845 lines
45 KiB
Modula-2
845 lines
45 KiB
Modula-2
# This is a makehrtf HRIR definition file. It is used to define the layout
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# and source data to be processed into an OpenAL Soft compatible HRTF.
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#
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# This definition is used to transform the left ear HRIRs from the full set
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# of KEMAR HRIRs provided by Bill Gardner <billg@media.mit.edu> and Keith
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# Martin <kdm@media.mit.edu> of MIT Media Laboratory.
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#
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# The data (full.zip) is available from:
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#
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# http://sound.media.mit.edu/resources/KEMAR.html
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#
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# It is copyrighted 1994 by MIT Media Laboratory, and provided free of charge
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# with no restrictions on use so long as the authors (above) are cited.
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#
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# This definition is used to generate the default HRTF table used by OpenAL
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# Soft.
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# The following are the data set metrics. They must always be specified at
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# the start of a definition file, but their order is not important.
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# Sampling rate of the HRIR data (in hertz).
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rate = 44100
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# The channel type of incoming HRIR data (mono or stereo). Mono channel
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# inputs will result in mirroring to provide the right ear HRIRs. If not
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# specified, this defaults to mono.
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type = mono
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# The number of points to use from the HRIR data. This should be a
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# sufficiently large value (to encompass the entire impulse response). It
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# cannot be smaller than the truncation size (default is 32) specified on the
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# command line.
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points = 512
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# The radius of the listener's head (measured ear-to-ear in meters). The
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# makehrtf utility uses this value to rescale measured propagation delays
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# when a custom head radius is specified on the command line. It is also
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# used as the default radius when the spherical model is used to calculate an
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# approximate set of delays. This should match the data set as close as
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# possible for accurate rescaling when using the measured delays (the
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# default). At the moment, radius rescaling does not adjust HRIR coupling.
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radius = 0.09
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# A list of the distances between the source and the listener (in meters) for
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# each field. These must start at or above the head radius and proceed in
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# ascending order. Since the MIT set is single-field, there is only one
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# distance.
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distance = 1.4
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# A list of the number of azimuths measured for each elevation per field.
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# Elevations are separated by commas (,) while fields are separated by
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# semicolons (;). There must be at least 5 elevations covering 180 degrees
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# degrees of elevation for the data set to be viable. The poles (first and
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# last elevation) must be singular (an azimuth count of 1).
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azimuths = 1, 12, 24, 36, 45, 56, 60, 72, 72, 72, 72, 72, 60, 56, 45, 36, 24, 12, 1
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# Following the metrics is the list of source HRIRs for each field,
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# elevation, and azimuth triplet. They don't have to be specified in order,
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# but the final composition must not be sparse. They can however begin above
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# a number of elevations (as typical for HRIR measurements).
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#
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# The field index is used to determine the distance coordinate (for mult-
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# field HRTFs) while the elevation and azimuth indices are used to determine
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# the resulting polar coordinates following OpenAL Soft's convention (-90
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# degree elevation increasing counter-clockwise from the bottom; 0 degree
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# azimuth increasing clockwise from the front).
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#
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# More than one HRIR can be used per source. This allows the composition of
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# averaged magnitude responses or the specification of stereo HRTFs. Target
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# ears must (and can only be) specified for each source when the type metric
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# is set to 'stereo'.
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#
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# Source specification is of the form (~BNF):
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#
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# source = ( sf_index | mf_index ) source_ref [ '+' source_ref ]*
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#
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# sf_index = '[' ev_index ',' az_index ']' '='
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# mf_index = '[' fd_index ',' ev_index ',' az_index ']' '='
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# source_ref = mono_ref | stereo_ref
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#
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# fd_index = unsigned_integer
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# ev_index = unsigned_integer
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# az_index = unsigned_integer
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# mono_ref = ref_spec ':' filename
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# stereo_ref = ref_spec ':' filename ear
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#
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# ref_spec = ( wave_fmt '(' wave_parms ')' [ '@' start_sample ] ) |
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# ( bin_fmt '(' bini_parms ')' [ '@' start_byte ] ) |
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# ( bin_fmt '(' binf_parms ')' [ '@' start_byte ] ) |
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# ( ascii_fmt '(' asci_parms ')' [ '@' start_element ] ) |
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# ( ascii_fmt '(' ascf_parms ')' [ '@' start_element ] )
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# filename = double_quoted_string
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# ear = 'left' | 'right'
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#
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# wave_fmt = 'wave'
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# wave_parms = channel
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# bin_fmt = 'bin_le' | 'bin_be'
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# bini_parms = 'int' ',' byte_size [ ',' bin_sig_bits ] [ ';' skip_bytes ]
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# binf_parms = 'fp' ',' byte_size [ ';' skip_bytes ]
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# ascii_fmt = 'ascii'
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# asci_parms = 'int' ',' sig_bits [ ';' skip_elements ]
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# ascf_parms = 'fp' [ ';' skip_elements ]
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# start_sample = unsigned_integer
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# start_byte = unsigned_integer
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# start_element = unsigned_integer
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#
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# channel = unsigned_integer
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# byte_size = unsigned_integer
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# bin_sig_bits = signed_integer
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# skip_bytes = unsigned_integer
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# sig_bits = unsigned_integer
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# skip_elements = unsigned_integer
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#
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# For bin_sig_bits, positive values mean the significant bits start at the
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# MSB (padding toward the LSB) while negative values mean they start at the
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# LSB.
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# Even though the MIT set is provided as stereo .wav files, each channel is
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# for a different sized KEMAR ear. Since it is not a stereo data set, no ear
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# is specified. The smaller KEMAR ear (in the left channel: 0) is used.
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[ 5, 0 ] = wave (0) : "./MITfull/elev-40/L-40e000a.wav"
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[ 5, 1 ] = wave (0) : "./MITfull/elev-40/L-40e006a.wav"
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[ 5, 2 ] = wave (0) : "./MITfull/elev-40/L-40e013a.wav"
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[ 5, 3 ] = wave (0) : "./MITfull/elev-40/L-40e019a.wav"
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[ 5, 4 ] = wave (0) : "./MITfull/elev-40/L-40e026a.wav"
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