Field of the invention
[0001] The invention relates to production process automation and is directed at producing
mechanical ultrasonic oscillations by using electric energy.
Prior art
[0002] An ultrasonic phase stabilized oscillator is known, comprising serially connected
driving oscillator and power amplifier, connected to an ultrasonic converter, connected
to a current sensor output and a phase locked loop connected to an adjusting element,
its output connected to the driving oscillator input (patent
RU 25699, cl. B 06 B 1/0, 20.10.2002)
[0003] The disadvantage of the known device is an impossibility to implement the entire
amplitude-frequency response, as there are branches instable is forced oscillation
regimes. Precisely for this reason the device does not have sufficient stability what
decreases possible technologic load.
[0004] Possible configurations of amplitude-frequency responses of such ultrasonic technologic
system at various values of feeding force P are given in Fig.1. Sceleton curves «a»
defining the dependence of natural frequency of non-linear system on the amplitude
of oscillations and the line of limiting amplitudes «b», that is an envelope of resonance
curves, are shown with thin solid lines.
[0005] At P=0, i.e. at idle running we have a typical amplitude-frequency response of a
linear oscillating system. With the feeding force increase up to a certain critical
value P
cr the resonance curve nature does not change, and the resonance frequency moves to
a higher frequency area. Upon exceeding the critical value of the feeding force the
resonance curve appearance leaps. An instable branch appears which is shown by a dot-and-dash
line. In this case the resonance mode may be achieved either by pulling oscillations
from the higher frequency area or by hard start, by imparting additional energy to
the system. But even if the resonance regime is successfully achieved, it's rather
problematical to keep near the resonance state, as a small exciting frequency decrease
or small load increase lead to failure of oscillations as is shown by a vertical arrow
in Fig.1
[0006] Therefore it is necessary to control frequency when the ultrasonic system operating
conditions are changed. Apparently that at minor change of conditions the system oscillations
amplitude, tuned to its natural frequency ω
O, falls sharply. The similar in operation device as well as majority of known devices
with forced oscillations implementation attempt to implement control by changing the
driving oscillator frequency. Meanwhile it is taken into account that at resonance
the phase shift between voltage and current in the power circuit is a constant value
and deviation from this constant value is used as a criterion of tuning to the resonance
frequency.
[0007] It's worth while to note that regardless of the driving oscillator frequency control
unit structure, the system operating in the forced oscillations regime is able to
work only at feeding forces P < P
cr until non-linear effects in resonance curves behavior do not show themselves. At
P > P
cr any overregulation leads to oscillations failure. That's why the known device does
not allow to use all performance potentials of ultrasonic technologic systems. The
case is that the implementation of non-linear resonance modes would allow to operate
at feeding forces, several tens times exceeding the critical value P
cr.
[0008] The closest technical solution is the device for exciting and automatic stabilization
of resonance oscillations of ultrasonic systems, comprising an electroacoustic converter
and oscillation sensor connected to an amplifier, which is integrated into a feedback
circuit, and a power supply (certificate of authorship
SU 483148, cl. B 06 B 1/02, 05.09.1975). A microphone gapped with regard to a free butt-end
of the oscillating system, excited by the electroacoustic converter, is used as an
oscillation sensor.
[0009] The disadvantage of this device is constructive complexity of microphone installation
into the oscillating system package, due to the necessity to ensure running wave emission
by the free butt-end of the oscillating system because any wave reflections from the
package walls result is standing waves generation and make the device unable to work.
Disclosure of the invention
[0010] The purpose of the invention is to remove the above disadvantages. The technical
result of the invention implementation is simplification of the construction of the
device for exciting and stabilization of ultrasonic systems, enhancement of a possible
technological load and increase of the device operation stability. The set task is
solved and the technical result is achieved by the fact that the device for exciting
and automatic stabilization of resonance oscillations of ultrasonic systems, comprising
an electroacoustic converter connected to an amplifier, which is integrated into a
feedback circuit, and a power supply is equipped with a current intensity sensor in
the power circuit of the electroacoustic converter which is formed by means of the
feedback circuit equipped with the phase shifter, the input thereof is connected to
the current intensity sensor and the output thereof is connected to the amplifier
input. The proposed device does not have the prior art disadvantages, because the
feedback is arranged using electric parameters instead of mechanic ones.
Short description of drawings
[0011]
Fig.1 shows change of amplitude-frequency responses of an ultrasonic technologic system
working into a non-linear technologic load upon its change;
Fig.2 shows the device block structure;
Fig.3 shows the amplifier response.
Best method for carrying out the invention
[0012] The device for exciting and automatic stabilization of resonance oscillations of
ultrasonic systems comprises an oscillation system, its oscillations are excited by
electroacoustic converter, piezoelectric converter 1, connected to amplifier 2, which
is integrated into a feedback circuit, and power supply 3. Current intensity sensor
4 is connected to electroacoustic converter power circuit I
3 which is formed by means of the feedback circuit. The feedback circuit is also equipped
with phase shifter 5, the input thereof is connected to the current intensity sensor
4 and the output thereof is connected to the amplifier input 2. Alternative electric
voltage is fed to converter 1 coatings what results in exciting of mechanical oscillations
that are transferred to a tool installed at a free end of the concentrator. The whole
system is squeezed up against the work piece (marked by section lining) by static
force (Fig.2). A vibrating tool performs the technological operation. The technology
process execution efficiency depends mainly on amount of pressure effort and tool
oscillation amplitude. The more are these amounts the higher is the performance of
the device.
[0013] This circuit lacks the driving oscillator, and the oscillation frequency is not imposed
on the device from the outside. The system operates in the self-excited oscillation
regime instead of that of forced oscillations. In this case the oscillations are excited
using the positive feedback circuit.
[0014] In the proposed device the positive feedback circuit is made using electric parameters,
i.e. the intensity of current in the converter power circuit. In order to ensure excitation
and maintain resonance oscillations upon technologic load variation over a wide range,
a phase shifter is integrated into the feedback circuit, ensuring phase shift between
the converter supply current and voltage, corresponding to the resonance regime.
[0015] As the device operates in the self-excited oscillation regime the non-linear amplifier
is constructed so as to ensure the self-excitation of oscillations. Self-excitation
occurs if the initial amplification factor is big enough. The self-excitation occurs
always in case of relay characteristic. The oscillation amplitude is adjusted by amplifier
response limiting level (Fig.3), where U
S is sensor voltage, proportional to the current intensity in the power circuit and
U
H is electroacoustic converter supply voltage. The slope of the initial part of the
response defines the initial amplification factor. If a certain value of the initial
amplification factor is exceeded the self-excitation of oscillations occurs.
[0016] The amplitude of steady oscillations is determined by U
V saturation level. At a certain phase shift value, set by the phase shifter, the oscillations
of the ultrasonic system occur at its resonance frequency even if it changes owing
to change of system or technologic load parameters over a wide range.
Industrial applicability
[0017] Owing to its implementation in the self-oscillation regime device, by changing the
phase in the feedback circuit the entire amplitude-frequency response can be implemented,
including the branches instable in the forced oscillation regime. Due to precisely
this reason the claimed device is absolutely stable and allows to increase the technologic
load in tens of times compared to equally powerful systems operating in the forced
oscillation regime. This device can be used for turning, wire drawing, strengthening
surface treatment, etc.