transfer function,HEv,and the acousto-electric transfer
function,HsE,measured in the IMEHD-aided condition:HsvA
=VA/ps.
3.4.23 acousto-vibrational transfer function(unimplanted),
Hsvu, n—stapes velocity(unimplanted)when driven by the
input sound field,divided by the input sound field pressure:
Hsvu =Vu/ps.
3.4.23.1 Discussion—This quantity can be measured di-
rectly or computed from the product of the middle-ear transfer
function,HTv,and the ear-canal transfer function,Hsr,mea-
sured in the unimplanted condition:Hsvu=vU/Ps=HsrHTv.
3.4.24 ear-canal pressure transfer function,Hsz, n—ear
canal sound pressure,Pr,produced by the input sound field
pressure,ps,in the unimplanted case,divided by that input
sound field pressure:Hsr=Prps;this quantity is unitless(1,
2)³
.
3.4.25 electro-vibrational transferfunction,HEv ,n—stapes
velocity(IMEHD-aided)when driven by the IMEHD output
transducer,divided by the transducer input: HEv=vA/E.
3.4.26 equivalent sound pressure transfer function,HES,
n—unimplanted sound field pressure needed to produce a
stapes velocity equivalent to that produced by an electrical
IMEHD input in the IMEHD-aided condition,divided by the
IMEHD input.
3.4.26.1 Discussion—If the electrical IMEHD input pro-
duces a linear change in stapes velocity with a change in input
electrical stimulus,the equivalent sound pressure transfer
function,HEs,can be computed as the quotient between the
vibro-electric transfer function (IMEHD-aided),HEv,and the
vibro-acoustic transfer function (unimplanted), Hsvu:HEs=
(v/E)/(v/ps)= HEVHsvu.
3.4.27 insertion gain transfer function(sound field),Hss,
n—ratio of the equivalent sound pressure produced in the
IMEHD-aided case with a given electrical input to the IMEHD
output transducer and the input sound field pressure used as
input in the IMEHD-aided case required to produce the same
IMEHD output transducer electrical input:Hss=Pe/ps; this
ratio is unitless.
3.4.27.1 Discussion—With a linear sound signal processor,
the insertion gain(sound field)can be computed from the
product of the equivalent sound pressure transfer function,HES,
and the electro-acoustic transfer function, HsE:Hss=Pe/Ps=
Hse·Hes.Hss willdepend on the particular gain settings used,
for example,full-on gain or minimal gain.The gain should be
reported whenever that transfer function is used.
3.4.28 insertion gain transfer function(velocity),HVv
n—ratio of the stapes velocity (IMEHD-aided)and the stapes
velocity(unimplanted)produced by a given input sound field:
Hvv =VAVu;the ratio is unitless and can be expressed in
decibels as 20-log10(HV).
3.4.28.1 Discussion—With a linear sound signal processor
and IMEHD,that is,a processor whose electrical output E is
proportional to the input sound field pressure,ps,and an
IMEHD whose vibrational output is proportional to its electri-
3The boldface numbers in parentheses refer to the list of references at the end of
this standard.
cal output,the insertion gain(sound field),Hss,willequal the
insertion gain transfer function (velocity),Hv.
3.4.29 maximum insertion gain transfer function(sound
field),Hss,maxn n—maximum insertion gain transfer function
(sound field)that can be achieved with the implant electronics.
3.4.30 middle-ear transferfunction, HT,n—stapes velocity
(unimplanted)produced by an ear-canal sound pressure,di-
vided by the ear-canal sound pressure,in units of mm/s/Pa:
HTv=vUPr ·
3.5 Acronyms:
3.5.1 IHD—implantable hearing device
3.5.2 IMEHD—implantable middle-ear hearing device
3.5.3 LDV—laser Doppler vibrometry
3.5.4 SPL—sound pressure level
4.Summary of Practice
4.1 This practice involves the use of human temporal bones
and laser Doppler interferometry measurements of middle ear
structures velocities,to test for the ex-vivo performances of
IMEHD.Once a procedure for measuring system output has
been defined,several characteristics of the IMEHD can be
specified.Detailed instructions for measuring and reporting
these characteristics are given below.The important character-
istics are:
4.1.1 For Transducers:
4.1.1.1 Equivalent sound pressure transfer function,
4.1.1.2 IMEHD output transducer frequency range,and
4.1.1.3 IMEHD harmonic distortion.
4.1.2 For the System:
4.1.2.1 Maximum insertion gain transfer function(sound
field)(see full-on gain in ANSI S3.22,paragraph 3.7),
4.1.2.2 Maximum equivalent sound pressure level(see
OSPL90 in ANSI S3.22,paragraph 3.5),and
4.1.2.3 IMEHD system frequency range.
5.Significance and Use
5.1 IMEHDs are alternatives to air conduction hearing aids.
They are similar to air conduction hearing aids in that they
process incoming sound by applying frequency shaping and
compression to create an analog,vibratory audio frequency
output.IMEHDs differ from hearing aids in that they do not
create an airborne acoustical output signal with an electroa-
coustical output transducer in the external ear canal,but rather
a mechanical stimulation that results in the vibration of the
cochlear fluid.Therefore,the IMEHD output signal is not
readily accessible after implantation in the way hearing aid
output is accessible with real-ear probe microphone measure-
ments.Different devices will use different methods of coupling
to the ossicular chain or cochlea.This makes it difficult to
design a uniform model of the middle ear in the way the 2-cm³
coupler is used as a model of the external ear canal with
conventional hearing aids.
5.2 This practice provides uniformity of data collection
practices,thus allowing IMEHD in vitro performances to be
evaluated and readily compared.Once clinical data are