Torsional vibrator

Abstract: A torsional vibrator (1) comprises a direct-current electric motor (2) provided with induced windings (7) supplied with direct current through inverter means (11) capable of changing their polarity in an alternating manner with a preselected frequency. To a shaft (8) of the electric motor (2) a wheel (13) is made integral that is formed by a rim (14) and by a tyre (15) and acceleration transducers (18, 19, 20, 21) are associated with the rim (14) and with the tyre (15) of the wheel. The shaft (8) of the motor (2) is driven to execute angular oscillations (27) that torsionally excite said wheel (13) and cause it to vibrate in rotational direction. The acceleration transducers (18, 19, 20, 21) detect rotational vibrations and provide measurements of acceleration of the rim (14) and of the tyre (15).

Description: The present invention relates to a torsional vibrator capable of torsionally exciting a tyre of a wheel and of providing measurements of angular acceleration. Such measurements of angular acceleration allow the determination of the torsional foundation stiffness of the tyre, which is a concentrated parameter that represents the pneumatic stiffness of sidewall and carcass of the tyre, with the tyre inflated, that is to say the stiffness between the tread strip + belts + carcass and rim of a wheel. P.W.A. Zegelaar et al. in "Tyre Models for the Study of In-Plane Dynamics", The Dynamics of Vehicle on Roads and on Tracks, Supplement to Vehicle System Dynamics, Volume 23, 1994" describe an apparatus for measuring the foundation stiffness of a tyre of a wheel. The tyre, fastened to a rim of the wheel, is constrained within a "circular casing" and a static torque is applied to the rim. From the measurement of the angle of rotation of the rim the torsional foundation stiffness of the tyre is obtained. This apparatus provides a measurement of a static type that represents only with a certain approximation the foundation stiffness of the tyre under dynamic conditions, operating on the road. The object of the present invention is a torsional vibrator that allows the determination of the torsional foundation stiffness of a tyre by means of measurements of a dynamic type. The above mentioned object is achieved, according to the invention, with a torsional vibrator comprising a direct-current electric motor provided with inductor windings, with induced windings and with a shaft with which a wheel is made integral that comprises a rim and a tyre, first acceleration transducer means associated with said rim, second acceleration transducer means associated with said tyre, said induced windings being connected to means for supplying direct-current power through inverter means capable of changing the polarity of said induced windings in an alternating manner with a preselected frequency so that said shaft is driven to execute angular oscillations that torsionally excite said wheel, causing it to vibrate in rotational direction, said first and second acceleration transducer means detecting rotational vibrations and providing measurements of acceleration of said rim and of said tyre. The vibrator provides a torque of the "random" type (containing a high number of frequencies) to the wheel with the tyre and the transducer means provide measurements of the angular acceleration of the rim and of the wheel. The ratio between the two angular accelerations, depending on the frequency of excitation, provides a transfer function between output (angular acceleration of the tyre) and input (angular acceleration of the rim), that exhibits a resonance peak (maximum) at the natural rotational frequency of the tyre. If, then, the transfer function is known as to amplitude and phase, within the selected range of frequency, preferably 0 - 200 Hz, and if the moment of inertia of the tyre is also known (measured, for example, with a torsional pendulum), it is possible to make a mathematical calculation of the torsional foundation stiffness Cbt of the tyre . Features and advantages of the invention will now be illustrated with reference to an embodiment thereof represented as a non-limiting example in the enclosed figures, wherein Fig. 1 is a side view, in partial cross-section, of a torsional vibrator according to the invention; Fig. 2 is a front view of the torsional vibrator of Fig. 1; Figs. 3 and 4 are graphs that show amplitude and phase of a transfer function against changes in the frequency of excitation for a wheel torsionally excited with the vibrator according to the invention. In Figs. 1 and 2 there is shown diagrammatically a torsional vibrator 1 made according to the invention comprising an electric motor 2 of the direct-current type. The motor 2, in turn, comprises a carcass, or stator, 3 fastened to a supporting structure 4, inducer windings 6 and induced windings 7 supported by a rotor 5. The rotor 5 is keyed rigidly on a shaft 8, rotatably supported by the carcass 3. The inducer windings 6 are connected to a direct-current power supply unit at a stabilized voltage, not shown, by means of terminals 9. The induced windings 7 are connected to the direct-current power supply by means of collectors 23, conductors 10 and inverter means 11 capable of changing the polarity of the windings 7, and thus of the induced magnetic field, in an alternating manner (sinusoidal) with a preselected frequency ranging from 1 Hz to 200 Hz. The inverter means 11 can consist of high-power drives to alternate the polarity even at a high frequency. On the shaft 8 there is rigidly keyed a hub 12 provided with a flange on which there is fastened, by means of bolts 26, a rim 14 (Fig. 2) of a wheel 13. The wheel 13 comprises a tyre 15 provided with a tread 16. Two acceleration transducers 18 and 19, consisting of linear accelerometers, are fastened to the rim 14 in a diametrically opposite position, and two acceleration transducers 20 and 21, consisting of linear accelerometers, are fastened to the tyre 15 in a diametrically opposite position by means of a clamp 22, closed by a screw 28, that holds the tread 16 circumferentially. When the torsional vibrator 1 is in operation, the induced windings 7 are supplied with direct-current in an alternating manner through the inverter means 11 so that in the motor 2 a rotating magnetic field is generated that changes direction of rotation alternately. The driving shaft 8 performs angular oscillations (arrow 27) and torsionally excites the wheel 13 that thus vibrates in a rotational direction. The accelerometers 18, 19, 20 and 21 detect rotational vibrations and provide measurements of angular acceleration of the rim 14 and of the tyre 15, that is of the tread strip + belts + carcass. The torsional vibrator 1 provides a torque of the "random" type (containing a high number of frequencies) to the wheel with the tyre. In particular, the frequencies at which the driving shaft 8, and thus the wheel 13, vibrates torsionally, are linked to the frequencies of inversion of the rotating magnetic field. Thus, a rotational electric vibrator is available that allows to exite the tyre 15 torsionally in the range of frequencies that is desired. The measurements that are performed by means of the linear accelerometers 18, 19, 20 and 21 are the linear acceleration of the rim 14 and that of the tyre 15. From the linear acceleration of each accelerometer 18 or 19, on the rim 14 a calculation is made, given the latter's distance from the center of the wheel, of the angular acceleration of the rim, an average is then calculated of the measurement provided by the two accelerometers 18 and 19. The same procedure is carried out for the two accelerometers 20 and 21 on the tread 16 of the tyre. Calculating the ratio between the angular acceleration of the tyre 15 and that of the rim 14 (taken as an input), a transfer function in amplitude and phase is obtained, depending on the frequency of excitation. The Applicant has made a torsional vibrator like the one described wherein the motor 2 has a rating of 1.47 kW and a speed of 3,000 rpm. There is shown in Figs. 3 and 4 a plotting of the amplitude A and of the phase 0° (degrees) of a transfer function against the frequency of excitation (Hz). The transfer function is obtained from the ratio between angular acceleration of the rim and angular acceleration of the tyre of a wheel torsionally excited with the torsional vibrator 1. The tyre subjected to test is of the type P 6000, size 185/60 R 14, with an inflation pressure p = 2 bar. Once the transfer function between the two angular accelerations is known, that shows a resonance peak at the natural torsional frequency of the tyre, it is possible to obtain mathematically, applying the formulas of the dynamic systems with one degree of freedom, the torsional foundation stiffness of the tyre Cbt. For the calculation, it is necessary to know the moment of inertia of the tyre, that is determined experimentally, for example with a torsional pendulum, not shown as it is known. It is observed that the measurement of the torsional stiffness is of a dynamic type (frequency response of the tyre) and not static. Instead of the linear accelerometers 18, 19, 20 and 21 angular accelerometers can be used.

Claims: A torsional vibrator (1) comprising a direct-current electric motor (2) provided with inductor windings (6), with induced windings (7) and with a shaft (8) with which a wheel (13) is made integral that comprises a rim (14) and a tyre (15), first acceleration transducer means (18, 19) associated with said rim (14), second acceleration transducer means (20, 21) associated with said tyre (15), said induced windings (7) being connected to means for supplying direct-current power through inverter means (11) capable of changing the polarity of said induced windings (7) in an alternating manner with a preselected frequency so that said shaft (8) is driven to execute angular oscillations (27) that torsionally excite said wheel (13), causing it to vibrate in rotational direction, said first and second acceleration transducer means (18, 19, 20, 21) detecting rotational vibrations and providing measurements of acceleration of said rim (14) and of said tyre (15). A torsional vibrator according to claim 1, characterized in that said frequency ranges from 1 Hz to 200 Hz.

Inventors: DI BERNARDO CARLO, MATRASCIA GIUSEPPE, DI BERNARDO, CARLO, MATRASCIA, GIUSEPPE
Applicants: PIRELLI, PIRELLI PNEUMATICI
Application year: 1996
Main classification: G01M17
IPC codes: G01M7, B60C23, G01M17