U.S. patent number 3,846,792 [Application Number 05/196,032] was granted by the patent office on 1974-11-05 for electric sound-producing device.
Invention is credited to Richard Wolliscroft Haigh.
United States Patent |
3,846,792 |
Haigh |
November 5, 1974 |
ELECTRIC SOUND-PRODUCING DEVICE
Abstract
An electric sound producing device includes a ferromagnetic
diaphragm, an electromagnet for deforming the diaphragm and an
oscillator for repeatedly supplying short duration current pulses
to the electromagnets. The oscillator may be driven by a
multivibrator to produce intermittent sound pulses or by a
saw-tooth pulse generator to produce sound with an apparently
cyclically varying frequency.
Inventors: |
Haigh; Richard Wolliscroft
(Shelsley Beauchamp, EN) |
Family
ID: |
26247442 |
Appl.
No.: |
05/196,032 |
Filed: |
November 5, 1971 |
Foreign Application Priority Data
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Nov 7, 1970 [GB] |
|
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53087/70 |
Apr 20, 1971 [GB] |
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10310/71 |
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Current U.S.
Class: |
340/384.73;
340/388.1 |
Current CPC
Class: |
G08B
3/10 (20130101); B06B 1/0284 (20130101); G10K
9/13 (20130101); B06B 2201/53 (20130101) |
Current International
Class: |
G10K
9/00 (20060101); G08B 3/00 (20060101); B06B
1/02 (20060101); G08B 3/10 (20060101); G10K
9/12 (20060101); G08b 003/10 () |
Field of
Search: |
;340/384E,388 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Pitts; Harold I.
Attorney, Agent or Firm: Holman & Stern
Claims
I claim:
1. An electrical sound-producing device comprising a resilient
diaphragm of ferromagnetic material having a substantially flat
portion, an electromagnet including a tubular core having one end
adjacent said flat portion of the diaphragm and spaced therefrom by
an air gap, the other end thereof being mounted on a spigot,
whereby said diaphragm is deformed when current is supplied to said
electromagnet, and an oscillator for repeatedly supplying current
in short duration pulses to said electromagnet.
2. A device as claimed in claim 1 in which the oscillator produces
pulses of duration approximately equal to half the period of the
natural vibration of the diaphragm.
3. An electrical sound producing device comprising a resilient
diaphragm of ferromagnetic material, an electromagnet whereby said
diaphragm is deformed when current is supplied to said
electromagnet, said electromagnet including a core having one end
adjacent said diaphragm, a coil comprising a pair of windings on
said core and an oscillator of which said core and windings form an
essential part for repeatedly supplying current to the windings in
short duration pulses.
4. A device as claimed in claim 3 in which said oscillator
comprises first and second terminals, an n-p-n transistor with its
collector connected via one winding of said coil to the first
terminal and its emitter connected to the second terminal, a first
resistor and a diode in series circuit bridging said first winding,
a capacitor connected in a circuit with the second winding of the
coil connecting the second terminal to the base of the transistor
and a charging circuit for said capacitor including a second
resistor.
5. A device as claimed in claim 4 in which said charging circuit
consists of said second resistor connected between the end of the
second winding which is connected to the capacitor and the first
terminal.
6. A device as claimed in claim 4 in which said charging circuit
comprises a further resistor connecting the second resistor to the
first terminal, a further transistor with its collector/emitter
path connecting the interconnection of the second and further
resistors to said second terminal and means for applying a signal
to the base of said further transistor.
7. A device as claimed in claim 6 in which said further resistor
and said further transistor form part of a multivibrator whereby
the charging circuit is energized intermittently so that the device
produces sound intermittently.
8. A device as claimed in claim 6 in which said further resistor
and said further transistor form part of a sawtooth pulse generator
circuit whereby the pulse repetition frequency of the oscillator is
varied cyclically.
9. A device as claimed in claim 4 further comprising a further
diode with its anode connected to the first terminal to prevent
reverse voltages being applied to the first mentioned
transistor.
10. A device as claimed in claim 4 in which the anode of the diode
is connected to the collector of the transistor and its cathode is
connected to the first resistor, and further comprising a further
capacitor connecting the cathode of said diode to the emitter of
the transistor.
11. A device as claimed in claim 4 further comprising a further
capacitor interconnecting the first and second terminals.
12. A device as claimed in claim 4 further comprising a third
resistor connecting said capacitor to the second winding.
13. An electrical sound producing device comprising a body formed
in two parts, a flexible resilient diaphragm of ferromagnetic
material supported by one body part, an electromagnet supported by
the other body part whereby the diaphragm is deformed when current
is supplied to the electromagnet, means for adjusting the position
of said two parts relative to one another during assembly of the
device to vary the air gap between the electromagnet and the
diaphragm, sealing means joining the body parts together in an
adjusted relationship and an oscillator contained within said body
for repeatedly supplying current to the electromagnet in short
duration pulses.
14. A device as claimed in claim 13 in which said parts have mating
cylindrical surfaces and are rotatable relative to one another
about the common axis of said surfaces during assembly, said parts
having interengaging means for displacing the two parts axially
relative to one another on turning of one part relative to the
other.
15. A device as claimed in claim 14, in which said interengaging
means comprises a plurality of abutments on one part and a
plurality of inclined ramps on the other part.
16. A device as claimed in claim 13, in which the part of the body
which supports the diaphragm has an internal groove into which an
external rib on a member of which the diaphragm is an integral part
is a snap fit.
17. A device as claimed in claim 13, in which the part of the body
which carries the electromagnet has an integral spigot on which
there is fitted a tubular core forming part of said
electromagnet.
18. A device as claimed in claim 17, in which a coil of the
electromagnet is mounted on the core.
19. A device as claimed in claim 18, in which there is provided an
annular insulation member surrounding the coils and supporting the
component parts of the oscillator.
20. A device as claimed in claim 17, in which the electromagnet
further comprises a cup-shaped member, having a hole fitted on said
spigot and engaged by the core, forming a magnetic connection
between the core and the periphery of the diaphragm, an air gap
being defined between the core and the center of the diaphragm.
21. An electrical sound-producing device comprising a body, a
flexible resilient diaphragm mounted in said body, a tubular
acoustic resonator on the body tuned to the natural frequency of
the diaphragm and whose axis is perpendicular to the plane of the
diaphragm, an electromagnet in the body for deforming the diaphragm
when current is supplied thereto and an oscillator contained in the
body for repeatedly supplying current to the electromagnet in short
duration pulses of lengths approximately equal to half the period
of the natural vibration of the diaphragm, and wherein the internal
diameter of the resonator is less than the diameter of the
diaphragm.
22. An electrical sound-producing device comprising a body, a
diaphragm within the body dividing the interior of the body into
two chambers, a horn on the body opening into one chamber and of
increasing cross-sectional area in a direction away from said one
chamber, an electromagnet having a pair of windings in the other
chamber for deforming the diaphragm when the current is supplied to
the electromagnet, and an oscillator circuit including said pair of
windings within said other chamber for repeatedly supplying current
to the electromagnet in short duration pulses.
23. A device as defined in claim 22, further comprising a pulse
rate control circuit in said other chamber connected to said
oscillator and cyclically varying the pulse repetition rate of the
oscillator.
24. A device as defined in claim 23, in which said pulse rate
control circuit is a saw-tooth pulse generator circuit whereby the
pulse repetition frequency of the oscillator is caused to commence
each cycle at a low frequency and rise continuously to a high
frequency, thereafter recommencing at said low frequency.
Description
SUMMARY OF THE INVENTION
This invention relates to an electric sound producing device and
has as an object to provide such a device in a convenient form.
An electric sound-producing device in accordance with the invention
comprises a resilient diaphragm of ferromagnetic material, an
electromagnet whereby said diaphragm is deformed when current is
supplied to said electromagnet, and an oscillator for repeatedly
supplying current to said electromagnet in short duration
pulses.
BRIEF DESCRIPTION OF THE DRAWINGS
In the accompanying drawings:
FIG. 1 is a section through an example of a device in accordance
with the invention;
FIG. 2 is a fragmentary section on line 2--2 in FIG. 1,
FIG. 3 is a view like FIG. 1 showing another example of the
invention, and
FIGS. 4, 5 and 6 are circuit diagrams of three electrical circuits
for use with either of the embodiments shown in FIGS. 1 to 3,
and
FIG. 7 is a view like FIG. 1 showing yet another example of the
invention, and
FIG. 8 is a circuit diagram which is specifically intended for use
with the example of FIG. 7 but which could also be used with the
examples of FIG. 1 and 2 or FIG. 3.
DESCRIPTION OF THE PREFERRED EMBODIMENT
The device shown in FIGS. 1 and 2 includes a body formed of a
synthetic resin material in two parts, namely a base 10 and a cap
11. The base 10 and the cap 11 are fitted together with mating
cylindrical surfaces so that the cap can be turned relative to the
base 10. A plurality of abutments 12 on the base 10 coact with a
series of inclined ramp faces 13 in the cap to determine the
relative axial positions of the cap and base. An adhesive 14 is
used to secure the two parts together after adjustment as will be
explained hereinafter.
A diaphragm member 15 is carried by the cap 11. This diaphragm
member is formed from thin steel sheet and has a flat portion 16, a
rim 17, a cylindrical marginal portion 18 having an external rib 19
thereon and a lip 20 around its free edge. The rib 19 is a snap fit
in an internal groove in the cap. The flat portion 16 of the
diaphragm is free to vibrate in a direction perpendicular to its
plane and by making its diameter 1 inch and its thickness 0.01
inch, a natural frequency of approximately 3,000 Hz can be
obtained. This is a frequency to which the normal human ear is
particularly sensitive.
The base 10 has an integral spigot 21 therein extending
perpendicularly to the plane of the flat portion 16 of the
diaphragm member 15. Mounted on this spigot 21 is a mild steel
electromagnet core 22 of longitudinally split tubular form. A coil
23 is mounted on this core 22. A shallow cup-shaped steel member 24
is fitted on the base part 10 with the core 22 in contact with it
around a hole in the member 24 surrounding the spigot 21. The edge
of the member 24 receives the lip 20 of the diaphragm member 15, so
that the diaphragm member 15, the core 22 and the member 24 form a
magnetic circuit with an air-gap between the core 22 and the centre
of the flat portion 16 of the diaphragm member 15.
The drive circuit for the coil 23 has its components supported on
an annular insulation member 25 itself carried by wires 26
extending through holes in the member 24 and the base 10 and
connected to power input terminals 27. One of the wires 26 is
insulated to prevent the terminals 27 being short-circuited by the
member 24.
As shown in FIG. 4, which illustrates a very simple circuit for the
device, the coil 23 has two windings 28 and 29. The winding 28 has
one end connected to a positive input terminal 27 and its other end
is connected to the collector of an n-p-n transistor 30. This
transistor 30 has its emitter connected to the other terminal 27. A
resistor R.sub.1 is connected between the collector of the
transistor 30 and the anode of a diode 31 which has its cathode
connected to the positive terminal 27.
The other winding 29 is connected at one end to the base of the
transistor 30 and at the other end to one electrode of a capacitor
C and one end of a resistor R.sub.2. The other electrode of the
capacitor C is connected to the negative terminal 27 and the other
end of the resistor R.sub.1 is connected to the positive terminal
27.
The circuit described forms an oscillator which operates to produce
a train of pulses in the coil 23. When the circuit is first
connected to the battery the capacitor C charges up through the
resistor R.sub.2 until current starts to flow to the base of the
transistor 30. The resulting collector current through the winding
28 induces a voltage in the winding 29 which drives the transistor
30 into a fully conducting condition. The current in winding 28
increases until the electro-magnet is saturated when the induced
voltage falls and the transistor becomes nonconductive. The current
in winding 28 then flows through the resistor R.sub.1 and the diode
31 and decays. Meanwhile, the capacitor C has been partially
discharged and this then recharges to initiate another pulse. The
pulse repetition frequency can be varied by varying the values of
the resistor R.sub.2 and the capacitor C, and this frequency is
chosen so as to be substantially less than the natural frequency of
the diaphragm. For efficient operation the resistor R.sub.1 is
chosen so that the pulse length is approximately equal to half the
natural period of the diaphragm.
The device thus produces a train of pulses of high frequency sound.
The quality of the sound can be varied by a suitable choice of the
natural frequency of the diaghragm, and the pulse repetition
rate.
The device can be inexpensively produced and can produce a
relatively loud noise for a small power consumption. It has the
advantage over conventional electromechanical devices incorporating
contact breakers that there are no wearing parts and dirt and
corrosion will not significantly affect the operation of the
device.
In the circuit shown in FIG. 5 there are three additions to the
circuit of FIG. 4. Firstly a resistor R.sub.3 is connected in
series with the capacitor C and the winding 29. In the circuit of
FIG. 4 the pulse length may tend to vary somewhat with variations
of temperature owing to possible variations in the incidental
resistance of the base-emitter circuit of the transistor 30. The
inclusion of the resistor R.sub.3 stabilizes this resistance and
hence the pulse length. Secondly the positions of the resistor
R.sub.1, and the diode 31 are interchanged and a capacitor C.sub.2
is connected between the cathode of the diode 31 and the negative
terminal 27. This capacitor C.sub.2 reduces the level of electrical
interference injected back into the supply by operation of the
device and also gives a measure of protection to the transistor 30
from high peak transient voltages in the supply which may result
from the operation of other equipment, from the same supply.
Finally a diode 32 is introduced between the positive terminal 27
and the resistor R.sub.1 to protect the transistor from damage
caused by reverse voltages resulting from inadvertently connecting
the terminals 27 to the incorrect terminals of the battery or other
supply.
As a further possibility the device may be arranged to operate
intermittently either by connecting the terminals 27 to the supply
via a thermal-type flasher unit or as shown in FIG. 6. In this case
the circuit 33 which corresponds to the circuit of FIG. 5 with two
exceptions operates as before to supply pulses to the winding 28.
The capacitor C.sub.2 is, however, shown in an alternative position
between the cathode of the diode 32 and the negative terminal 27.
In this position it still provides suppression of electrical
interference, but safeguards the transistor 30 against high peak
transient voltages to a lesser extent. The other modification is
the disconnection of the winding 29 from the cathode of the diode
32 and its connection instead to the output terminal 35 of a
multivibrator 34. This multivibrator is of conventional form
including two n-p-n transistors 36, 37 with their collectors
connected via resistors 38, 39 respectively to the cathode of diode
32 and their emitters connected to the negative terminal 27. The
bases of the transistors are connected via resistors 40, 41
respectively to the cathode of the diode 32. A capacitor 42
connects the base of the transistor 37 to the collector of the
transistor 36. A capacitor 43 is connected between the base of the
transistor 36 and the anode of a diode 44 having its cathode
connected to the collector of the transistor 37. A resistor 45 is
connected between the anode of the diode 44 and the cathode of the
diode 32. The output terminal 35 is connected to the collector of
the transistor 37.
It will be appreciated that the multivibrator produces an
intermittent output. The circuit 33 will operate only when an
output is received from circuit 34, i.e. during these periods when
the transistor 37 is non-conductive.
In the alternative embodiment of the invention shown in FIG. 3, the
cap 11 is replaced by a resonator 46 which fits on to the base 10
like the cap 11 and has an internal groove to receive the rib 19 on
the diaphragm member. The resonator 46 has tubular portion 47
connected at one end to an annular wall portion 48 adjacent the
diaphragm member. The other end of the portion 47 has an end wall
49 which is perforated so that the tubular portion 47 is
effectively and acoustically open at both ends. The length of the
portion 47 is chosen so that its fundamental frequency is
approximately equal to the natural frequency of the diaphragm. Thus
when the diaphragm is caused to vibrate a resonance condition will
be established and the quality and volume of the sound produced
will be affected.
In the example shown the internal diameter of the tubular portion
47 is less than the diameter of the flat portion 16 of the
diaphragm member. This too has an effect on the quality of sound
produced by the device. In the case where the tubular portion 47
has a diameter equal to or greater than the diameter of the
diaphragm the acoustic loading on the diaphragm is low and the
diaphragm/resonator combination would tend to "ring" at a
relatively low volume after initiation of vibration of the
diaphragm. With a reduced diameter resonator tubular portion 47 the
acoustic loading is increased so that a shorter and more intense
wave train is produced.
Any of the three circuits of FIGS. 4 to 6 may be used in
conjunction with the device of FIG. 3.
Mention is made above of axial adjustment of the position of the
cap 11 (or resonator 46) relative to the base 10 with a view to
varying the air gap between the end of the core 22 and the flat
portion 16 of the diaphragm member 15. Such adjustment is effected
during assembly of the device by fitting the cap 11 and base 10
together with the adhesive 14 between them and adjusting the cap 11
before the adhesive sets. The terminals 27 are connected to a
supply and the cap 11 is turned to reduce the airgap until the
diaphragm is heard to strike the core, the cap is then turned in
the opposite direction until such striking ceases. The adhesive is
then left to set permanently fixing the cap in its adjusted
position and also sealing the body against the ingress of dirt and
liquids. The holes in the base 10 through which the wires 26 are
passed would likewise be sealed.
Alternatively sealing of the body could be effected by ultrasonic
welding after adjustment of the gap.
Adjustment of the airgap to the minimum is of some importance in
obtaining maximum efficiency from the device. As mentioned above
the pulse length is arranged to be approximately equal to one half
of the natural vibration of the diaphragm. Thus if the diaphragm
commences at rest in its normal position it will be moved towards a
new equilibrium position appropriate to the magnetic field set up
by the current in the coil. On reaching this position the diaphragm
will continue to move under its own momentum with the magnetic
attraction progressively increasing.
Finally the diaphragm reaches a rest position and, ideally it is at
this point that the pulse to the electro-magnet terminates.
Clearly, therefore, the total displacement of the diaphragm will
increase with reduction of the air gap for the same power
consumption.
In the example shown in FIG. 7 the cap 11 or resonator 46 is
replaced by an exponential horn 50. Once again the narrow end of
this horn is of smaller diameter than that of the diaphragm to
place a high acoustic load on the diaphragm. A high intensity sound
can thus be obtained.
The circuit of FIG. 8 utilises an oscillator 33 as before, with a
saw-tooth pulse generator circuit 59 including a capacitor 51
connecting the resistor R.sub.2 to the negative terminal 28 and a
further resistor 52 connecting it to the positive terminal 27. Also
connected to the resistor R.sub.2 is the emitter of a p-n-p
transistor 53 the collector of which is connected to the negative
terminal via a resistor 54. The base of the transistor 53 is
connected via a resistor 55 to the negative terminal and via a
resistor 56 to the base of another -p-n-p transistor 57, the
collector of which is connected to the base of the transistor 53. A
capacitor 58 connects the base of the transistor 57 to the
collector of the transistor 53. The emitter of the transistor 57 is
connected to the positive terminal.
The cycle of operation of the circuit may be regarded as commencing
with the capacitor 51 uncharged and the transistor 53
non-conductive. When the supply is connected the capacitor 51
charges up so that initially the voltage on the resistor R.sub.2 is
at the negative terminal voltage but this rises as the capacitor 51
charges, progressively increasing the pulse repetition frequency of
the oscillator. When the voltage across the capacitor 51 exceeds
the bias applied to the base of the transistor 53, the latter
starts to conduct and the changing voltage at its collector, caused
by current flow through the resistor 54, is applied to the base of
the transistor 57 via the capacitor 58. This in turn causes the
bias on the base of the transistor 53 to be reduced and the
regenerative action causes transistor 53 to switch fully on and
discharge the capacitor 51 extremely rapidly. The cycle then
restarts.
Thus the device emits pulses of sound at the resonant frequency of
the diaphragm, which is preferably as mentioned above, in the
region of 3,000 Hz. The pulse repetition frequency varies
cyclically from a low frequency rising to a high frequency and then
commencing at the low frequency again. The total effect is a sound
of which the apparent frequency follows this pattern, although in
fact all the sound emitted is at or near the aforementioned
resonant frequency.
If desired, an additional transistor may be introduced between the
resistor R.sub.2 and the capacitor 51 to allow the magnitude of the
current handled by the "time-base" circuit to be reduced.
Alternatively the additional transistor may be connected to the
base of the transistor 30. In each case the additional transistor
would be connected as an emitter follower.
The horn of FIG. 7 may also be used in conjunction with any of the
circuits shown in FIGS. 4, 5 and 6.
* * * * *