SENSOR FOR WEAR MEASUREMENT, METHOD OF MAKING, AND METHOD OF OPERATING SAME

Abstract

A wear sensor comprising: an insulating substrate having a top surface and a bottom surface; a conductive electrode formed on said top surface of said insulating substrate; an insulating wear lining material having a first side secured to said top surface of said insulating substrate and conductive electrode, an opposite second side that will be worn down by relative motion between the wear sensor and a moving component; one or more contact points where the electrical properties between the electrode and the moving component can be measured; and one or more perforations through the thickness of the substrate and electrode, through which an adhesive may flow, thereby increasing the peel strength between the wear sensor and race or between the wear sensor and the wear liner.

Claims

1.-6. (canceled)

7. A wear sensor comprising: a conductive filament that is deposited on or woven into an insulating, wear resistant material, such that the capacitance between the conductive filament and a moving component increases as the wear resistant material is worn away.

8. A wear sensor according to claim 7 wherein the conductive filament is a carbon fiber.

9. A wear sensor according to claim 7 wherein the conductive filament is a carbon nanotube yarn.

10. A wear sensor according to claim 7 wherein the conductive filament is a metal wire.

11. A wear sensor according to claim 7 wherein the conductive filament is a metal coated fiber.

12. (canceled)

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0023] These and other objects, features and advantages of the present invention will be more fully disclosed or rendered obvious by the following detailed description of the preferred embodiments of the invention, which is to be considered together with the accompanying drawings wherein like numbers refer to like parts and further wherein:

[0024] FIG. 1A illustrates a new sleeve bearing with a sensor inserted into a wear liner in accordance with the present invention;

[0025] FIG. 1B illustrates a symmetrically worn sleeve bearing with a sensor inserted into a wear liner in accordance with the present invention;

[0026] FIG. 1C illustrates a non-concentrically worn sleeve bearing with a sensor inserted into a wear liner in accordance with the present invention;

[0027] FIGS. 2A-2D illustrate a sleeve bearing with a capacitive sensor inserted into a wear liner in accordance with the present invention, wherein the capacitive sensor is to be measured with a probe contact;

[0028] FIGS. 3A-3D illustrate a sleeve bearing with a capacitive sensor inserted into a wear liner in accordance with the present invention, wherein the sleeve bearing comprises an antenna with significant inductance for creating a resonant LC circuit;

[0029] FIGS. 4A-4D illustrate a spherical bearing with a capacitive sensor inserted into a wear liner in accordance with the present invention, wherein the capacitive sensor is to be measured with a probe contact;

[0030] FIGS. 5A and 5B illustrate a method of interrogating a capacitive sensor inserted into a wear liner of a spherical bearing in accordance with the present invention, using a capacitance meter;

[0031] FIGS. 6A-6D illustrate a spherical bearing with a capacitive sensor inserted into a wear liner in accordance with the present invention, and wherein the spherical bearing comprises an antenna with significant inductance for creating a resonant LC circuit;

[0032] FIGS. 7A and 7B illustrate a method of interrogating the capacitive sensor described in FIGS. 6A-6D with a tracking generator, matching network, interrogating antenna, and a spectrum analyzer;

[0033] FIG. 8A illustrates a new square telescoping bearing with a sensor inserted into a wear liner in accordance with the present invention;

[0034] FIG. 8B illustrates a worn square telescoping bearing with a sensor inserted into a wear liner in accordance with the present invention; and

[0035] FIGS. 9A-9C depict a process flow for producing the wear liner of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0036] The present invention comprises an insulating wear liner with a sensor that is positioned either within the liner or placed on the non-wearing surface of the liner. The sensor is comprised of a conductive electrode and one or more pads for interrogating the electrical properties of the sensor. The liner is situated between the race and the moving part.

[0037] By way of example but not limitation, a sensor may be positioned inside of the wear liner of a sleeve bearing, and the capacitance between the wear liner and the shaft can be calculated in the new condition of the shaft and wear liner, and after wear by a shaft.

[0038] Looking now at FIG. 1A, FIG. 1 illustrates a new sleeve bearing with a sensor inserted into the wear liner according to this invention.

[0039] The new, unused sleeve bearing is assembled with a shaft which has radius R.sub.shaft. The shaft is centered in the bearing, concentric with the race, which has a radius R.sub.race. The sensor conductive electrode is positioned inside the liner, having radius R.sub.sensor, such that all three are concentric and R.sub.race>R.sub.sensor>R.sub.shaft.

[0040] We assume the liner has a uniform dielectric constant of ∈. The new bearing, with no wear, will have a capacitance C.sub.new between the sensor and the shaft, which is given by:

[00001]$C_{\mathrm{new}}=\frac{2.Math.\pi .Math..Math.{\mathrm{.Math.}}_0.Math.\mathrm{.Math.}}{\ln \left(\frac{R_{\mathrm{sensor}}}{R_{\mathrm{shaft}}}\right)}$

[0041] Table 1 shows a calculation of capacitance for a new shaft bearing.

TABLE-US-00001 TABLE 1 Calculation of capacitance for new liner in a sleeve bearing NEW LINER inch Value Metric Unit Wear liner thickness T 0.012 0.00030 m sensor position Sp 0.006 0.00015 m Diameter of Shaft Dsh 0.500 0.01270 m Diameter of Race Dr = Dsh + 2T 0.524 0.01331 m Diameter of Sensor Ds = Dsh + 2Sp 0.512 0.01300 m Bearing Length L 0.500 0.01270 m Dielectric constant of liner e 2 2 Permittivity of vacuum e0 8.85E−12 F/m Radius of shaft Rsh = Dsh/2 0.00635 m Radius of race Rr = Dr/2 0.00665 m Radius of sensor Rs = Ds/2 0.00650 m Capacitance sensor-shaft C = 2 * pi * e * e0/(ln(Rs/Rsh) 4689.2 pF/m Capacitance Bearing, pF Cb = C * L 59.6 pF

[0042] There will also be capacitance between the sensor electrode and the outer race, but this value should be constant over the life of the bearing. Between the sensor electrode and the moving shaft, there will be wear. Accordingly, the thickness of the wear liner will decrease, and the shaft will exhibit more play. One aspect of this invention is the effect of concentricity on the measured capacitance of a sensor embedded in a wear lining. We recognize two wear modes that could occur, concentric uniform or non-concentric non-uniform.

[0043] To illustrate uniform wear, we consider a bearing that is worn with perfect symmetry so that some of the wear liner is removed from its entire circumference. Next, we position the shaft in perfect concentricity with the race and sensor electrode. FIG. 1B illustrates a symmetrically worn sleeve bearing with a sensor inserted into the wear liner according to the present invention.

[0044] In this arrangement, there are two capacitors in series, one made of air C.sub.air, and another made from the remaining liner C.sub.liner The air gap, having thickness W, will have a capacitance based on the radial gap, R.sub.liner=R.sub.shaft+W. The capacitance of that gap will follow:

[00002]$C_{\mathrm{air}}=2.Math.{\mathrm{\pi .Math.}}_0\left(\frac{{\mathrm{.Math.}}_{\mathrm{air}}}{\ln \left(\frac{\left(R_{\mathrm{shaft}}+W\right)}{R_{\mathrm{shaft}}}\right)}\right)$

[0045] Likewise, the wear liner will have a capacitance based on its thickness, equal to R.sub.sensor−R.sub.liner, or R.sub.sensor−(R.sub.shaft+W)

[00003]$C_{\mathrm{liner}}=2.Math.{\mathrm{\pi .Math.}}_0\left(\frac{{\mathrm{.Math.}}_{\mathrm{liner}}}{\ln \left(\frac{R_{\mathrm{sensor}}}{R_{\mathrm{shaft}}+W}\right)}\right)$

[0046] The total capacitance, C.sub.T, will follow that of two capacitors in series; C.sub.T=(C.sub.air×C.sub.liner) (C.sub.air+C.sub.liner). Table 2 shows the result of this calculation.

TABLE-US-00002 TABLE 2 Concentrically worn sleeve bearing CONCENTRIC WEAR inch Value Metric Unit Wear liner thickness T 0.012 0.000305 m sensor position Sp 0.006 0.000152 m Diameter of Shaft Rsh = Dsh/2 0.500 0.012700 m Diameter of Race Rr = Dr/2 0.524 0.013310 m Diameter of Sensor Rs = Ds/2 0.512 0.013005 m Bearing Length L 0.500 0.012700 m Dielectric constant of liner e 2 2 Permittivity of vacuum e0 8.85E−12 F/m Radius of shaft Rshaft 0.00635 m Radius of race Rr 0.00665 m Radius of sensor Rsensor 0.00650 m Wear W 0.004 0.00010 m Radius of liner Rliner = Rshaft + Wear 0.00645 m Capacitance shaft to liner Cair = 2 * pi * e0(1/ln(Rliner/Rshaft) 3503 pF/m Capacitance liner to electrode Cliner = 2 * pi * e0(e/ln(Rsensor/Rliner) 14180 pF/m Total Capacitance/m CT = (Cair * Cliner)/(Cair + Cliner) 2809 pF/m Capacitance C = CT * L 35.7 pF

[0047] The resulting capacitance is lower than the value calculated in Table 1 for the new bearing. We note that this is the case only if the shaft is held at the center. If loaded, the shaft will be non-concentric and the following example will apply.

[0048] Next, to illustrate the non-concentric, non-uniform case, we consider a bearing that has been loaded and worn preferentially on one side. The result is that the shaft is no longer concentric with the sensor. FIG. 1C illustrates a non-concentrically worn sleeve bearing with a sensor inserted into the wear liner according to the present invention.

[0049] The capacitance of two cylinders eccentrically located one inside the other with radii (R.sub.shaft) and (R.sub.sensor), respectively, but with the centers of the two cylinders having a distance (W) apart, will be larger than in the concentric case. Ignoring the replacement of the worn-away dielectric with air, the capacitance would be:

[00004]$C=2.Math.\pi .Math..Math.{\mathrm{.Math.}}_0.Math.\mathrm{.Math.}\left(\frac{1}{a.Math..Math.\cosh \left(-\left(W^2-R_{\mathrm{shaft}}^2-R_{\mathrm{sensor}}^2\right)/2.Math.R_{\mathrm{shaft}}.Math.R_{\mathrm{sensor}}\right)}\right)$

[0050] The capacitance is calculated for an eccentrically worn sleeve bearing in Table 3.

TABLE-US-00003 TABLE 3 Non-concentric wear of a sleeve bearing WORN LINER inch Value Metric Unit Wear liner thickness T 0.012 0.000305 m sensor position Sp 0.006 0.000152 m Diameter of Shaft Dsh 0.500 0.012700 m Diameter of Race Dr = Dsh + 2T 0.524 0.013310 m Diameter of Sensor Ds = Dsh + 2Sp 0.512 0.013005 m Bearing Length L 0.500 0.012700 m Dielectric constant of liner e 2 2 e0 e0 8.85E−12 F/m Radius of shaft Rsh = Dsh/2 0.006350 m Radius of race Rr = Dr/2 0.006655 m Radius of sensor Rs = Ds/2 0.006502 m Eccentric Wear W 0.004 0.000102 m Capacitance/m shaft to sensor C = 2 * pi * e * e0 * (1/(acosh(−(W{circumflex over ( )}2 − Rsh{circumflex over ( )}2 − Rs{circumflex over ( )}2)/2Rsh * Rs) 6440.4 pF/m Capacitance of Bearing Cb = C * L 81.8 pF

[0051] In Table 3, we see that the capacitance is significantly higher for the non-concentric worn bearing than for the new bearing. A notable aspect of this invention is that the capacitance between a metallic shaft and a sensor placed inside or behind the wear liner will increase with concentric or non-concentric wear, as long as the shaft is loaded. The capacitance is an inverse function of the liner thickness. Accordingly, the capacitance increases rapidly as the liner thickness approaches zero.

[0052] Between the two previous examples, we expect to find the non-uniform, non-concentric case to be prevalent, as the loading and wear of bearings is rarely uniform. As such, we can relate the wear of a bearing to a measurable increase in capacitance between the shaft and the sensor.

[0053] The capacitance measurement can be made at different frequencies. A standard frequency for capacitance measurement is 10 kHz. Measurements taken at a higher frequency improve the sensitivity of the measurement, but also increase the error due to interference. The optimal frequency for accuracy will depend on the electromagnetic interference in the environment surrounding the bearing. The measurement of Q factor, which can be calculated from the active and inductive current components in the sensor, provides information about the status of the liner. If at any point the gap between the sensor and the ball approaches zero, Q will drop rapidly toward zero. It will also be electrically shorted at this point. A Q under 5 indicates that the bearing needs immediate replacement, and a Q above 20 indicates a bearing with good health. The electrical shorting of the sensor and ball can also be used as an indicator that the wear liner has failed in at least one spot, and therefore needs replacement.

[0054] Turning again to FIG. 1, FIG. 1A illustrates a new sleeve bearing (without wear) 200, comprising an outer race 201, a movable shaft 203, a wear liner 206 and a sensor 205 inserted into wear liner 206.

[0055] FIG. 1B illustrates the sleeve bearing 200 of FIG. 1A after symmetric wear of wear liner 206. The symmetric wear of wear liner 206 results in a worn sleeve bearing 200 having an equal air gap 222 between wear liner 206 and movable shaft 203, with erosion of all wear on sleeve bearing 200 lining up to sensor 205.

[0056] FIG. 1C illustrates an asymmetrically, a non-concentrically worn sleeve bearing 200 with a sensor 205, where shaft 203 is closer to sensor 205 in one location than in another location. An air gap 222 is created by the removed material.

[0057] Looking now at FIG. 2A, FIG. 2A illustrates a sensor 205 for a sleeve bearing 200, comprising a race 201, a shaft 203, a sensor 205 and a wear liner 206. Sensor 205 comprises a conductive trace 208 sandwiched between a lower and upper layer of insulating substrate 209 which may be of differing thicknesses (FIG. 2B). When sensor 205 is laid flat (FIG. 2C), conductive trace 208 can be seen in detail, along with tabs 210 that extend from sleeve bearing 200. Slots 215 formed on sensor 205 assist in the flow of adhesive between layers. Electrode pads 213 are positioned on the surface of tabs 210 which can be probed with a capacitance meter to measure the capacitance between one electrode pad and shaft 203 (FIG. 2D).

[0058] Looking now at FIG. 3A, FIG. 3A illustrates a sensor 205 for a sleeve bearing 200, comprising a race 201, a shaft 203, a sensor 205 and a wear liner 206. Sensor 205 comprises a conductive trace 208 sandwiched between a lower layer of insulating substrate 209 and an upper layer of insulating substrate 214 (FIG. 3B). When sensor 205 is laid flat (FIG. 3C), conductive trace 208 can be seen in detail, along with tabs 210 that extend from sleeve bearing 200. Slots 215 formed on sensor 205 assist in the conformation of the sensor to surface variations, and to flow of adhesive between layers. Electrode pads 213 are positioned on the surface of tabs 210 which can be taken together as a connection point 220 for an antenna 221.

[0059] FIG. 4A illustrates a spherical bearing 200 comprising a race 201, a ball 202, a shaft 203, a sensor 205, a wear liner 206 and an insulator 207. Sensor 205 comprises a conductive trace 208 sandwiched between two layers of insulating substrate 209 (FIG. 4B). When sensor 205 is laid flat (FIG. 4C), conductive trace 208 can be seen in detail, along with tabs 210 that extend from sleeve bearing 200. Holes 211 formed on sensor 205 assist in the flow of adhesive between layers. Strain relief cuts 212 formed on sensor 205 enable sensor 205 to deform into a more conformal shape. Electrode pads 213 are positioned on the surface of tabs 210 for the interrogation of sensor 205 (FIG. 4D). Viewed end on, after installation, electrode pads 213 may be touched with one probe of a capacitance meter.

[0060] Looking now at FIGS. 5A and 5B, FIGS. 5A and 5B, illustrate a method of interrogating sensor 205. As shown in FIG. 5A, a probe 225 of a precision capacitance meter 230 makes contact with an electrode pad 213 on the circumference of spherical bearing 200. Assuming that race 201 and shaft 203 are both conductive and electrically connected elsewhere, the capacitance measured by the precision capacitance meter shall be comprised of the capacitance between ball 202 and sensor 205, which is electrically in series with the capacitance between sensor 205 and race 201.

[0061] FIG. 6A illustrates a spherical bearing 200 comprising a race 201, a ball 202, a shaft 203, a sensor 205, a wear liner 206 and an insulator 207. Sensor 205 comprises a conductive trace 208 sandwiched between two layers of insulating substrate 209 (FIG. 6B). When sensor 205 is laid flat (FIG. 6C), conductive trace 208 can be seen in detail, along with tabs 210 that extend from sleeve bearing 200. Holes 211 formed on sensor 205 assist in the flow of adhesive between layers. Strain relief cuts 212 formed on sensor 205 enable sensor 205 to deform into a more conformal shape. Electrode pads 213 are positioned on the surface of tabs 210 for the interrogation of the sensor (FIG. 4D). Viewed end on, after installation, tabs 210 and electrode pads 213 are connected at a point 220 to an antenna 221, which may be mounted on the face of race 201.

[0062] Looking now at FIGS. 7A and 7B, FIGS. 7A and 7B illustrate a method of interrogating sensor 205 wirelessly. A signal produced by a tracking generator 235 is coupled through a matching network 240 to a loop antenna 245, which interacts with sensor antenna 221, for measuring bearing wear remotely. The output frequency of tracking generator 235 is varied over time, and at one moment will match the frequency of the LC circuit created by the sensor's capacitance and the antenna's inductance. At that moment, a spectrum analyzer 250 will detect the resonance frequency. The shift in resonant frequency shift from the change in sensor capacitance will correspond to the reduction in the wear liner thickness. Preferably, sensor antenna 221 may be placed in a detent, which is a circumferential groove in bearing race 201.

[0063] FIG. 8A illustrates a new square telescoping bearing with a sensor inserted into the wear liner in accordance with the present invention.

[0064] FIG. 8B illustrates a worn square telescoping bearing with a sensor inserted into the wear liner in accordance with the present invention.

[0065] One illustrative procedure for producing a device according to the present invention is shown in FIGS. 9A-9C. In FIG. 9A, there is shown an insulating substrate 209 with a metallic coating 208. In FIG. 9B, a second layer of insulator 214 is applied to sandwich the electrode, which may be patterned. In FIG. 9C, at least one hole or a pattern is cut out, producing a sensor that can be inserted into a bearing. Holes in the sheet are expected to improve the bonding with the substrate.

[0066] Turning back to FIG. 8A, FIG. 8A is an end-view of a new, un-worn telescoping structure comprising an outer sleeve 201, an inner shaft 203 and a wear lining 206, which has been instrumented with a sensor 205 part-way through wear lining 206. In FIG. 8B, wear liner 206 has been worn, leaving an air gap 222 and a reduced lining thickness on one side. The capacitance of this system can be modeled as the sum of the four parallel plate capacitors. Capacitance in this system is equal to the product of the permittivity of free space ∈.sub.0, the dielectric constant ∈ and the area A divided by the distance d: C=∈∈.sub.0A/d.

[0067] Comparing FIG. 8A to FIG. 8B, the lining thickness on the sides is unchanged, but in FIG. 8B the upper and lower distances are changed. At the bottom, the thickness of wear lining 206 has been reduced by wear, and a corresponding air gap 222 has opened up above shaft 203 at the top. The upper capacitor will have a lower value than before as the distance between shaft 203 and sensor 205 is increased by air gap 222. The lower capacitor will have a much higher value than before, as it has a distance between shaft 203 and sensor 205 that is reduced by the same distance as air gap 222. The increase in capacitance for the lower capacitor will more than make up for the decrease in capacitance for the upper capacitor. This is clear because the function 1/d is nonlinear. It approaches infinity as the quantity ‘d’ gets small, and it approaches zero as ‘d’ gets large.

[0068] We note that a similar type of measurement could be made if the wear liner material was conductive, and the resistance was measured as a function of wear.

[0069] There are two methods to measure the capacitance of the sensor. The first is to measure the value directly with a probe and a capacitance meter. The other alternative is to measure the resonant frequency of the combination of the sensor's capacitance and the attached antenna's inductance. A similar measurement could be implemented using an inductive sensor and a distributed capacitor to create the resonant circuit.

[0070] The preceding examples should be construed as non-limiting, as other methods of implementing the sensor are possible. Also, other methods can be used to measure the wear in addition to capacitance, including inductance and resistance.

MODIFICATIONS OF THE PREFERRED EMBODIMENTS

[0071] It should be understood that many additional changes in the details, materials, steps and arrangements of parts, which have been herein described and illustrated in order to explain the nature of the present invention, may be made by those skilled in the art while still remaining within the principles and scope of the invention.