1 # This is a makehrtf HRIR definition file. It is used to define the layout
2 # and source data to be processed into an OpenAL Soft compatible HRTF.
4 # This definition is used to transform the left ear HRIRs from the full set
5 # of KEMAR HRIRs provided by Bill Gardner
<billg@media.mit.edu
> and Keith
6 # Martin
<kdm@media.mit.edu
> of MIT Media Laboratory.
8 # The
data (full.zip
) is available from
:
10 # http
://sound.media.mit.edu
/resources
/KEMAR.html
12 # It is copyrighted
1994 by MIT Media Laboratory
, and provided free of charge
13 # with no restrictions on use so long as the
authors (above
) are cited.
15 # This definition is used to generate the default HRTF table used by OpenAL
18 # The following are the data set metrics. They must always be specified at
19 # the start of a definition file
, but their order is not important.
21 # Sampling rate of the HRIR
data (in hertz
).
24 # The channel type of incoming HRIR
data (mono or stereo
). Mono channel
25 # inputs will result in mirroring to provide the right ear HRIRs. If not
26 # specified
, this defaults to mono.
29 # The number of points to use from the HRIR data. This should be a
30 # sufficiently large
value (to encompass the entire impulse response
). It
31 # cannot be smaller than the truncation
size (default is
32) specified on the
35 # The radius of the listener
's head (measured ear-to-ear in meters). The
36 # makehrtf utility uses this value to rescale measured propagation delays
37 # when a custom head radius is specified on the command line. It is also
38 # used as the default radius when the spherical model is used to calculate an
39 # approximate set of delays. This should match the data set as close as
40 # possible for accurate rescaling when using the measured delays (the
41 # default). At the moment, radius rescaling does not adjust HRIR coupling.
44 # A list of the distances between the source and the listener (in meters) for
45 # each field. These must start at or above the head radius and proceed in
46 # ascending order. Since the MIT set is single-field, there is only one
50 # A list of the number of azimuths measured for each elevation per field.
51 # Elevations are separated by commas (,) while fields are separated by
52 # semicolons (;). There must be at least 5 elevations covering 180 degrees
53 # degrees of elevation for the data set to be viable. The poles (first and
54 # last elevation) must be singular (an azimuth count of 1).
55 azimuths = 1, 12, 24, 36, 45, 56, 60, 72, 72, 72, 72, 72, 60, 56, 45, 36, 24, 12, 1
57 # Following the metrics is the list of source HRIRs for each field,
58 # elevation, and azimuth triplet. They don't have to be specified in order
,
59 # but the final composition must not be sparse. They can however begin above
60 # a number of
elevations (as typical for HRIR measurements
).
62 # The field index is used to determine the distance
coordinate (for mult
-
63 # field HRTFs
) while the elevation and azimuth indices are used to determine
64 # the resulting polar coordinates following OpenAL Soft
's convention (-90
65 # degree elevation increasing counter-clockwise from the bottom; 0 degree
66 # azimuth increasing clockwise from the front).
68 # More than one HRIR can be used per source. This allows the composition of
69 # averaged magnitude responses or the specification of stereo HRTFs. Target
70 # ears must (and can only be) specified for each source when the type metric
73 # Source specification is of the form (~BNF):
75 # source = ( sf_index | mf_index ) source_ref [ '+' source_ref ]*
77 # sf_index = '[' ev_index ',' az_index ']' '='
78 # mf_index = '[' fd_index ',' ev_index ',' az_index ']' '='
79 # source_ref = mono_ref | stereo_ref
81 # fd_index = unsigned_integer
82 # ev_index = unsigned_integer
83 # az_index = unsigned_integer
84 # mono_ref = ref_spec ':' filename
85 # stereo_ref = ref_spec ':' filename ear
87 # ref_spec = ( wave_fmt '(' wave_parms ')' [ '@
' start_sample ] ) |
88 # ( bin_fmt '(' bini_parms ')' [ '@
' start_byte ] ) |
89 # ( bin_fmt '(' binf_parms ')' [ '@
' start_byte ] ) |
90 # ( ascii_fmt '(' asci_parms ')' [ '@
' start_element ] ) |
91 # ( ascii_fmt '(' ascf_parms ')' [ '@
' start_element ] )
92 # filename = double_quoted_string
93 # ear = 'left
' | 'right
'
96 # wave_parms = channel
97 # bin_fmt = 'bin_le
' | 'bin_be
'
98 # bini_parms = 'int
' ',' byte_size [ ',' bin_sig_bits ] [ ';' skip_bytes ]
99 # binf_parms = 'fp
' ',' byte_size [ ';' skip_bytes ]
100 # ascii_fmt = 'ascii
'
101 # asci_parms = 'int
' ',' sig_bits [ ';' skip_elements ]
102 # ascf_parms = 'fp
' [ ';' skip_elements ]
103 # start_sample = unsigned_integer
104 # start_byte = unsigned_integer
105 # start_element = unsigned_integer
107 # channel = unsigned_integer
108 # byte_size = unsigned_integer
109 # bin_sig_bits = signed_integer
110 # skip_bytes = unsigned_integer
111 # sig_bits = unsigned_integer
112 # skip_elements = unsigned_integer
114 # For bin_sig_bits, positive values mean the significant bits start at the
115 # MSB (padding toward the LSB) while negative values mean they start at the
118 # Even though the MIT set is provided as stereo .wav files, each channel is
119 # for a different sized KEMAR ear. Since it is not a stereo data set, no ear
120 # is specified. The smaller KEMAR ear (in the left channel: 0) is used.
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