bandpass_reference_rgb)
desat_temp1 = torch.abs(desat_hue - bandpass_hue)
desat_temp2 = torch.abs((desat_hue + 1.0) - bandpass_hue)
desat_temp3 = torch.abs(desat_hue - (bandpass_hue + 1.0))
desat_hue_distance = 2.0 * torch.minimum(torch.minimum(desat_temp1, desat_temp2),
desat_temp3) # [0, 0.5] -> [0, 1]
# -> [h, w]
# - Pixels with their hue at least `bandpass_q` away from `bandpass_hue` are fully desaturated.
# - As distance falls below `bandpass_q`, a blend starts very gradually.
# - As the hue difference approaches zero, the pixel is fully passed through.
# - The 1.0 - ... together with the square makes a sharp spike at the reference hue.
desat_diff2 = (1.0 - torch.clamp(desat_hue_distance / bandpass_q, max=1.0))**2
strength_field = strength * (1.0 - desat_diff2) # [h, w]; "field" as in physics, NOT as in CRT TV
else:
strength_field = strength # just a scalar!
# Desaturate, then apply tint
Y = luminance(image[:3, :, :]) # -> [h, w]
Y = Y.unsqueeze(0) # -> [1, h, w]
tint_color = torch.tensor(tint_rgb, device=self.device, dtype=image.dtype).unsqueeze(1).unsqueeze(2) # [c, 1, 1]
tinted_desat_image = Y * tint_color # -> [c, h, w]
# Final blend
image[:3, :, :] = (1.0 - strength_field) * image[:3, :, :] + strength_field * tinted_desat_image
def banding(self, image: torch.tensor, *,
strength: float = 0.4,
density: float = 2.0,
speed: float = 16.0) -> None:
"""[dynamic] Bad analog video signal, with traveling brighter and darker bands.
This simulates a CRT display as it looks when filmed on video without syncing.
`strength`: maximum brightness factor
`density`: how many banding cycles per full image height
`speed`: band movement, in pixels per frame
Note that "frame" here refers to the normalized frame number, at a reference of 25 FPS.
"""
c, h, w = image.shape
yy = torch.linspace(0, math.pi, h, dtype=image.dtype, device=self.device)
# Animation
# FPS correction happens automatically, because `frame_no` is normalized to CALIBRATION_FPS.
cycle_pos = (self.frame_no / h) * speed
cycle_pos = cycle_pos - float(int(cycle_pos)) # fractional part
cycle_pos = 1.0 - cycle_pos # -> motion from top toward bottom
band_effect = torch.sin(density * yy + cycle_pos * math.pi)**2 # [h]
band_effect = torch.unsqueeze(band_effect, 0) # -> [1, h] = [c, h]
band_effect = torch.unsqueeze(band_effect, 2) # -> [1, h, 1] = [c, h, w]
image[:3, :, :].mul_(1.0 + strength * band_effect)
torch.clamp_(image, min=0.0, max=1.0)
def scanlines(self, image: torch.tensor, *,
field: int = 0,
dynamic: bool = True,
channel: str = "Y") -> None:
"""[dynamic] CRT TV like scanlines.
`field`: Which CRT field is dimmed at the first frame. 0 = top, 1 = bottom.
`dynamic`: If `True`, the dimmed field will alternate each frame (top, bottom, top, bottom, ...)
for a more authentic CRT look (like Phosphor deinterlacer in VLC).
`channel`: One of:
"Y": darken the luminance (converts to YUV and back, slower)
"A": darken the alpha channel (fast, but makes the darkened lines translucent)
Note that "frame" here refers to the normalized frame number, at a reference of 25 FPS.
"""
if dynamic:
start = (field + int(self.frame_no)) % 2
else:
start = field
if channel == "A": # alpha
image[3, start::2, :].mul_(0.5)
else: # "Y", luminance
image_yuv = rgb_to_yuv(image[:3, :, :])
image_yuv[0, start::2, :].mul_(0.5)
image_rgb = yuv_to_rgb(image_yuv)
image[:3, :, :] = image_rgb