[0001] The invention relates to an electrodynamic transducer comprising a magnet system
having a first pole and a second pole forming an air gap, and a diaphragm arranged
in the air gap, on which diaphragm a conductor is arranged. Such a transducer is known
from the published Netherlands Patent Application 79,03,908 which has been laid open
to public inspection. The transducer disclosed in said Application is a transducer
of the ribbon type, whose voice coil is constituted by the conductor on the diaphragm.
A drawback of the known transducer is that its life is limited because the conductor
on the diaphragm will break in the course of time.
[0002] It is the object of the invention to provide a transducer in which the conductor
on the diaphragm is less susceptible to breakage, enabling the life of the transducer
to be extended.
[0003] To this end the electrodynamic transducer in accordance with the invention is characterized
in that the conductor is made of a copper-silver alloy, the silver content being between
0.01% and 0.5% by weight.
[0004] The inventive step is based on the recognition of the following fact. The conductor
in the known transducer is obtained by applying a photo-etching process to an alumination-plastics
laminate. In order to obtain a maximum sensitivity the aluminium material used for
the conductor is of a maximum purity. The maximum permissible electric power for the
known transducer is first of all determined by the maximum permissible temperature.
For example, if the diaphragm is made of the material polyimide temperatures up to
approximately 400°C are permissible.
[0005] However, for the aluminium conductor this temperature gives rise to problems. It
is known that the recrystallisation temperature of pure aluminium lies between 150°C
and 200°C. In this range the tensile strength of aluminium is substantially zero.
[0006] When the electrical load applied to the voice coil is high the temperature rises
considerably. The aluminium track pattern of the conductor then expands in the longitudinal
direction, causing the diaphragm to become wrinkled in the stationary condition. In
the event of a fluctuating (high) electrical load the voice coil, and hence the diaphragm,
is continually wrinkled and smoothed. This results in a higher distortion in the acoustic
output signal of the transducer. Moreover, in the long run this gives rise to fatigue
effects, finally causing breakage in the conductor tracks.
[0007] Apparently, the maximum permissible power for a specific life expectancy is substantially
lower than can be anticipated only on the basis of the thermal properties of the polyimide
material.
[0008] It is true that by the addition of other metals to aluminium the recrystallisation
temperature can be raised substantially, but this results in an excessive reduction
of the conductivity, which is at the expense of the sensitivity.
[0009] In accordance with the invention it is proposed to use a different material for the
conductor, so that a substantially higher permissible electrical load can be achieved
and a longer life can be obtained, whilst the distortion in the output signal of the
transducer can be reduced significantly.
[0010] Pure copper has a recrystallisation temperature which lies at approximately 150°C.
By the addition of small amounts of silver, however, the recrystallisation temperature
increases. An addition of the order of from 0.01% by weight of silver, yields a significant
rise in recrystallisation temperature, which already lies above the recrystallisation
temperature of aluminium. As long as the addition does not exceed 0.5%, adding silver
to the copper hardly effects the conductivity. Therefore the value of 0.5% should
be regarded as an upper limit, because a higher value results in a (no longer acceptable)
reduction in conductivity.
[0011] Now a conductor material is obtained which is far better capable of withstanding
the high temperatures occurring during use of an electrodynamic transducer without
its correct operation being adversely affected. Preferably, the silver content is
selected to be between 0.025% and 0.25% by weight. In this range a recrystallisation
temperature is obtained which already lies above 260°C, whilst for example in the
case of 0.1% by weight of silver this temperature already lies at approximately 330°C,
the specific resistance still being low (substantially equal to that of pure copper).
[0012] An additional advantage of a substantially higher recrystallisation temperature is
that the coefficient of linear expansion of the material and, similarly, the temperature
coefficient of the electrical resistance is smaller. This means that (substantially)
no wrinkling of the diaphragm will arise. Moreover, a possible loss of sensitivity
as a result of the higher specific mass of the silver-copper alloy relative to that
of aluminium will be compensated for by a reduced compression. (In this respect "compression"
is to be understood to mean: doubling the input voltage causes the output power to
rise by less than 6 dB.)
[0013] The behaviour of copper alloys, in particular alloys of copper and silver, is described
in "Kupfer und Kupferlegierungen in der Technik" by Kurt Dies, Springer Verlag 1967,
see in particular Chapter 5.1.
[0014] An embodiment of the invention will now be described in more detail, by way of example,
with reference to the sole Figure. The Figure shows an embodiment of the electrodynamic
transducer in accordance with the invention.
[0015] Figure 1 is a sectional view of an electrodynamic transducer in accordance with the
invention. The construction of the magnet systems corresponds to the construction
of the magnet system of the transducer known from Netherlands Patent Application 81,02,572
(PHN 10,062) which has been laid open to public inspection. The transducer may be
of circular or rectangular shape. In the latter case the Figure is a sectional view
of the transducer taken perpendicularly to the longitudinal direction of the conductors
in an air gap. The magnet system of the transducer comprises a first pole in the form
of a pole plate 2, 3 comprising two plate-shaped parts 2ʹ, 2ʺ and 3ʹ, 3ʺ, a second
pole in the form of a centre pole 1, a closing plate 4, and the parts 5 and 6. The
magnetic field in the magnet system can be obtained by constructing the parts 5 and
6 as permanent magnets. The direction of magnetisation is indicated by the arrows
20 and 21. However, the direction of magnetisation may also be reversed. The other
parts of the magnet system are made of a soft-magnetic material, for example soft-iron.
[0016] If the transducer is of the circular type 5, 6 represents a sectional view of an
annular magnet. In the rectangular version 5 and 6 are cross-sections of two bar magnets
which extend parallel to one another. It is also possible to make the parts 5 and
6 of a soft-magnetic material and to construct the centre pole, at least its hatched
portion 1ʹ, as a permanent magnet.
[0017] In the circular version an air gap 8 is formed between the pole plate 2, 3 and the
centre pole 1. The air gap 8 and the pole plate 2, 3 are then annular. In the rectangular
version air gaps 8 are formed between the pole plate 2 and the centre pole 1 and between
the pole plate 3 and the centre pole 1, which air gaps, like the pole plates 2 and
3, extend parallel to one another. In the air gap (gaps) 8 a diaphragm 7 is arranged,
on which at least one conductor 9 is arranged, which extends over the diaphragm surface
in a direction perpendicular to the plane of drawing. The Figure shows either three
conductors which extend over the diaphragm surface parallel to each other in an air
gap, or one conductor which extends over the diaphragm surface in three spiral turns
around the centre pole. The conductors are connected to an audio amplifier (not shown)
in such a way that the signal currents in the conductor(s) 9 between the pole plate
2 and the centre pole 1 are directed perpendicularly to the plane of drawing and the
signal currents in the conductor(s) 9 between the pole plate 3 and the centre pole
1 flow in exactly opposite direction. Since the magnetic field in the air gap 8 between
the upper plate 2 and the centre pole 1 extends in or parallel to the plane of the
diaphragm and is directed oppositely to the magnetic field in the air gap 8 between
the pole plate 3 and the centre pole 1, the diaphragm has an excursion which is substantially
in phase over the entire surface area. Therefore, this transducer is referred to as
an isophase transducer, or more specifically: a ribbon loudspeaker.
[0018] The pole plate (plates) 2, 3 (each) comprise two plate-shaped parts 2ʹ, 3ʹ and 2ʺ,
3ʺ. The two plate-shaped parts 2ʹ, 3ʹ and 2ʺ, 3ʺ adjoin each other over a part of
their facing major surfaces, which major surfaces extend substantially in and parallel
to the diaphragm plane. Another portion of said major surface of one or both plate-shaped
parts (one of the parts in the Figure) recede(s) slightly, as is indicated by the
reference numeral 10, so that a space 11 is obtained. The diaphragm 7 is now arranged
between the plate-shaped parts 2ʹ, 3ʹ and 2ʺ, 3ʺ in such a way that a peripheral portion
of the diaphragm situated in said space(s) 11. The diaphragm 7 may be clamped for
example on or in a frame 12 which is secured between the two plate-shaped parts. However,
alternatively the diaphragm may be clamped between the parts 2ʹ, 2ʺ and 3ʹ, 3ʺ. The
width
x of the frame 12 is smaller than the width
y of the space 11. Moreover, the height
z of the space 11 is such that the movable portion of the periphery of the diaphragm
7, which is situated in the space 11, can move freely and cannot contact the pole
plate (plates) 2, 3.
[0019] Instead of making at least one of the major surfaces recede, the space 11 between
the plate-shaped parts can also be realised by interposing, for example, a plate of
a soft-magnetic material between the two facing major surfaces. The thickness of
plate of soft-magnetic material must then correspond to the height
z of the space 11.
[0020] Further, a damping material (not shown) may be arranged in the spaces 11 underneath
and/or above the diaphragm, which material comes in mechanical contact with the diaphragm.
This damping material damps the higher natural resonances in the diaphragm (
i.e. free vibrations of the diaphragm in a resonant pattern corresponding to the resonant
frequency of the diaphragm in response to the drive of the diaphragm), which yields
an improvement of the transducer output signal, which then exhibits less distortion.
[0021] Preferably, the centre pole 1 also extends to the other side of the diaphragm. The
part 1ʺ at this side of the diaphragm is indicated by a dashed line. The part of the
diaphragm which is situated between the two parts 1 and 1ʺ of the centre pole is freely
movable. The part 1ʺ is retained in the indicated position by a support, not shown.
For an improved impedance matching of the medium into which the transducer radiates
its acoustic signals the end faces of the parts 1ʺ, 2ʹ and 3ʹ which face the air gap
8 are rounded. This means that in a direction perpendicular to the plane of the diaphragm
these end faces diverge increasingly as the distance from the diaphragm increases,
so that a horn-like radiation aperture is obtained.
[0022] The conductor(s) 9 is (are) made of a copper-silver alloy, the silver content being
between 0.01% and 0.5% by weight. Preferably, the silver content is between 0.025%
and 0.25% by weight. In particular a silver content of approximately 0.1% by weight
yields very satisfactory results as regards the thermal and mechanical loadability
of the transducer.
[0023] In this respect it is to be noted that the inventive step is not limited to the embodiment
shown. The invention also applies to those embodiments which differ from the embodiment
shown in respects which are irrelevant to the invention. For example, the invention
may also be applied to a transducer described in the Applicant's Netherlands Patent
Application 85,01,166 (PHN 11,359), which has been laid open to public inspection.