adjusted function name to late_lateral_sound_level

Author: simon.buechner22

pyrato/parameters.py

@@ -509,14 +509,14 @@ def _energy_ratio(limits, energy_decay_curve1, energy_decay_curve2):
 
     return energy_ratio
 
-def late_lateral_level(energy_decay_curve_ref_10m,
+def late_lateral_sound_level(energy_decay_curve_ref_10m,
                        energy_decay_curve_lateral):
     r"""
-    Calculate the late lateral level.
+    Calculate the late lateral sound level.
 
-    The late lateral level :math:`L_\mathrm{J}` is a measure of the strength
-    of late-arriving lateral sound.
-    According to [#isoLLJ]_, it is defined as the ratio between the
+    The late lateral sound level :math:`L_\mathrm{J}` is a measure of the
+    strength of late-arriving lateral sound.
+    According to [#isoLLJ]_, it is defined as the level ratio between the
     lateral sound energy captured with a figure of eight microphone
     arriving after 80 ms and the total sound energy of a reference
     impulse response measured with an omnidirectional microphone
@@ -571,8 +571,8 @@ def late_lateral_level(energy_decay_curve_ref_10m,
 
     Returns
     -------
-    Late Lateral Level : numpy.ndarray
-        Late lateral level (:math:`L_\mathrm{J}`) in decibels,
+    Late Lateral Sound Level : numpy.ndarray
+        Late lateral sound level (:math:`L_\mathrm{J}`) in decibels,
         shaped according to the channel shape of the input EDCs.
 
     References

tests/test_parameters.py

@@ -9,7 +9,7 @@
 from pyrato.parameters import definition
 from pyrato.parameters import early_lateral_energy_fraction
 from pyrato.parameters import _energy_ratio
-from pyrato.parameters import late_lateral_level
+from pyrato.parameters import late_lateral_sound_level
 
 # parameter clarity tests
 @pytest.mark.parametrize(
@@ -644,7 +644,7 @@ def test_LJ_accepts_timedata_and_returns_correct_shape(
 ):
     """Return type and shape of pyfar.TimeData input for identical edcs."""
     edc = make_edc(energy=energy, sampling_rate=1000)
-    result = late_lateral_level(edc, edc)
+    result = late_lateral_sound_level(edc, edc)
 
     assert isinstance(result, (float, np.ndarray))
     assert result.shape == expected_shape
@@ -655,7 +655,7 @@ def test_LJ_returns_nan_for_zero_denominator_signal():
     edc_ref = pf.TimeData(np.zeros((1, 128)), np.arange(128) / 1000)
     edc_lat = pf.TimeData(np.ones((1, 128)), np.arange(128) / 1000)
 
-    result = late_lateral_level(edc_ref, edc_lat)
+    result = late_lateral_sound_level(edc_ref, edc_lat)
     assert np.isnan(result)
 
 def test_LJ_calculates_known_reference_value(make_edc):
@@ -682,7 +682,7 @@ def test_LJ_calculates_known_reference_value(make_edc):
     edc_lateral = make_edc(energy=edc_lateral,
                            sampling_rate=1000, normalize=False)
 
-    result = late_lateral_level(edc_ref, edc_lateral)
+    result = late_lateral_sound_level(edc_ref, edc_lateral)
 
     expected = 10 * np.log10(0.5)
     np.testing.assert_allclose(result, expected, atol=1e-5)
@@ -706,7 +706,7 @@ def test_LJ_for_exponential_decay_analytical(make_edc):
                        sampling_rate=sampling_rate,
                        total_samples=total_samples)
 
-    result = late_lateral_level(edc_ref, edc_lat)
+    result = late_lateral_sound_level(edc_ref, edc_lat)
 
     a_lat = 13.8155 / 2.2