The present invention concerns a plasticizing unit for an injection molding machine having the features of the classifying portion of claim 1 and a method having the features of the classifying portion of claim 7.
AT 512 647 B1 to the present applicant discloses a method of ascertaining a radial temperature profile in a plasticizing cylinder of a plasticizing unit of the general kind set forth. The method uses the principle of transit time measurement of ultrasound signals. The following are further known:
The plasticizing operation can involve temperature fluctuations in the plasticizing cylinder, which detrimentally influence the quality of the plasticized melt.
The object of the invention is to provide a plasticizing unit of an injection molding machine, in which temperature fluctuations influencing the quality of the plasticized melt can be detected, as well as the provision of a corresponding method.
Advantageous embodiments are defined in the appendant claims.
The unwanted fluctuations in the product quality of injection-molded plastic components are to be attributed in particular to detrimental axial temperature profiles (temperature gradients) in the plasticized melt as they are generally much higher than the radial temperature profiles. The axial temperature profiles occur due to the reduction in the effective screw length in the metering feed of the plastic melt into the screw prechamber. To permit active open-loop or closed-loop control of the melt temperature in the metering feed (for example by means of dynamic pressure and/or speed of rotation of the screw), measurement of the axial melt temperature is necessary. The invention permits that in a simple fashion.
Advantages of the invention:
The invention is discussed in detail for various embodiments with reference to
The Figures show a portion of a plasticizing unit 1 for an injection molding machine in the form of a rotatable plasticizing screw 4 arranged displaceably in a cylinder bore of a plasticizing cylinder (with wall 2). The plasticizing screw 4 is moved away from the injection nozzle by the metering feed of plasticized plastic material in the region between the injection nozzle (not shown) and the tip of the plasticizing screw 4 (screw prechamber 3). In that case a so-called mass cushion is formed in the screw prechamber 3.
If an ultrasound pulse is sent through a plastic melt along a sound transit path S (between an ultrasound transmitter and an ultrasound receiver) the transit time ttransit of the pulse through the melt derives from the formula:
wherein cL,S(p,T) denotes the longitudinal speed of sound which is dependent on the pressure p and the temperature T at a position s along the sound transit path S.
If the longitudinal speed of sound cL is known as the function of the pressure p and the temperature T (by calibration measurement or preferably by looking up tables known to the man skilled in the art , which give the transit time of sound for various plastics—that is possible because at least approximately a constant pressure obtains in the screw prechamber in the metering operation), it is possible to arrive at the mean temperature along the sound transit path S from the transit time measurement.
Ultrasound transit time measurements are carried out at a plurality of axial positions for measuring the axial temperature distribution in the screw prechamber 3. The measurements can be performed by means of so-called reflection or transmission measurements.
Reflection measurement is shown in
An ultrasound transducer array with a plurality of ultrasound transducers 5 is disposed along the screw prechamber 3 at the wall 2 of the plasticizing cylinder. Alternatively measurement can also be implemented with an ultrasound transducer 5 alternately at different axial positions over a plurality of injection molding cycles.
An ultrasound pulse which is passed into the plasticizing cylinder is reflected at the upper edge of the cylinder bore. A part of the sound energy further passes through the plasticized plastic melt, is reflected at the lower edge of the cylinder bore and goes back to the ultrasound transducer. The speed of sound (at the dynamic pressure pdynamic during the metering feed) and thus the mean melt temperature Tm along the sound transit path can be inferred from the difference in the transit times of reflections at the upper and lower edges (tupper and tlower) of the cylinder bore and the known diameter of the cylinder bore dcylinder:
Measurement at various axial positions gives an axial temperature profile in the screw prechamber 3. Calculation is effected in an evaluation unit 8 shown in
In transmission measurement, shown in
An ultrasound pulse passed from an ultrasound transducer 5 of the transmitter array 6 into the plasticizing cylinder passes through the first half of the wall 2 of the plasticizing cylinder, further through the plastic melt and thereafter through the second half of the wall 2 of the plasticizing cylinder to the opposite ultrasound transducer 5 of the receiver array 7. The transit times ts, tc through the wall 2 of the ttotal, cylinder still have to be deducted from the total transit time measured in that way, of the t ultrasound pulse. Those transit times can be ascertained by reflection measurements by means of the ultrasound transducers 5 in the transmitting and receiving arrays 6 and 7. The speed of sound is deduced from
An axial temperature profile in the screw prechamber 3 is afforded by the measurement at various axial positions. Calculation is effected in an evaluation unit 8 shown in
The measurement of te is relatively tedious. On the assumption that an almost rotationally symmetrical temperature profile prevails in the wall 2 te is approximately equal to ts. It is thus possible to dispense with the measurement of te.
The invention can be used to produce a temperature distribution which is advantageous for the injection molding process, in the metering feed.
The start of measurement is effected in the metering feed. As soon as the plasticizing screw 4 pulls back and the sound transit path is thus free at a position a measurement in respect of the speed of sound can be effected at the respective position. An advantage with the arrangement is the fact that the pressure (dynamic pressure) in the screw prechamber 3 is known and is approximately constant and there is no need to directly calculate the pressure- and temperature-dependent melt temperature from the measured speeds of sound.
Just the change in the speed of sound at various axial positions is sufficient to ascertain axial temperature differences (axial temperature gradient). Conversion of the ultrasound transit times into speeds of sound or temperatures is effected in an evaluation unit 8. The calculated speeds of sound or temperature values are used by an open-loop or closed-loop control 9 to influence machine parameters (for example dynamic pressure, preferably the screw speed) by way of a motor M driving the plasticizing screw in such a way that a temperature drop in the screw prechamber 3, by virtue of a reduced screw length of the plasticizing screw 4, can be compensated. That influence is preferably implemented from one cycle to another, that is to say not necessarily during a cycle of the plasticizing unit 1 or the injection molding machine of which the plasticizing unit 1 is a part.
The evaluation unit 8 and the open-loop or closed-loop control unit 9 can be physically jointly provided in one component.
In all embodiments the ultrasound transducers 5 bear against the wall 2 of the plasticizing cylinder and are therefore not disposed in bores in the wall 2, which extend through the wall 2. It would be conceivable for the ultrasound transducers 5 to be arranged sunk in blind bores in the wall 2, for example in the case of space problems with heating bands mounted on the plasticizing cylinder.
Advantageously the ultrasound transducers 5 are pressed against the wall 2 of the plasticizing cylinder, for example by way of magnetic holding means. The application of an ultrasound gel between the ultrasound transducers 5 and the wall 2 is commendable. If passive cooling of the ultrasound transducers 5 by the ambient air is not sufficient it is also possible to provide for active cooling.
Number | Date | Country | Kind |
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639/2014 | Aug 2014 | AT | national |