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The Journal of Neuroscience, September 1, 2000, 20(17):6684-6693
Centrifugal Pathways Protect Hearing Sensitivity at the
Cochlea in Noisy Environments That Exacerbate the Damage
Induced by Loud Sound
Ramesh
Rajan
Department of Physiology, Monash University, Monash, Victoria 3800, Australia
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ABSTRACT |
Loud sounds damage the cochlea, the auditory receptor organ,
reducing hearing sensitivity. Previous studies demonstrate that the
centrifugal olivocochlear pathways can moderately reduce these temporary threshold shifts (TTSs), protecting the cochlea. This effect involves only the olivocochlear pathway component known as the
crossed medial olivocochlear system pathway, originating from
the contralateral brainstem and terminating on outer hair cells in the
cochlea. Here I demonstrate that even moderate noise backgrounds can
significantly exacerbate the cochlear TTSs induced by loud tones, but
this is prevented because in such conditions there is additional
activation of uncrossed olivocochlear pathways, enhancing protection of
cochlear hearing sensitivity. Activation of the uncrossed pathways
differs from that of the crossed pathway in that it is achieved only in
noise backgrounds but can then be obtained under monaural conditions of
loud tone and background noise. In contrast, activation of the crossed
pathway is achieved only by binaural loud tones and is not further
enhanced by background noise. Thus, conjoint activation of both crossed
and uncrossed efferent pathways can occur in noise backgrounds to
powerfully protect the cochlea under conditions similar to those
encountered naturally by humans.
Key words:
cochlea; olivocochlear efferents; loud sounds; hearing
damage; noise backgrounds; protection; TTS
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INTRODUCTION |
An early manifestation of the
damaging effects of loud sounds is a temporary hearing desensitization
[temporary threshold shifts (TTSs)] that occurs without any
morphological damage to cochlear structures or only variable damage
(Robertson and Johnstone, 1980 ; Robertson et al., 1980 ; Robertson,
1982 ; Tilney et al., 1982 ; Liberman and Dodds, 1987 ; Gao et al., 1992 ;
Harding et al., 1992 ; Dew et al., 1993 ; Borg et al., 1995 ). It is
generally accepted (Cody and Russell, 1986 ; Liberman et al., 1986 ;
Patuzzi et al., 1989 ; Cooper and Rhode, 1992 ; Patuzzi, 1992 ; Ruggero et
al., 1993 ) that TTSs is primarily attributable to effects on the outer
hair cells (OHCs) of the cochlea, whose local actions in
transduction are critical for normal hearing sensitivity and frequency
selectivity (Harrison and Evans, 1977 ; Dallos and Harris, 1978 ;
Liberman and Kiang, 1978 ; Robertson and Johnstone, 1979 ; Schmeidt et
al., 1980 ; Cody and Russell, 1986 ; Liberman et al., 1986 ; Patuzzi and
Robertson, 1988 ; Cody, 1992 ).
The mammalian cochlea receives a dual-component efferent innervation
(Guinan et al., 1983 ; Warr et al., 1986 ). The lateral olivocochlear
system (LOCS), almost exclusively from only the ipsilateral lateral
superior olivary nucleus, terminates on dendrites of afferent neurons.
The medial olivocochlear system (MOCS), from ipsilateral [uncrossed
MOCS (UMOCS)] and contralateral [crossed MOCS (CMOCS)]
periolivary nuclei, terminates on OHCs. Physiological activation of the
MOCS by binaural stimulation can reduce TTSs induced by loud tones
(Cody and Johnstone, 1982 ; Rajan and Johnstone, 1988 ; Rajan, 1992 ,
1995a ,b , 1996 ). Only the CMOCS pathway is involved, and lesioning only
this pathway prevents the effect (Rajan and Johnstone, 1988 ; Rajan,
1995b ).
The efferent effect on TTSs to damaging tones shows features consistent
with a protective system: protection is graded to TTSs (Rajan and
Johnstone, 1988 ; Rajan, 1992 , 1995b ), occurs to any loud tone, but is
evoked most easily by tones most readily damaging the cochlea (Rajan,
1995b ), and occurs to each of successive loud tones (Rajan, 1996 ). This
has lead to suggestions (Rajan, 1992 ; Brown et al., 1998 ) that cochlear
centrifugal pathways have an important functional role at high sound
levels and to interest in determining if they were involved in other
forms of protection from loud sound (Kujawa and Liberman, 1997 ; Zheng
et al., 1997a ), including from permanent damage (Handrock and Zeisberg,
1982 ; Liberman and Gao, 1995 ; Zheng et al., 1997b ). However, because classical electrically elicited efferent effects are strongest on
cochlear responses at low sound levels and decline by high levels
(Galambos, 1956 ; Weiderhold, 1986 ), the functional value of this
protection is yet to be widely accepted and it is sometimes described
as an epiphenomenon (Borg et al., 1995 ) to a primary, yet unknown,
role. Here I demonstrate that in background noise, there is conjoint
activation of crossed and uncrossed efferent pathways to powerfully
protect (by almost 30 dB) from loud sound whose effects would otherwise
be exacerbated by the noise. This compelling evidence for a functional
role for efferent protection from loud tone-induced damage has direct
relevance to human susceptibility to loud sounds in noisy workplace or
recreational environments.
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MATERIALS AND METHODS |
Animal treatment and measurement of hearing
sensitivity. Procedures involved in animal treatment and measuring
cochlear hearing sensitivity have been detailed elsewhere (Rajan et
al., 1991 ; Rajan, 1995a ). In brief, adult cats weighing between 3 and 6 kg were tested under procedures approved by the Monash University Standing Committee on Ethics in Animal Experimentation and conforming to guidelines of the National Health and Medical Research Council of
Australia. Cats were anesthetized (60 mg/kg) and maintained with
continuous intravenous infusion of Nembutal at 2-3
mg · kg 1 · hr 1.
Depth of anesthesia was monitored through continuous recording of
rectal temperature, ECG, and EMG activity from forearm muscles and by
regular hourly checks of the response to strong noxious pinching of the
forepaw and of the presence of pupillary dilatation and absence of
corneal reflexes. The output from the ECG/EMG electrodes was displayed
on an oscilloscope and fed into a speaker for continuous monitoring of
the cat's condition and depth of anesthesia. Body temperature was
maintained at 37.5 ± 0.5°C by a thermostatically controlled
warming blanket, regulated by feedback from a rectal probe. Cats were
tracheostomized and artificially ventilated on room air. Tidal volume
was determined from normogram cat respiratory data. Respiratory rate
was set between 20 and 25 breaths/min depending on the cat's size.
Surgery (Rajan et al., 1991 ) was performed to implant stainless steel
electrodes against the round window membrane of both cochleas to
measure cochlear hearing sensitivity bilaterally. Hearing sensitivity
was assessed by measuring thresholds for the compound action potential
(CAP) of the auditory nerve at frequencies from 1 to 40 kHz (Rajan et
al., 1991 ; Rajan, 1995a ). Thresholds were compared to normative data
(Rajan et al., 1991 ; Rajan, 1995a ), and only animals with normal
hearing sensitivity bilaterally from 1 to 40 kHz were used.
Tones and noise stimuli to each ear were generated independently by one
of four channels of a digital synthesis system, gated under computer
control and passed through separate computer-controlled attenuators,
before feeding into one of four channels of an electronic mixer box.
The mixer was used to manually switch delivery of stimuli to each ear
as desired. Crosstalk between different channels of the mixer box was
more than 100 dB up to 10 kHz, 100 dB from 10-20 kHz, and declined
thereafter to 95 dB at 40 kHz. Two output channels from the mixer box
separately fed sound to one of two Sennheiser HD 535 speakers, each in
specially designed housing leading out to a sound delivery tube placed
in one external auditory meatus (Rajan et al., 1991 ).
Surgical inactivation of efferent pathways. Inactivation of
various components of the cochlear efferent pathways was made using
surgical lesions at the floor of the fourth ventricle, after removing
the overlying cerebellum (Rajan, 1995a ). Because of the coursing of the
efferent fibers, it is possible from this brainstem location to lesion
all efferent pathways to one or both cochleas, or crossed pathways to
both cochleas (Warren and Liberman, 1989 ), but not the crossed pathway
to only one cochlea or only the uncrossed pathways to a cochlea. Thus,
lesions were made to either totally de-efferent only one cochlea
(Rajan, 1995a ,b ), lesion only the crossed efferent pathways bilaterally
(Rajan, 1995a ,b ), or combine these manipulations to cut crossed
pathways to both cochleas and all efferent pathways to one cochlea,
leaving only uncrossed pathways intact to only one cochlea.
To totally de-efferent only one cochlea, a lesion was made 1.5-2 mm
lateral of the midline and on the brainstem side ipsilateral to the
cochlea to be de-efferented. To cut only crossed pathways (bilaterally), the lesion was made exactly at the midline. To cut
crossed pathways to both cochleas and all efferent pathways to one
cochlea, two lesions were placed as a combination of the previous two
lesion types. The first lesion was at the midline to cut crossed
pathways bilaterally and a second lesion placed 1.5-2 mm lateral of
the midline to cut all efferent pathways to only one cochlea. Lesions
were always 6- to 8-mm-long, extending around the location of the
facial colliculi that were identifiable on the floor of the fourth
ventricle. Postmortem histological analysis, occasionally combined with
histochemical staining for acetylcholine esterase (which stains the
efferent pathways), was used to confirm the location of the cuts
(Warren and Liberman, 1989 ; Rajan, 1995a ).
In all animals with lesions placed in the brainstem, the CAP audiogram
was measured before and after placing any lesions. The heart rate, ECG
waveform, and body temperature were also noted before the lesion and
rechecked immediately after the lesion.
Traumatic loud sound exposures and measurement of cochlear
desensitization. The traumatic loud tone used to cause TTSs
was at 13 kHz and was presented at 100 dB sound pressure level (SPL) continuously for 15 min. This frequency was chosen as it is from within
the most sensitive part of the cat's CAP audiogram (Rajan et al.,
1991 ) and, of particular relevance to this study, frequencies from this
region cause hearing damage more easily than do other frequencies
(Rajan, 1995b ), as well as more readily activate the previously
described (Rajan, 1995b ) protective effects of the crossed efferent pathways.
With monaural testing the loud tone was delivered to only the test ear;
the output to the non-test ear was blocked off by turning off the mixer
box switch to that ear and by turning off, through computer control,
that output channel from the stimulus synthesis system. With binaural
testing the loud tone was delivered simultaneously and concurrently to
both ears. In testing the effects of noise backgrounds, continuous
noise (0.5-40 kHz) was switched on 3 sec before the loud tone and
remained on for the duration of the tone. Tone and noise were switched
off simultaneously by computer control after 15 min of loud tone (and
noise) exposure.
Cats were assigned to groups exposed to the loud tone in a background
of silence or of noise. Groups exposed to the tone in a background of
silence were: Silence 1 (n = 6 cats) and Silence 2 (n = 6), exposed monaurally and binaurally,
respectively, without any lesions to cochlear efferent pathways;
Silence 3 (n = 5), exposed binaurally after a lesion to
cut all cochlear efferent pathways unilaterally; and Silence 4, exposed
binaurally after lesions of only crossed pathways bilaterally
(n = 2). Noise groups were exposed to the loud tone in
a background of noise. In Noise 1 (n = 4), the noise
level was 40 dB SPL, in Noise 2 (n = 7) at 60 dB SPL,
and in Noise 3 (n = 6), Noise 4 (n = 5), Noise 5 (n = 6), Noise 6 (n = 6),
and Noise 7 (n = 5) at 80 dB SPL. Groups Noise 1-5
were exposed to the tone and noise binaurally, Noise 1-3 after
unilateral total de-efferentation, Noise 4 after a lesion of only
crossed pathways (bilaterally), and Noise 5 after lesions to cut
crossed pathways bilaterally as well as all efferent pathways (i.e.,
the remaining uncrossed pathways) to only one side. Groups Noise 6 and
7 were exposed monaurally to the tone in noise, in Noise 6 with no
lesions to cochlear efferent pathways and in Noise 7 after the same two
types of lesions as in Noise 5. In Noise 7 the crossed de-efferented
ears were tested first and later, after data collection from these
ears, the totally de-efferented ears were tested, also monaurally. The
experimental conditions in each group are summarized in Table
1.
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Table 1.
Test groups and experimental conditions of laterality of
loud tone exposure (loud tone always at 13 kHz, 100 dB SPL for 10 min)
and background to exposure
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A further group (group "Noise-alone") was tested with monaural
noise by itself at 80 dB SPL either with no lesions to efferent pathways (n = 2) or after unilateral de-efferentation
(n = 8). To ensure that any noise effects would not be
missed, thresholds were measured from 15 sec after the noise-alone
exposure, much earlier than the post-test measurement time in all other
groups exposed to the loud tone, as detailed below.
In all groups with loud tone exposure, CAP thresholds were measured 5 min after the end of the loud tone at frequencies from 7 to 30 kHz, in
a constant (but not linear) order. It took ~2.5 min to measure
thresholds from 9 to 28 kHz bilaterally. Frequency-specific TTSs were
calculated as the difference between the pre-loud tone and post-loud
tone thresholds. Comparisons between groups or treatments were
comparisons between TTSs at corresponding frequencies. Two-way repeated
measures ANOVAs were used to compare effects between different
experimental conditions. If the ANOVA revealed a significant difference
between conditions, generally with a significant interaction term
between experimental condition and frequency, unpaired Student's t tests were used to compare threshold losses at
corresponding frequencies in the two conditions.
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RESULTS |
Basic protective effects of the crossed olivocochlear pathway on
TTSs induced by loud tones in a background of silence
For the standard loud tone here (at 13 kHz, 100 dB SPL for 15 min), I first confirmed previous demonstrations (Cody and Johnstone, 1982 ; Rajan and Johnstone, 1988 ; Rajan, 1995a ,b ) using other loud tones
(at different frequencies, and for different durations) that in a
background of silence, binaural, but not monaural, loud sound could
activate the crossed efferent pathway to reduce loud tone-induced TTSs.
These results will be compared to the effects of the loud sound in
noise backgrounds.
In a background of silence, the standard loud tone applied monaurally
(group Silence 1; Fig. 1a)
produced TTSs >25 dB at frequencies from 13 to 20 kHz. Damage
decreased outside this range, more rapidly at lower than higher
frequencies. Maximum threshold shift of ~50 dB occurred at 15 kHz.
Binaural exposure to the same tone (group Silence 2; Fig.
1a) resulted in significantly smaller TTSs from 11 to 28 kHz
(Table 2A). Reductions
in TTSs (i.e., protection; Fig. 1b, Protection 1) were
generally graded to TTSs occurring with monaural exposure (i.e., to the
corresponding-frequency data in group Silence 1), and the largest mean
reduction of ~15 dB was at 15 kHz. These effects of binaural versus
monaural exposure are identical to those reported previously for other
loud sounds applied in silence (Cody and Johnstone, 1982 ; Rajan and
Johnstone, 1988 ; Rajan, 1995a ,b ).

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Figure 1.
In a background of silence the crossed efferent
pathway is activated by binaural, but not monaural, stimulation to
protect the cochlea from loud sound-induced TTSs. a, c,
Loud sound-induced TTSs of frequency-specific thresholds for the
auditory nerve CAP. Data are mean data (error bars indicate SE)
from groups or treatment conditions exposed to a loud tone in a
background of silence. In a, binaural tonal exposure in
group Silence 2 (open circles and dotted
line) produced lower TTSs than did monaural exposure in group
Silence 1 (closed circles and full line);
and in Silence 3, binaural tonal exposure after unilateral lesion of
all efferent pathways produced TTSs in de-efferented ears in Silence 3 (closed squares and long dashed line)
similar to those in Silence 1, and TTSs in efferent-intact ears in
Silence 3 (open squares and short dashed
line) similar to those in Silence 2. In c, group
Silence 4 (closed inverted triangles and long
dashed line) was exposed binaurally after bilateral lesions of
only the crossed efferent pathways; this resulted in TTSs in these
crossed de-efferented ears similar to those in the totally
de-efferented ears in Silence 3 (closed squares and
short dashed line) and larger than in efferent-intact
ears in Silence 3 (open squares and short dashed
line). b, Protection of the cochlea in treatment
conditions from a: Protection 1 was the difference in
mean TTSs in Silence 1 and those in Silence 2; Protection 2 was the
difference in mean frequency-specific TTSs in totally de-efferented
ears and in efferent-intact ears of group Silence 3.
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Table 2.
In a background of silence the crossed efferent pathway is
activated by binaural, but not monaural, stimulation to protect the
cochlea from loud sound-induced TTSs
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Surgical inactivation of cochlear efferent pathways confirmed they were
responsible for protection in the binaural condition. In group Silence
3, after totally de-efferenting only one cochlea the loud tone was
applied binaurally; from 10 to 28 kHz TTSs in de-efferented ears (Fig.
1a) were significantly larger than in efferent-intact ears
(Table 2B). Threshold shifts in the latter ears were
always similar to corresponding-frequency TTSs from efferent-intact
binaurally exposed group Silence 2 (Table 2B), whereas TTSs in de-efferented Silence 3 ears were similar to those in
the monaurally exposed efferent-intact group Silence 1 (Table 2B). Thus, in silence, binaural loud sound activates
cochlear efferents to protect, and monaural loud sound does not. Given this, the protection in Silence 3 (difference between TTSs in de-efferented and efferent-intact ears; Fig. 1b,
Protection 2) was identical to the protection seen when
comparing the binaurally exposed efferent-intact group Silence 2 against the monaurally exposed efferent-intact group Silence 1 (Fig.
1b, Protection 1). In both comparisons, maximum
protection was at 15 kHz and was 15 dB reduction from a peak threshold
shift of ~50 dB.
This protection involved only the crossed efferent pathway, as shown by
lesioning only this pathway (bilaterally) in Silence 4 before binaural
application of the loud tone. The identical treatment in the two ears
in each animal resulted in bilaterally similar TTSs; data from
corresponding frequencies from all ears were therefore pooled.
Threshold shifts in these crossed de-efferented ears were similar (Fig.
1c) to those in totally de-efferented ears of the binaurally
exposed Silence 3 (Table 2C) but were significantly larger
from 11 to 24 kHz (Table 2C) than in efferent-intact ears in
Silence 3. So, although uncrossed efferent pathways were intact in
Silence 4, they did not reduce TTSs, confirming that cochlear
protection gained with binaural loud tones in silence is attributable
to only the crossed pathway.
There is enhanced protection of hearing sensitivity by cochlear
efferent pathways in non-damaging noise backgrounds that can exacerbate
loud sound-induced TTSs
The effects of a noise background to the loud tone on TTSs were
first tested in groups in which one cochlea was totally de-efferented. The lesion was followed by binaural exposure to the loud tone in a
noise background. Results are compared to results in group Silence 3, in which the same lesion type was followed by binaural tone exposure in
a background of silence.
Depending on intensity, noise backgrounds exacerbated TTSs in
de-efferented ears (Fig. 2a).
The exacerbation was most pronounced at frequencies >15 kHz, which was
the frequency most affected by the tone in a background of silence.
With noise at 40 dB SPL (group Noise 1) there was no exacerbation of
TTSs: frequency-specific TTSs in de-efferented ears were similar to
those in de-efferented ears of Silence 3 (Table
3A). With noise at 60 dB SPL
(Noise 2) or 80 dB SPL (Noise 3) de-efferented ears suffered
significantly larger tone-induced TTSs at 12, 13, and from 16 to 28 kHz
than de-efferented ears of Silence 3 (Table 3A). Comparing
the noise groups, increasing noise intensity from 40 to 60 dB SPL
caused significantly greater TTSs mainly from 16 to 28 kHz (Table
3A), and increasing intensity from 60 to 80 dB SPL further
significantly exacerbated TTSs mainly from 22 to 28 kHz (Table
3A).

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Figure 2.
Both crossed and uncrossed efferent pathways
protect the cochlea from loud sound-induced TTSs in nondamaging noise
backgrounds that exacerbate TTS. a, b, TTSs after
binaural loud tone exposure in a background of binaural noise or
silence in different groups, after total de-efferentation of only one
ear. Data are mean data (error bars indicate SE) from either
efferent-cut (OC ; closed symbols) ears
(a) or efferent-intact (OC+; open
symbols) ears (b) in each group. In
a and b the different symbols are for
groups Silence 3 (squares and long dashed
line), Noise 1 (noise = 40 dB SPL, upright
triangle and dotted line), Noise 2 (noise = 60 dB SPL, inverted triangle and long dashed
line), and Noise 3 (noise = 80 dB SPL,
diamond and full line). Comparison of
a and b shows that noise levels of >40
dB SPL progressively exacerbated TTSs in de-efferented ears but not in
efferent-intact ears. Additionally, in a data from the
"Noise alone" group, which was exposed only to noise at 80 dB SPL
(cross symbols, full line), show that noise by itself
did not cause TTS. c, Protection of the cochlea in noise
backgrounds compared to that in silence; protection in each
tone-exposed group from a and b was
calculated as the difference in mean frequency-specific TTSs in the
efferent-cut ears (a, OC ears) and those in the
efferent-intact ears (b, OC+ ears) of the same group.
Squares, Silence 3; upright triangle, Noise 1;
inverted triangle, Noise 2; diamond, Noise
3.
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Table 3.
Both crossed and uncrossed efferent pathways protect the
cochlea from loud sound-induced TTSs in nondamaging noise backgrounds
that can exacerbate the sound-induced TTS
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In contrast to de-efferented ears, in efferent-intact ears (Fig.
2b) background noise did not increase TTSs above those
occurring in efferent-intact ears to the loud tone in a background of
silence. Threshold shifts in each group with a noise background (Noise 1, 2, and 3) were similar (Table 3B) to TTSs in
efferent-intact ears in group Silence 3 exposed to the binaural
tone in a background of silence, as well as similar between the three
noise groups (p always > 0.05, generally > 0.3).
Noise by itself at 80 dB SPL did not cause any TTSs in de-efferented or
efferent-intact ears. Data from these conditions were pooled and are
illustrated in Figure 2a. Noise only induced small and
nonsystematic threshold changes, either of increased sensitivity or
desensitization, within the 2-3 dB variability for threshold measurements with the technique used here (Rajan et al., 1991 ; Rajan,
1995a ).
Because higher-level noise backgrounds progressively exacerbated loud
tone-induced TTSs only in de-efferented ears, the difference between
TTSs in de-efferented and efferent-intact ears (i.e., the protection in
efferent-intact ears) increased with increasing noise level,
particularly at >15 kHz. The protection in noise backgrounds is
illustrated in Figure 2c and compared to that in group
Silence 3, in which unilateral de-efferentation was followed by
binaural tone exposure in a background of silence. In the latter case protection followed the pattern of TTS. Mean protection >10 dB occurred from 13 to 18 kHz, with peak protection of 15 dB at 15 kHz, the frequency suffering the largest threshold shift. At higher or
lower frequencies TTSs in de-efferented ears and protection in
efferent-intact ears both decreased. Noise at 40 dB SPL had no
exacerbating effect on TTSs in de-efferented ears, and protection in
efferent-intact ears was similar to that in group Silence 3 exposed to
the loud tone in a background of silence. With noise at 60 dB SPL there
was a significant increase in TTSs at high frequencies in de-efferented
ears and a large increase in protection at these frequencies in
efferent-intact ears. Mean protection of >10 dB now occurred from 12 to 28 kHz, with peak protection of 23 dB at 19 kHz. With noise at 80 dB
SPL there was further exacerbation of TTSs in de-efferented ears,
particularly at high frequencies, and more protection in
efferent-intact ears. Mean protection of >10 dB extended from 11 to 28 kHz with peak protection of almost 30 dB from 20 to 22 kHz.
The enhanced cochlear protection to binaural tones in binaural
noise backgrounds is attributable to activation of the uncrossed
efferent pathways additional to the crossed pathways
In confirmation of previous studies (Cody and Johnstone, 1982 ;
Rajan and Johnstone, 1988 ; Rajan, 1995a ,b ), it was shown earlier that
in a background of silence only the crossed efferent pathway mediates
protection obtained with exposure to binaural loud sound. To determine
if the enhanced protection in the higher-level noise backgrounds was
also attributable to only this pathway, in group Noise 4 only this
pathway was cut bilaterally (as in Silence 4). The loud tone and noise
at 80 dB SPL were delivered binaurally. The identical treatment of the
two ears in each animal resulted in bilaterally similar TTS, and data
from corresponding frequencies in all animals were pooled. These data
were compared (Fig. 3a) to
data from efferent-intact ears and totally de-efferented ears in Noise
3 in which the binaural loud tone was also presented in binaural noise
at 80 dB SPL. The comparison showed that crossed and uncrossed efferent
pathways were involved in the enhanced protection in noise, in a
frequency-dependent manner. Despite the absence of the crossed pathway
in Noise 4, TTSs at all frequencies (9-28 kHz) were still lower than
in totally de-efferented ears of Noise 3 (Table 3C). Thus,
in Noise 4 the intact uncrossed efferent pathways still significantly
protected the cochlea over the entire affected frequency range.
However, from 12 to 18 kHz, the crossed pathway provides significant
protection in noise: in Noise 4, in which only this pathway was absent,
these frequencies suffered significantly larger TTSs (Table
3C) than did Noise 3 efferent-intact ears which possessed
crossed and uncrossed pathways.

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Figure 3.
Protection by the uncrossed efferent pathways from
loud tone-induced TTSs in a noise background can be elicited by
monaural stimulation. a, c, TTSs in various groups after
loud tone exposure either binaurally or monaurally, in a background of
noise at 80 dB SPL or of silence. Data are group mean data (error bars
indicate SE) from efferent-intact ears, totally de-efferented ears, or
crossed de-efferented ears. a, Both crossed and
uncrossed pathways are responsible for the cochlear protection seen
with binaural tone exposure in binaural noise. In efferent-intact ears,
binaural tone exposure in a noise background (Noise 3 efferent-intact
ears, open squares and full line)
produced low TTS. In totally de-efferented ears, the binaural tone
exposure in noise (Noise 3 totally de-efferented ears, closed
circles and full line; and Noise 5 totally
de-efferented ears, closed squares and long
dashed line) produced large TTS. In crossed de-efferented ears,
the binaural tone exposure in noise (Noise 4 crossed de-efferented
ears, open circles and dotted line; Noise
5 crossed de-efferented ears, open inverted triangles
and short dashed line) produced an intermediate amount
of TTSs at most frequencies. b, Protection of the
cochlea in noise backgrounds by uncrossed efferent pathways (UOC
alone) compared to that by action of both crossed and uncrossed
efferent pathways (Total OC). For the former, Estimate 1 was obtained from group Noise 5 from the difference between mean
frequency-specific TTSs in the totally de-efferented ears and in the
crossed de-efferented ears; Estimate 2 was the difference between mean
data from the totally de-efferented ears in Noise 3 and the crossed
de-efferented ears from Noise 4. The average (Average, full
line) of these two estimates is also illustrated. Total OC
protection is that previously illustrated in Figure 2c
for Noise 3 as the difference in mean frequency-specific TTSs in
totally de-efferented ears and efferent-intact ears of the same group.
c, Protection by uncrossed pathways can be elicited by
monaural exposure to the loud tone in a monaural noise background (at
80 dB SPL). In totally de-efferented ears, monaural tone exposure in
monaural noise (Noise 7 totally de-efferented ears, closed
inverted triangles and long dashed line)
produced large TTSs similar to that seen previously with binaural tone
exposure in binaural noise (Noise 3 totally de-efferented ears,
closed circles and full line). In
efferent-intact ears, a noise background to a monaural tone exposure
(Noise 6 efferent-intact ears, open circles and
full line) did not exacerbate TTSs above that to a
monaural tone exposure alone (Silence 1, open upright triangles,
dotted line). Furthermore, in crossed de-efferented ears a
noise background to a monaural tone exposure (Noise 7 crossed
de-efferented ears, inverted triangles and long
dashed line) also did not exacerbate TTSs above that to a
monaural tone exposure alone (i.e., Silence 1), indicating that the
intact uncrossed pathways in Noise 7 are able to protect from noise
exacerbation of TTS.
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The involvement of uncrossed pathways in the enhanced protection in
noise was confirmed directly by a within-group test in group Noise 5. In this group crossed pathways were lesioned bilaterally, and then all
efferent pathways (i.e., the remaining uncrossed pathways) to only one
cochlea were lesioned. Then the cats were exposed binaurally to the
loud tone in the background of noise at 80 dB SPL. The ears that were
only crossed de-efferented ears always suffered significantly lower
TTSs (Fig. 3a, Table 3C) than the totally
de-efferented ears; thus, in the crossed de-efferented ears, intact
uncrossed pathways still protected the cochlea. (As shown in Fig.
3a, TTSs in totally de-efferented ears in Noise 5 were
similar to those in totally de-efferented ears in Noise 3, and TTSs in
crossed de-efferented Noise 5 ears were similar to those in crossed
de-efferented Noise 4 ears. This is also demonstrated below in
calculations of the protection provided by uncrossed efferent
pathways.)
Two estimates were obtained of the protection provided by uncrossed
efferent pathways in a background of noise at 80 dB SPL. A within-group
estimate (Fig. 3b, UOC protection Estimate 1) was obtained from group Noise 5 from the difference between mean
frequency-specific TTSs in totally de-efferented and crossed
de-efferented ears. An across-group estimate (Fig. 3b,
UOC protection Estimate 2) was obtained from the difference
between mean data from totally de-efferented ears in Noise 3 and
crossed de-efferented ears in Noise 4. Protection by uncrossed pathways
was biased toward higher frequencies (Fig. 3b): protection
of >10 dB was found consistently only at frequencies >14 kHz with
peak protection of ~24-25 dB occurring from 20 to 22 kHz and
declining to ~17 dB at 28 kHz. Figure 3b (Total
OC) also compares this protection to that provided in noise when
all efferent pathways were intact, calculated previously (Fig.
2c) from the difference between totally de-efferented and efferent-intact ears in group Noise 3. The pattern of protection in the
latter case is dominated by the pattern caused by uncrossed pathways
alone: protection of >10 dB was consistently found from 11 kHz to all
higher frequencies. Peak protection of almost 30 dB was at 20-22 kHz,
with a small decline to ~22 dB at 28 kHz. This large protection in
group Noise 3 was attributable to the involvement of both crossed and
uncrossed efferent pathways (in efferent-intact ears in Noise 3) in the
noise background.
Protection by the uncrossed efferent pathways from loud
sound-induced TTSs in a noise background can be elicited by monaural
stimulation
As noted above, in a background of silence binaural loud tones are
required to activate protection, which is then mediated only by the
crossed efferent pathway. I determined whether the (larger) efferent
protection obtained in a background of noise, through involvement of
both crossed and uncrossed pathways, also required binaural
stimulation. In two groups tests were done with only monaural loud
sound in monaural ipsilateral noise at 80 dB SPL. In group Noise 6, all
efferent pathways were intact, and TTSs (Fig. 3c) was not
significantly different (Table
4A) from TTSs in group
Silence 1 in which the monaural loud tone was presented in a background
of silence. In contrast, as also illustrated in Figure 3c,
after total de-efferentation (in Noise 3; totally de-efferented ears)
TTSs to the monaural tone in the monaural noise background was greater
than TTSs in group Silence 1 to the monaural loud tone in a background
of silence. (Although loud tone and noise were applied binaurally in
Noise 3, the total de-efferentation of ears for which data are
considered here effectively renders those ears monaural.) Comparison of
Noise 6 data against those from totally de-efferented ears of Noise 3 showed that TTSs from 12 to 28 kHz in Noise 6 were significantly lower
than in Noise 3 totally de-efferented ears (Table
4A). This confirmed that in the monaural condition of
Noise 6, intact efferent pathways prevented noise from exacerbating
tone-induced TTS.
View this table:
[in this window]
[in a new window]
|
Table 4.
Protection by the uncrossed efferent pathways from loud
sound-induced threshold shifts in a noise background can be elicited by
monaural stimulation
|
|
To determine which efferent component was responsible for this
monaurally elicited protection, in group noise 7 two lesions were
placed, as in Noise 5; one to cut the crossed pathways bilaterally, and
the second to cut all efferent pathways (i.e., the remaining uncrossed
pathways) to only one cochlea. The monaural loud tone and noise were
first applied in the crossed de-efferented ears and later in the
totally de-efferented ears.
Threshold shifts in the crossed de-efferented Noise 7 ears were similar
to those in the efferent-intact ears of Noise 6 (Fig. 3c,
Table 3B). However, in the totally de-efferented ears in Noise 7, TTSs at 10-28 kHz were significantly higher than in
efferent-intact ears of Noise 6 (Fig. 3c, Table
4B) and also significantly higher than in crossed
de-efferented Noise 7 ears (Fig. 3c, Table
4B). Thus, under monaural conditions, uncrossed
efferent pathways can act alone to prevent noise exacerbating
tone-induced damage. However, at some frequencies, this protection is
not as great as that obtained in the (binaural) condition in which
crossed and uncrossed efferent pathways are active in protection.
Crossed de-efferented monaurally exposed Noise 7 ears (intact uncrossed
pathways) suffered significantly greater TTSs from 11 to 16 kHz than
did the efferent-intact binaurally exposed ears in group Noise 3 (Table
4C). It has been shown earlier that in the conditions in
these Noise 3 ears (all efferents intact, and tested binaurally), both
crossed and uncrossed pathways are active in protection. The extra
protection in these ears compared to the crossed de-efferented Noise 7 ears was attributable to the action of the crossed pathways in the
Noise 3 ears.
These analyses convincingly demonstrate that the protection in the
binaural tone and noise condition was caused by both crossed and
uncrossed efferent pathways. A further analysis refuted the alternative
hypothesis that stronger activity in uncrossed efferents was
responsible for the larger protection in the binaural condition compared to the monaural condition. Comparison of TTSs in crossed de-efferented monaurally exposed Noise 7 ears against those in crossed
de-efferented binaurally exposed group Noise 4 found no significant
differences (Table 4C) confirming that uncrossed efferent
pathways (intact in both groups) are as effectively activated by the
monaural test condition as by the binaural test condition.
In contrast, the results from the monaurally tested groups reconfirmed
that binaural conditions are required for the crossed efferent pathway
to be activated, even in a noise background. In this background the
monaural loud tone produced similar TTSs whether the crossed pathway
was intact (Noise 6) or lesioned (Noise 7), as long as uncrossed
pathways were intact. Thus, in a background of noise (as in a
background of silence, as shown earlier) the crossed efferent pathway
is not activated by a monaural loud tone. In accord with this
conclusion, the monaural loud tone produced similar TTSs whether
applied in a background of noise (Noise 6) or in a background of
silence (Silence 1).
 |
DISCUSSION |
This report establishes three important results. First, in the
absence of functional cochlear efferent pathways even a moderate noise
background, itself not causing any damage, significantly exacerbates
damaging effects of a loud tone, particularly at higher frequencies of
the tone-affected range. Second, in noise backgrounds there is
activation of efferent pathways additional to those activated by a
binaural loud tone in a background of silence, and this enhances cochlear protection compared to that in silence. Additional efferent pathways activated in noise are uncrossed efferent pathways not activated by the loud tone alone. Finally, in noise, uncrossed efferents are "automatically" activated by loud tones, even under monaural conditions of loud tone and noise, and prevent noise from
exacerbating tone-induced damage. The protective effects of uncrossed
pathways are only revealed when they are inactivated.
The observation that uncrossed efferent pathways have cochlear effects
in a noise background is consistent with the demonstration (Brown et
al., 1998 ) that single uncrossed efferent neurons are driven more
effectively by noise than tones, and the observation (Kawase and
Liberman, 1993 ; Kawase et al., 1993 ) of other (anti-masking) cochlear
effects of uncrossed pathways in noise. In the latter case, when
responses to tones in one ear are masked by noise in that ear, addition
of noise to the other ear activates uncrossed pathways to the test ear
to reduce some of the masking. The laterality of noise application to
reveal uncrossed efferent anti-masking effects and the protection of
the present study differ in that protection is observed when noise and
tone are presented to the same ear alone. This may only reflect the
difference that in studies of anti-masking effects, tone levels likely
to damage hearing were not used. This difference may also account for
the finding, in single-unit studies, that uncrossed efferent neurons
are driven by the ear other than the one to which they project
(Liberman and Brown, 1986 ) and facilitated by noise in the projection
ear (Liberman, 1988 ; Brown et al., 1998 ), whereas the present study shows that uncrossed efferents to a cochlea protect when noise and
loud tone are in their projection ear alone (i.e., monaural loud tone and noise) and binaural tone in noise did not produce any
more uncrossed efferent protection. (The extra protection in the
binaural condition was attributable to activation of the crossed
efferent pathway by binaural tones, not to any greater activation of
uncrossed pathways.) In the single-unit studies, too, sounds likely to
cause damage to hearing sensitivity were not used.
White noise did not cause TTSs; rather, in de-efferented ears it
exacerbated damage caused by the loud tone, particularly at high
frequencies in the affected range. Three features suggest that
uncrossed efferents prevent this exacerbation rather than acting
primarily on the mechanism whereby loud sound damages hearing sensitivity, whereas crossed efferents act specifically on the latter mechanism.
First, TTSs after a monaural loud tone in a noise background were
identical to TTSs after the monaural tone in a background of silence.
In the first condition only uncrossed efferents acted (to prevent noise
from exacerbating loud tone-induced TTSs), whereas in the second, TTSs
were not modulated by any efferent influence. Thus, when only uncrossed
pathways protected, they prevented noise from exacerbating TTSs beyond
levels caused by the loud tone. In contrast, when only the crossed
pathway protected (with application of binaural loud tone in a
background of silence), TTSs were reduced below the TTSs levels caused
by the tone alone (monaural loud tone in a background of silence).
Second, TTSs with application of binaural loud tone in background of
noise were not lower than the protected levels seen with application of
binaural loud tone in silence. In the first condition both crossed and
uncrossed efferent pathways protected, whereas in the second only the
crossed pathway protected. Thus, the additional activation of the
uncrossed pathways in the first condition did not reduce TTSs below
levels to which it had been reduced by the crossed pathway. Finally, uncrossed efferent protection (in background of noise) was greatest at
higher frequencies at which noise most exacerbated (in de-efferented ears) TTSs. In all tests peak TTSs was focused at 15 kHz (although in
noise backgrounds this peak broadened to include higher frequencies). However, protection at 15 kHz was generally similar whether the binaural tone was applied in a background of silence, when only the
crossed pathway protected, or in a noise background, when crossed and
uncrossed efferents protected. This was not caused by saturation of
uncrossed efferent protection: in contrast to protection at 15 kHz,
much greater protection was obtained in a noise background at the
higher frequencies at which noise exacerbated TTSs. (Note that even
then TTSs at the higher frequencies did not significantly exceed that
at 15 kHz). In contrast, crossed efferent protection was maximal at the
frequency most affected by the tone alone, as also found previously
(Rajan and Johnstone, 1988 ; Rajan, 1992 , 1995a ,b , 1996 ) using a larger
range of loud tone levels and frequencies, in a background of silence.
These effects suggest strongly that in the overall TTSs caused when a
tone occurs in a noisy background, the crossed pathway acts on the
mechanism whereby loud tones cause TTSs, whereas the uncrossed pathway
acts on the mechanism whereby noise, in de-efferented ears, allows loud
tones to cause more TTSs. Although the mechanism underlying TTSs is
unknown, a current view (Patuzzi et al., 1989 ; Patuzzi, 1992 ) suggests
it is caused by temporary inactivation of mechanosensitive transduction
ion channels in OHCs. It has been suggested (Patuzzi and Rajan, 1990 )
that such inactivation occurs only for movement of the cochlear
partition in one direction during sound-induced vibration of the
partition. Noise may exacerbate loud tone-induced TTSs by biasing the
cochlear partition further or for longer in this direction.
The two efferent pathways also differed in how they were activated to
produce protection. Previous studies with loud tones, in a background
of silence, have shown that the protective crossed efferent pathway is
activated only by binaural stimulation. [Note that the input does not
have to be binaurally equally intense (Cody and Johnstone, 1982 ; Rajan
and Johnstone, 1988 ), a condition that translates credibly to the
free-field in which loud sounds away from the midline will be unequally
loud bilaterally (Rajan, 1995b ).] This study extends that feature to
noise backgrounds by showing that in a noise background, a monaural
loud tone evoked protection only through uncrossed pathways. These
various data suggest that protective crossed efferent neurons are
activated frequency-specifically only by binaural tonal input. This is
consistent with the report, when testing with binaural loud sounds in a
background of silence, that protection requires binaural tones to be at
the same frequency (Cody and Johnstone, 1982 ). In contrast, uncrossed pathways only protect from TTSs caused by tones in the presence of
noise, but such activation occurs with monaural input from both tone
and noise, resulting in expression of uncrossed efferent protection as
fully as with binaural testing. These data suggest that crossed
efferent neurons involved in protection do not require convergence of
inputs from different frequency channels but require binaural input for
expression of cochlear protection. In contrast, uncrossed efferent
neurons involved in protection appear to require convergence of inputs
from many frequency channels, but this convergence occurs for monaural
input from the ear to which they project (and, ultimately, protect).
The crossed (contralateral) efferent pathway consists almost
exclusively of MOCS neurons terminating on OHCs (Guinan et al., 1983 ;
Warr et al., 1986 ); protective effects of the crossed pathway must
therefore be exercised only at this cochlear site. The uncrossed (ipsilateral) pathway consists of LOCS neurons terminating on dendrites
of cochlear afferent neurons, and MOCS neurons terminating on OHCs
(Guinan et al., 1983 ; Warr et al., 1986 ). Potentially either
subcomponent could be responsible for uncrossed pathway protection. It
is generally held (Weiderhold, 1986 ; Guinan, 1988 ) that all efferent
effects at the cochlea to date, and responses of single efferents, are
attributable solely to MOCS neurons terminating on OHCs. It therefore
seems most parsimonious to assume that uncrossed efferent protection is
attributable only to (ipsilateral) MOCS neurons (i.e., the UMOCS); also
it is difficult to see how actions at dendrites of cochlear afferent
neurons could prevent noise from exacerbating loud tone-induced damage.
Finally, the present results have a clear and important relevance to
human susceptibility to loud sound-induced damage to cochlear hearing
sensitivity. Exposure to loud sounds very often would occur in
environments with an ambient level of noise (such as workplace or
recreational environments). The present study shows that uncrossed
cochlear efferents are already "primed" to be activated in such
environments to prevent noise from exacerbating damage caused by any
loud sounds. Dysfunction of efferents, particularly uncrossed
efferents, could potentiate damage to hearing sensitivity and may be
responsible for some effects seen in cases of occupational hearing
damage, an increasing epidemiological problem. Designing conditions to
optimize the action of efferent pathways in noisy environments that
carry a risk of exposure to loud sound could significantly ameliorate
cochlear damage caused by loud sound in such environments.
 |
FOOTNOTES |
Received April 18, 2000; revised May 31, 2000; accepted June 13, 2000.
This work was supported by Grant 970505 from the National Health and
Medical Research Council of Australia.
Correspondence should be addressed to Dr. Rajan at the above address.
E-mail: ramesh.rajan{at}med.monash.edu.au.
 |
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