CN109858079B - Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model - Google Patents

Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model Download PDF

Info

Publication number
CN109858079B
CN109858079B CN201811586365.1A CN201811586365A CN109858079B CN 109858079 B CN109858079 B CN 109858079B CN 201811586365 A CN201811586365 A CN 201811586365A CN 109858079 B CN109858079 B CN 109858079B
Authority
CN
China
Prior art keywords
heat source
grinding
model
grinding wheel
cup
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201811586365.1A
Other languages
Chinese (zh)
Other versions
CN109858079A (en
Inventor
张慧博
李晓强
戴士杰
周润天
张帅
王小军
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hebei University of Technology
Original Assignee
Hebei University of Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hebei University of Technology filed Critical Hebei University of Technology
Priority to CN201811586365.1A priority Critical patent/CN109858079B/en
Publication of CN109858079A publication Critical patent/CN109858079A/en
Application granted granted Critical
Publication of CN109858079B publication Critical patent/CN109858079B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Constituent Portions Of Griding Lathes, Driving, Sensing And Control (AREA)
  • Polishing Bodies And Polishing Tools (AREA)

Abstract

The invention relates to a cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model, which comprises the following steps: the method comprises the following steps: setting grinding parameters before grinding, and measuring the grinding force of the cup-shaped grinding wheel during plane grinding by using a force sensor; step two: analyzing the research status quo of the grinding force distribution during the plane grinding of the cup-shaped grinding wheel and the characteristics during the material removal, and establishing a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction according to the corresponding relation of force and heat; step three: and establishing an analytical model and/or a numerical model of the temperature field based on the non-uniform heat source model in the second step, and substituting the planar grinding parameters of the cup-shaped grinding wheel to be predicted into the analytical model and/or the numerical analysis model to obtain corresponding predicted temperature. The method is suitable for temperature prediction by utilizing the cup-shaped grinding wheel to perform surface treatment and other grinding, and the predicted result is compared with the image result acquired by the high-definition thermal infrared imager to find that the result is accurate.

Description

Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model
Technical Field
The invention relates to the field of grinding in machine manufacturing, in particular to a cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model.
Background
Grinding is an effective method for improving surface quality and has wide application in the field of precision machining. Surface machining with cup-shaped grinding wheels is receiving increasing attention in this field because of its high efficiency and high grinding quality. There are many factors that affect the quality of the surface finish, and grinding temperature is one of them. High grinding temperatures can cause thermal damage to the workpiece surface, including burns and hot cracks. The studies currently made in this regard are:
[1] deng Chaohui, she Shuailong, yi Jun, et al, non-circular profile workpiece high speed grinding temperature prediction method based on variable heat source model CN 10 8151885A.
[2] Zheng Kan, meng Heng, liao Wenhe, etc. the method for predicting the grinding temperature of a brittle material by ultrasonic vibration assisted grinding CN 107133392A, all of which are methods for predicting the temperature of plane grinding of a special workpiece (brittle material, non-circular profile workpiece) by using a parallel grinding wheel, and at present, the method cannot theoretically provide more favorable support only by experimental monitoring aiming at the problems of plane grinding heat damage and the like of a cup-shaped grinding wheel. Therefore, finding an effective grinding temperature prediction method is an important approach to prevent problems such as grinding burn.
Disclosure of Invention
The invention provides a cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model for surface processing by utilizing a cup-shaped grinding wheel, aiming at solving the problems that the instantaneous high temperature causes heat damage to the surface of a workpiece during plane grinding, the temperature is difficult to monitor in real time and the like.
The technical scheme of the invention is as follows:
a cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model comprises the following steps:
the method comprises the following steps: setting grinding parameters before grinding, and measuring the grinding force of the cup-shaped grinding wheel during plane grinding by using a force sensor;
step two: analyzing the research status of the distribution of grinding force during the plane grinding of the cup-shaped grinding wheel and the characteristics during material removal, and establishing a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction according to the corresponding relation between force and heat;
step three: and establishing an analytical model and/or a numerical model of the temperature field based on the non-uniform heat source model in the second step, and substituting the planar grinding parameters of the cup-shaped grinding wheel to be predicted into the analytical model and/or the numerical analysis model to obtain corresponding predicted temperature.
The method for predicting the plane grinding temperature of the cup-shaped grinding wheel based on the non-uniform heat source model comprises the steps of providing a cutting heat source model and a friction heat source model,
if the cutting heat is distributed in cosine form on the front end face of the grinding wheel, the cutting heat Q cutting ·R w Expressed by equation (7):
Figure BDA0001919167180000011
wherein epsilon is the actual area contact coefficient; r is 1 And R 2 The outer diameter and the inner diameter of the grinding wheel are respectively; r w The heat distribution rate between the workpiece and the grinding wheel; q cutting Is the heat generated by the cutting force; phi is an angle; q. q.s 0 Is the heat flux density of the cross section at an angle of 0, thus obtaining q 0 Comprises the following steps:
Figure BDA0001919167180000021
then the cutting heat distribution q (φ) in the circumferential direction is expressed by the equation (9):
Figure BDA0001919167180000022
assuming that the cutting heat is distributed radially on the front end face of the grinding wheel in a chi-square manner, a chi-square function f (x) is expressed by the formula (10):
Figure BDA0001919167180000023
wherein c is 0 Taking a chi-square function with k =4, and symmetrically transforming the chi-square function into the following components:
Figure BDA0001919167180000024
the area S of the cross section when Φ =0 is:
Figure BDA0001919167180000025
according to the equal area principle, the method comprises the following steps:
Figure BDA0001919167180000026
thus obtaining c 0
Figure BDA0001919167180000027
Then the radial distribution q (r) of the cutting heat is expressed by the formula (15):
Figure BDA0001919167180000028
the cutting heat source model obtained by simultaneous circumferential and radial cutting heat formulas is expressed by formula (16):
Figure BDA0001919167180000029
the distribution of the friction heat source model is related to the distribution of friction force, and in the grinding process, the friction force generated by the relative motion of the end face of the grinding wheel and the workpiece in contact is uniformly distributed, so that the friction heat source model is the formula (17):
Figure BDA00019191671800000210
superposing the cutting heat source model and the friction heat source model to obtain a non-uniform heat source model q (r, phi), and expressing by a formula (18):
Figure BDA0001919167180000031
according to the method for predicting the plane grinding temperature of the cup-shaped grinding wheel based on the non-uniform heat source model, the construction process of the analytic model is as follows:
the method comprises the following steps of establishing an analytic model of a continuous surface heat source temperature field on an infinite workpiece:
Figure BDA0001919167180000032
wherein c is the specific heat capacity of the workpiece under the condition of constant pressure, J/(kg DEG C); rho is the material density, kg/m 3 (ii) a α is thermal diffusivity, m 2 S; q (r, phi) is the point heat source density, W/m 2 (ii) a X, Y, Z is a generalized coordinate system; v is the moving speed of the heat source, m/s; τ is time, in units of s; the thermal diffusivity α in equation (19) is expressed by equation (20):
Figure BDA0001919167180000033
then, a finite large heat conductor temperature field limited by boundary conditions is established, a mirror image heat source is supposed to symmetrically exist on the other side of the heat insulation surface, and the actual heat source and the mirror image heat source are respectively made of gamma i It is indicated that i =1 is an actual heat source, i =2 and 3 are mirror image heat sources:
Figure BDA0001919167180000034
where L is the distance between the mirror image heat source and the actual heat source, then the analytical model of the temperature field on the finite large plane is:
Figure BDA0001919167180000035
the cup-shaped grinding wheel plane grinding temperature prediction method based on the non-uniform heat source model comprises the following steps:
(1) Defining unit types and material parameters;
(2) Establishing a three-dimensional solid model of a workpiece;
(3) Generating a grid;
(4) Applying a convection boundary condition;
(5) Loading a non-uniform heat source model: defining the load step number as N, then establishing a local cylindrical coordinate system under a global Cartesian coordinate system, selecting nodes of a loading area, and then applying a non-uniform heat flow density load in the selected area;
the non-uniform heat flow density load is generated in the following way: editing the non-uniform heat source model by using a function editor in ANSYS, then storing, wherein the stored file name must have a func extension, then opening the stored file, exporting a heat source array in an array form, and then loading in the selected area;
(6) Solving: the solving process is a continuous cyclic process, the load is deleted after one solving, if the solving times N is less than N, the local cylindrical coordinate system is established in the step (5), and the cyclic loading is finished until the solving times N is more than or equal to N;
(7) And (4) processing a result: checking the result of the numerical model, if the result is correct, ending the temperature prediction, otherwise, adjusting or regenerating the grid and continuing applying boundary conditions such as convection and the like and the subsequent steps.
Compared with the prior art, the invention has the beneficial effects that:
(1) The previous prediction about the grinding temperature is based on experiments, which requires embedding a thermocouple in a workpiece, and the process is complicated, and damages can be caused to the workpiece, so that the method is not suitable for production practice. According to the method, when the non-uniform heat source model is established in the early stage, the grinding force and the rotating speed of the grinding wheel need to be collected, and then the grinding temperature is predicted according to the second step and the third step. When the method is actually used, a thermocouple does not need to be embedded in the workpiece, and the prediction method is simple and accurate.
(2) Based on the distribution of grinding force and the material removal characteristics during the plane grinding of the cup-shaped grinding wheel, the invention establishes a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction, and reasonably combines the shape of a heat source with the distribution of heat flux density. And a temperature field analytical model and a numerical model during the plane grinding of the cup-shaped grinding wheel are established based on the heat source model.
(3) When a numerical model (finite element model) is established, a loading mode of a moving function heat source is provided, so that the method can be suitable for the working process of grinding the cup-shaped grinding wheel.
(4) The existing detection of the grinding temperature aims at temperature prediction during plane grinding of a parallel grinding wheel, and no feasible method is available for predicting the temperature field of plane grinding of a cup-shaped grinding wheel. The influence of the temperature on the processing quality is more obvious when the cup-shaped grinding wheel is used for plane grinding, the invention mainly provides an effective method for grinding such as surface treatment by using the cup-shaped grinding wheel, and the prediction precision reaches about 8 percent through the comparison of the result predicted by the analytical model and the image result collected by the high-definition thermal infrared imager. Meanwhile, the temperature curve acquired by the K-type thermocouple and the temperature curve predicted by the numerical model have higher goodness of fit.
Drawings
FIG. 1 is a flow chart of the operation of the present invention.
FIG. 2 is a schematic diagram of grinding force isoparametric and temperature measurement.
Fig. 3 Matlab implementation of a non-uniform heat source model.
FIG. 4 is an analytical model of the planar grinding temperature field of the cup wheel.
FIG. 5 is a flow chart of numerical modeling (finite element analysis).
Figure 6 numerical model of the cup wheel plane grinding temperature field.
FIG. 7 shows the temperature field collected by the high-definition thermal infrared imager.
FIG. 8 is a comparison of the predicted results of the numerical model with the temperature curves collected at specific points by the thermocouples, wherein FIG. 8 (a) is a graph of the temperature at point A versus time; FIG. 8 (B) is a graph showing the temperature at the point B as a function of time; FIG. 8 (C) is a graph showing the temperature change with time at the point C.
In the figure: 1. a force sensor; 2. a cup-shaped grinding wheel; 3. a type K thermocouple; 4. a workpiece; 5. a test bed; 6. a high-definition thermal infrared imager; 7. a pressure transmitter; 8. a temperature transmitter; 9. a data acquisition card; 10. a computer;
Detailed Description
The invention is further described with reference to the following detailed description of embodiments in conjunction with the accompanying drawings.
The invention discloses a cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model, which specifically comprises the following steps of:
the method comprises the following steps: grinding parameters are set before grinding, and a force sensor is utilized to measure the grinding force during the plane grinding of the cup-shaped grinding wheel.
Step two: analyzing the current research situation of the grinding force distribution during the plane grinding of the cup-shaped grinding wheel and the characteristics during the material removal, and establishing a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction according to the corresponding relation between force and heat (wherein the grinding force distribution and the material removal characteristics during the plane grinding of the cup-shaped grinding wheel refer to the results of other researchers, such as:
[1]FUJIWARA T,TSUKAMOTO S,OHASHI K,et al.Study on Grinding Force Distribution on Cup Type Electroplated Diamond Wheel in Face Grinding of Cemented Carbide[J].Advanced Mat-erials Research,2014,1017(2014):9-14.
[2]LI X.Application of self-inhaling internal cooling wheel in vertical surface grinding[J].Chin-ese Journal of Mechanical Engineering,2014,27(1):86-91。
step three: and establishing an analytical model and/or a numerical model of the temperature field based on the non-uniform heat source model in the second step, and substituting the planar grinding parameters of the cup-shaped grinding wheel to be predicted into the analytical model and/or the numerical analysis model to obtain corresponding predicted temperature.
The temperature prediction method during the plane grinding of the cup-shaped grinding wheel based on the non-uniform heat source model comprises the following steps: setting grinding parameters before grinding, and acquiring grinding forces in three directions respectively marked as F by using force sensors arranged on a mechanical arm tail end execution device during grinding n 、F t And F v . The entire system used for the grinding force detection (see fig. 2) includes the forceThe device comprises a sensor 1, a cup-shaped grinding wheel 2, a test bed 5, a pressure transmitter 7 and a computer 10. When the cup wheel 2 starts to grind a workpiece 4 to be measured fixed on the test bed 5, the force sensor 1 installed between the cup wheel 2 and the mechanical arm transmits the measured potential difference to the pressure transmitter 7, and the pressure transmitter 7 converts the potential difference into a pressure value and transmits the pressure value to the computer to acquire the grinding force.
The temperature prediction method during the plane grinding of the cup-shaped grinding wheel based on the non-uniform heat source model comprises the following steps: dividing the grinding force measured in the first step into cutting force F c And frictional force F f Expressed by equation (1):
Figure BDA0001919167180000051
wherein μ is the coefficient of friction, F n As a vertical force, F t As the radial force, the instantaneous heat generation Q at the time of grinding can be obtained by the grinding force as formula (2):
Q=(F c +F f )v s =Q cutting +Q friction (2)
wherein Q cutting And Q friction The heat generated by the cutting force and friction force, and the heat distribution ratio R between the workpiece and the grinding wheel w Can be expressed as formula (3) according to a model of Hahn:
Figure BDA0001919167180000052
k in the formula w And k g The thermal conductivity of the workpiece and the grinding wheel, respectively, can be determined using equations (4) and (5), respectively:
k w =V f λ f +(1-V fm (4)
Figure BDA0001919167180000061
wherein V f Is the volume fraction of the fiber; lambda f 、λ m Thermal conductivity of the fiber and the epoxy resin respectively; x = λ rd The ratio of the thermal conductivity of the bonding agent to the thermal conductivity of the diamond; v d Is the volume fraction of the abrasive grains of the grinding wheel. The heat Q flowing into the surface of the workpiece can be obtained by the above formula w Comprises the following steps:
Q w =Q·R w =(Q cutting +Q friction )R w (6)
according to the relation between force and heat (power P), when the rotating speed v of the grinding wheel is s At a certain time, the distribution of grinding heat is the same as that of grinding force during the plane grinding of the cup-shaped grinding wheel. The non-uniform heat source model comprises a cutting heat source model and a friction heat source model.
The distribution of the cutting heat source model is related to the distribution of the cutting force, and since the material removal mainly occurs at the front end surface of the grinding wheel during the planar grinding of the cup-shaped grinding wheel and a large cutting force is generated in the central region in the advancing direction of the grinding wheel, the load of the abrasive grains is greater than that of the left and right ends of the grinding wheel. Therefore, if the cutting heat is distributed in cosine form on the front end face of the grinding wheel, the cutting heat Q cutting ·R w Expressed by equation (7):
Figure BDA0001919167180000062
wherein epsilon is the actual area contact coefficient; r is 1 And R 2 The outer diameter and the inner diameter of the grinding wheel are respectively, and phi is an angle; q. q.s 0 Is the heat flux density of the cross section at an angle of 0, thus obtaining q 0 Comprises the following steps:
Figure BDA0001919167180000063
then the cutting heat distribution q (φ) in the circumferential direction is expressed by the equation (9):
Figure BDA0001919167180000064
relatively large cutting forces are generated in the region of the radially leading edge of the grinding wheel, whereas relatively small cutting forces are generated in the region of the trailing edge of the grinding wheel. Therefore, assuming that the cutting heat is distributed radially in the front end face of the grinding wheel in a chi-square manner, the chi-square function f (x) is expressed by the formula (10):
Figure BDA0001919167180000065
wherein c is 0 K is a scale factor and k is a degree of freedom. Taking the k =4 chi-squared function and performing a symmetric transformation:
Figure BDA0001919167180000066
the area S of the cross section at Φ =0 is:
Figure BDA0001919167180000067
according to the equal area principle, the method comprises the following steps:
Figure BDA0001919167180000068
thus obtaining c 0
Figure BDA0001919167180000071
Then the radial distribution q (r) of the cutting heat is expressed by the formula (15):
Figure BDA0001919167180000072
the cutting heat source model obtained by simultaneous circumferential and radial cutting heat formulas is expressed by formula (16):
Figure BDA0001919167180000073
the distribution of the friction heat source model is related to the distribution of the friction force, and the friction force generated by the relative motion of the end face of the grinding wheel and the workpiece in contact is uniformly distributed in the grinding process, so the friction heat source model is the formula (17):
Figure BDA0001919167180000074
and (3) superposing the cutting heat source model and the friction heat source model to obtain a non-uniform heat source model q (r, phi) which is expressed by a formula (18):
Figure BDA0001919167180000075
according to the method for predicting the temperature during the plane grinding of the cup-shaped grinding wheel based on the non-uniform heat source model, the construction process of the analytic model is as follows:
the method comprises the following steps of establishing an analytic model of a continuous surface heat source temperature field as follows:
Figure BDA0001919167180000076
wherein c is the specific heat capacity of the workpiece under the condition of constant pressure, and J/(kg DEG C); rho is the material density, kg/m 3 (ii) a α is thermal diffusivity, m 2 S; q (r, phi) is the point heat source density (i.e. the above-mentioned non-uniform heat source model), W/m 2 (ii) a X, Y, Z is a generalized coordinate system, i.e. the temperature value can be known by randomly taking a point (X, Y, Z) on the surface of the workpiece; v is the moving speed of the heat source, m/s; τ is time, in units of s.
The thermal diffusivity, α, in the equation can be expressed by the following equation:
Figure BDA0001919167180000081
then establishing a bounded stripThe finite thermal conductor temperature field of the member limits is derived from an infinite workpiece, which is finite in nature, and the surface of the workpiece exposed to air can be approximated as an adiabatic surface. To solve the problem of heat transfer from a large, finite object, it can be assumed that a mirror image heat source is symmetrically present on the other side of the insulating surface. The actual heat source and the mirror image heat source are respectively made of gamma i (i =1 for the actual heat source, i =2 and 3 for the mirror image heat source) is expressed as:
Figure BDA0001919167180000082
wherein L is the distance between the mirror image heat source and the actual heat source, then the analytical model of the temperature field on the finite large plane is:
Figure BDA0001919167180000083
the numerical model (finite element analysis) is established by the following steps:
(1) Defining unit types and material parameters;
(2) Establishing a three-dimensional solid model of a workpiece;
(3) Generating a grid;
(4) Applying boundary conditions such as convection;
(5) Loading a non-uniform heat source model;
(6) Solving for
(7) And (6) processing the result.
The above finite element building process is characterized by step (5) compared with the existing finite element building process, in which the above non-uniform heat source model is introduced.
According to the invention, an analytic model and a numerical model of the temperature field can be simultaneously established, when both exist, the analytic model is verified by using the numerical model (the numerical model refers to finite element analysis), and grinding predicted temperatures obtained by the two are similar and can be used as final predicted temperatures to meet actual production requirements. The built non-uniform heat source model can be calculated in Matlab; the analytical model of the established temperature field can calculate the result in Mathcad; the established temperature field numerical model can be realized in computer-aided technologies such as finite elements.
In addition, a temperature field image to be predicted of the high-definition thermal infrared imager can be acquired, data acquired through experiments are compared with the prediction results of the analytic model and the numerical model, the result obtained by the prediction method is consistent with the experiment result, and the correctness of the analytic model and the numerical model established by the method is further verified. And a K-type thermocouple can be used for collecting the temperature of a position on the surface of the workpiece, which is easy to burn, and the accuracy of the model is verified through an experimental curve and a prediction curve in a numerical model. The device (see figure 2) used in the temperature measurement experiment comprises a K-type thermocouple 3, a workpiece 4, a test bed 5, a high-definition thermal infrared imager 6, a temperature transmitter 8, a data acquisition card 9 and a computer 10; embedding a K-type thermocouple 3 in a workpiece 4 before grinding (see A, B and C positions in FIG. 2), and fixing the workpiece 4 on a test bench 5; and simultaneously, the high-definition thermal infrared imager is arranged beside the grinding experiment. In the grinding process, the K-type thermocouple 3 transmits the collected potential difference to the temperature transmitter 8, the temperature transmitter 8 converts the potential difference into a temperature signal, and the temperature signal is collected and sent to a computer 10 for analysis through a data acquisition card 9; and at the moment of finishing the grinding and retracting, the high-definition thermal infrared imager 6 transmits the acquired temperature field image to the computer 10 for analysis. The high-definition thermal infrared imager can acquire the whole grinding temperature field of the surface of the workpiece and can be used for verifying the accuracy of an analytical model and a numerical model of the temperature field; the thermocouple can obtain a change curve of the temperature of a special point along with time, the accuracy of the model can be verified through a prediction curve and an experimental curve, the high-definition thermal infrared imager is expensive in temperature collection and high in cost, and the collected temperature field image is visual and comprehensive; the thermocouple acquisition cost is low, but only a temperature curve of a certain point can be obtained, and the distribution of the whole grinding temperature field cannot be obtained.
Example 1
The material processed by the embodiment is a composite material, and due to the particularity of the composite material, instantaneous heat aggregation phenomenon can be formed by the heat which is sharply increased when the cup-shaped grinding wheel is used for plane grinding, so that the highest temperature of an instantaneous contact point in a grinding area can reach the melting point temperature of a workpiece material, resin softening and strength reduction are easily caused, the bonding capability to carbon fibers is reduced, and surface groove marks are finally formed. Therefore, the cup-shaped grinding wheel plane grinding temperature prediction method based on the non-uniform heat source model is provided for solving the problems of difficulty in real-time temperature detection and the like in the grinding process. As shown in fig. 1, the method specifically includes the following steps.
The method comprises the following steps: measuring the grinding force of the cup-shaped grinding wheel 2 during plane grinding by using a six-dimensional force sensor, and collecting the rotating speed v of the grinding wheel when the grinding wheel is stable s (ii) a The workpiece 4 to be tested is fixed on the test bed 5, and the force sensor 1 is installed at the tail end of the mechanical arm and connected with the pressure transmitter 7 to transmit data to the computer 10 for analysis. The following table 1 sets the grinding parameters prior to machining:
TABLE 1 determination of grinding parameters
Figure BDA0001919167180000091
The force during grinding is obtained by the force sensor 1 as follows:
Figure BDA0001919167180000092
step two: analyzing the research status quo of the grinding force distribution during the plane grinding of the cup-shaped grinding wheel and the characteristics during the material removal, and establishing a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction according to the relationship between force and heat pair; dividing the grinding force measured in the first step into a cutting force and a friction force, and expressing the cutting force and the friction force as follows:
Figure BDA0001919167180000093
where μ is the coefficient of friction. The instantaneous heating value during grinding can be obtained by the grinding force as follows:
Q=(F c +F f )v s =Q cutting +Q friction
wherein Q cutting And Q friction The heat generated by the cutting force and friction force, and the heat distribution ratio R between the workpiece and the grinding wheel w The model according to Hahn can be expressed as:
Figure BDA0001919167180000094
k in the formula w And k g The thermal conductivity coefficients of the workpiece and the grinding wheel are obtained by the following formula:
k w =V f λ f +(1-V fm
Figure BDA0001919167180000101
wherein V f Is the volume fraction of the fiber; lambda [ alpha ] f 、λ m Thermal conductivity of the fiber and the epoxy resin respectively; x = λ rd The ratio of the thermal conductivity of the binding agent to the thermal conductivity of the diamond; v d Is the volume fraction of the abrasive grains of the grinding wheel. The heat flowing into the surface of the workpiece can be obtained by the following formula:
Q w =Q·R w =(Q cutting +Q friction )R w
according to the relation between force and heat (power P), when the rotating speed v of the grinding wheel is s At a certain time, the distribution of grinding heat is the same as that of grinding force during the plane grinding of the cup-shaped grinding wheel. The non-uniform heat source model comprises a cutting heat source model and a friction heat source model.
The distribution of the cutting heat source model is related to the distribution of the cutting force, and since the material removal mainly occurs at the front end surface of the grinding wheel during the planar grinding of the cup-shaped grinding wheel and a large cutting force is generated in the central region in the advancing direction of the grinding wheel, the load of the abrasive grains is greater than that of the left and right ends of the grinding wheel. Therefore, the cutting heat is assumed to be distributed in a cosine form on the front end face of the grinding wheel:
Figure BDA0001919167180000102
wherein epsilon is the actual area contact coefficient; r 1 And R 2 Respectively the outer diameter and the inner diameter of the grinding wheel, thus obtaining q 0 Comprises the following steps:
Figure BDA0001919167180000103
the cutting heat is then distributed circumferentially as:
Figure BDA0001919167180000104
relatively large cutting forces are generated in the region of the radially leading edge of the grinding wheel, whereas relatively small cutting forces are generated in the region of the trailing edge of the grinding wheel. Therefore, assuming that the cutting heat is radially distributed in a chi-square manner on the front end surface of the grinding wheel, the chi-square function is as follows:
Figure BDA0001919167180000105
wherein c is 0 Is the proportionality coefficient and k is the degree of freedom. Taking a chi-square function with k =4, the symmetric transformation is:
Figure BDA0001919167180000106
the area S of the cross section when Φ =0 is:
Figure BDA0001919167180000107
according to the equal area principle, the method comprises the following steps:
Figure BDA0001919167180000108
thus obtaining c 0
Figure BDA0001919167180000111
The cutting heat is then distributed in the radial direction:
Figure BDA0001919167180000112
the circumferential and radial equations of simultaneous cutting heat are modeled as follows:
Figure BDA0001919167180000113
Figure BDA0001919167180000114
the distribution of the friction heat source model is related to the distribution of the friction force, and in the grinding process, the contact relative motion of the end face of the grinding wheel and the workpiece generates friction, so that the distribution model of the friction heat source is as follows:
Figure BDA0001919167180000115
superposing the cutting heat source model and the friction heat source model to obtain a non-uniform heat source model as follows:
Figure BDA0001919167180000116
the reference material yields the following parameters:
(a) Carbon fiber composite material workpiece
(1) Density: ρ =1.572g/cm 3
(2) Specific heat capacity at constant pressure: c = 802.84J/(kg. Degree. C)
(3) Volume fraction of carbon fiber: v f =0.6
(4) Thermal conductivity of carbon fiber: lambda f =0.50~1.10W/(m·K)
(5) Thermal conductivity of epoxy resin: lambda [ alpha ] m =0.20~0.80W/(m·K)
(b) Type B cup grinding wheel (D75T 25H20W10X 3)
(1) Thermal conductivity of resin binder: lambda [ alpha ] r =0.9W/(m·K)
(2) Thermal conductivity of diamond abrasive grains: lambda d =146W/(m·K)
(3) Volume fraction of diamond: v d =0.7
(4) Coefficient of friction: μ =0.3
The non-uniform heat source model is drawn in Matlab, and when the cup-shaped grinding wheel plane grinding is realized, the non-uniform heat source model is shown in FIG. 3.
Step three: establishing an analytical model of the temperature field based on the non-uniform heat source model in the step two, and verifying the model by using a numerical model (finite element analysis);
establishing an analytical model for plane grinding of a cup-shaped grinding wheel;
and (II) establishing a numerical model (finite element analysis) of the cup-shaped grinding wheel plane grinding.
Establishing an analytical model of cup-shaped grinding wheel plane grinding in the third step (I), specifically comprising the following steps of establishing an analytical model of a continuous surface heat source temperature field:
Figure BDA0001919167180000121
wherein c is the specific heat capacity of the workpiece under the condition of constant pressure, J/(kg DEG C); rho is the material density, kg/m 3 (ii) a α is thermal diffusivity, m 2 S; q (r, phi) is the point heat source density, W/m 2 (ii) a v is the moving speed of the heat source, m/s; τ is time, s. The thermal diffusivity, α, in the equation can be expressed by the following equation:
Figure BDA0001919167180000122
then, a finite thermal conductor temperature field limited by the boundary conditions is established, the above derivation being carried out on an infinite workpiece, whereas in practice the workpiece is finite and the surface of the workpiece exposed to air can be approximately seen as the adiabatic surface. To solve the problem of heat transfer from a large, finite object, it can be assumed that a mirror image heat source is symmetrically present on the other side of the insulating surface. The actual heat source and the mirror image heat source are respectively made of gamma i Expressed as:
Figure BDA0001919167180000123
i=1,2,3;Y 1 =Y,Y 2 =Y-L,Y 3 =Y+L;Z=0
the analytical model of the temperature field over a finite large plane is then:
Figure BDA0001919167180000124
the analytical model of the temperature field is calculated in MathCAD to obtain the temperature field distribution shown in figure 4;
establishing a numerical model (finite element analysis) of the cup-shaped grinding wheel plane grinding in the step three (II), programming by using an APDL language in ANSYS software, and specifically, the flow is shown in FIG. 5:
(1) Defining unit types and material parameters;
according to example calculation data of a grinding temperature field, three-dimensional transient heat transfer analysis is carried out by using SOLID70 unit in ANSYS, the processed material is a composite material, and material parameters mainly comprise density rho and heat conductivity coefficient k w And the specific heat capacity c under the constant pressure condition, wherein the numerical value of the specific heat capacity c is based on the material parameters given in the second step.
(2) Establishing a three-dimensional solid model of a workpiece;
in the embodiment, the shape of the workpiece is simple, and the parameterized modeling is simple, quick and efficient. The workpiece dimensions were (length × width × height): 0.3 m.times.0.15 m.times.0.015 m
(3) Generating a grid;
the division of the mesh in the three-dimensional transient model directly affects the accuracy of the simulation. Too small a mesh size may result in too long a simulation time and even a breakdown, while too large a mesh size may result in reduced accuracy of the results. In order to optimize the simulation process, a grid with a larger size is adopted on one side far away from the grinding surface, and the grid on one side far away from the grinding surface in the modeling is set to be 0.5mm; and the grinding contact surface adopts a grid with higher precision, and the grid of the contact surface in the modeling is set to be 0.2mm.
(4) Applying boundary conditions such as convection;
the boundary conditions in this experiment are mainly illustrated by: initial temperature and convective heat transfer coefficient of air.
Setting the initial temperature value as T 0 =20 ℃, and the convective heat transfer coefficient of air is h = 20W/(m) 2 ·K)。
(5) Loading a non-uniform heat source model;
the loading of the non-uniform heat source model specifically comprises the steps of starting a starting cycle subroutine (namely a loading procedure), firstly defining the load step number as N in the subroutine, secondly establishing a local cylindrical coordinate system under a global Cartesian coordinate system, selecting nodes of a loading area, and then applying a non-uniform heat flow density load in the selected area, wherein the non-uniform heat flow density load is generated in the following mode: and editing and storing the non-uniform heat source model by using a function editor in ANSYS, wherein the stored file name must have a func extension, opening the stored file, exporting a heat source array in an array form, and then loading in the selected area. The specific loading method is shown in fig. 5.
(6) Solving;
and (4) the solving process is a continuous cyclic process, the load is deleted after one solving, if the solving times N is less than N, the steps of establishing the local cylindrical coordinate system and the subsequent steps in the step (5) are repeated until the solving times N is more than or equal to N, and the cyclic subprogram is ended.
(7) And (6) processing the result.
The numerical model results are examined using a post-processing module. If the result is correct, the temperature prediction is finished, otherwise, boundary conditions such as convection and the like and the following steps are continuously applied after the grid is adjusted and regenerated.
And (3) utilizing an APDL (android package) parameterized language to model a numerical model. The numerical model of the temperature field of this example is shown in fig. 6.
And acquiring and comparing the temperature field image by using a high-definition thermal infrared imager. And the high-definition thermal infrared imager 6 in the figure 1 transmits the collected temperature field model to a computer 10 for analyzing and verifying the accuracy of the analytical model and the numerical model of the temperature field during the planar grinding of the cup-shaped grinding wheel, and finally the aim of predicting the grinding temperature is fulfilled. The temperature field collected by the thermal imager is shown in fig. 7, the measured values of the four marked points in fig. 7 are compared with the predicted value of the analytical model in fig. 4, and the prediction accuracy of the grinding temperature reaches about 8 percent as shown in table 2.
TABLE 2 comparison of predicted values with Experimental values
Figure BDA0001919167180000131
Temperature acquisition is carried out at three positions A, B and C on the surface of the workpiece 4 by using the K-type thermocouple 3 as shown in FIG. 6, and the acquired data is transmitted to a computer 10 through a temperature transmitter 8 and a data acquisition card 9 to be analyzed: the result predicted by the numerical model has better goodness of fit with the temperature curve of the experimental result, as shown in fig. 8.
Nothing in this specification is said to apply to the prior art.

Claims (3)

1. A cup-shaped grinding wheel plane grinding temperature prediction method based on a non-uniform heat source model comprises the following steps:
the method comprises the following steps: setting grinding parameters before grinding, and measuring the grinding force of the cup-shaped grinding wheel during plane grinding by using a force sensor;
step two: analyzing the research status quo of the grinding force distribution during the plane grinding of the cup-shaped grinding wheel and the characteristics during the material removal, and establishing a non-uniform heat source model which is distributed in different functions in the circumferential direction and the radial direction according to the corresponding relation of force and heat;
step three: establishing an analytical model and/or a numerical model of a temperature field based on the non-uniform heat source model in the second step, and substituting the planar grinding parameters of the cup-shaped grinding wheel to be predicted into the analytical model and/or the numerical analysis model to obtain corresponding predicted temperature;
the non-uniform heat source model comprises a cutting heat source model and a friction heat source model,
if the cutting heat is distributed in cosine form on the front end face of the grinding wheel, the cutting heat Q cutting ·R w Expressed by equation (7):
Figure FDA0003813421740000011
wherein epsilon is the actual area contact coefficient; r is 1 And R 2 The outer diameter and the inner diameter of the grinding wheel are respectively; r w The heat distribution rate between the workpiece and the grinding wheel; q cutting Is the heat generated by the cutting force; is more than an angle; q. q.s 0 Is the heat flux density of the cross section at an angle of 0, thus obtaining q 0 Comprises the following steps:
Figure FDA0003813421740000012
then the cutting heat distribution q (φ) in the circumferential direction is expressed by the equation (9):
Figure FDA0003813421740000013
assuming that the cutting heat is distributed radially on the front end face of the grinding wheel in a chi-square manner, a chi-square function f (x) is expressed by the formula (10):
Figure FDA0003813421740000014
wherein c is 0 Taking a chi-square function of k =4 as a proportionality coefficient and k is a degree of freedomThe symmetry transformation is:
Figure FDA0003813421740000015
the area S of the cross section at Φ =0 is:
Figure FDA0003813421740000016
according to the equal area principle, the method comprises the following steps:
Figure FDA0003813421740000017
thus obtaining c 0
Figure FDA0003813421740000021
Then the radial distribution q (r) of the cutting heat is expressed by the formula (15):
Figure FDA0003813421740000022
the simultaneous circumferential and radial cutting heat equations to obtain the cutting heat source model are expressed by equation (16):
Figure FDA0003813421740000023
the distribution of the friction heat source model is related to the distribution of friction force, and in the grinding process, the friction force generated by the relative motion of the end face of the grinding wheel and the workpiece in contact is uniformly distributed, so that the friction heat source model is the formula (17):
Figure FDA0003813421740000024
wherein Q is friction Heat generated by friction work;
and (3) superposing the cutting heat source model and the friction heat source model to obtain a non-uniform heat source model q (r, phi), and expressing by a formula (18):
Figure FDA0003813421740000025
2. the method for predicting the plane grinding temperature of the cup-shaped grinding wheel based on the non-uniform heat source model according to claim 1, wherein the analytical model is constructed by the following steps:
the method comprises the following steps of establishing an analytic model of a continuous surface heat source temperature field on an infinite workpiece:
Figure FDA0003813421740000026
wherein c is the specific heat capacity of the workpiece under the condition of constant pressure, J/(kg DEG C); rho is the material density, kg/m 3 (ii) a α is thermal diffusivity, m 2 S; q (r, phi) is the point heat source density, W/m 2 (ii) a X, Y, Z is a generalized coordinate system; v is the moving speed of the heat source, m/s; τ is time, in units of s; the thermal diffusivity in the formula is represented by formula (20):
Figure FDA0003813421740000031
then, a finite large heat conductor temperature field limited by boundary conditions is established, a mirror image heat source is supposed to symmetrically exist on the other side of the heat insulation surface, and the actual heat source and the mirror image heat source are respectively made of gamma i Indicating that i =1 is the actual heat source, i =2 and 3 are mirror image heat sources:
Figure FDA0003813421740000032
where L is the distance between the mirror image heat source and the actual heat source, then the analytical model of the temperature field on the finite large plane is:
Figure FDA0003813421740000033
3. the method for predicting the plane grinding temperature of the cup-shaped grinding wheel based on the non-uniform heat source model as claimed in claim 1, wherein the numerical model is established by the following steps:
(1) Defining unit types and material parameters;
(2) Establishing a three-dimensional solid model of a workpiece;
(3) Generating a grid;
(4) Applying a convection boundary condition;
(5) Loading a non-uniform heat source model: defining the load step number as N, then establishing a local cylindrical coordinate system under a global Cartesian coordinate system, selecting nodes of a loading area, and then applying a non-uniform heat flow density load in the selected area;
the non-uniform heat flow density load is generated in the following way: the method comprises the steps that a function editor in ANSYS is used for editing and storing a non-uniform heat source model, a stored file name must have a func extension, then a stored file is opened, a heat source array in an array form is exported and generated, and then the heat source array is loaded in a selected area;
(6) Solving: the solving process is a continuous cyclic process, the load is deleted after one solving, if the solving times N is less than N, the local cylindrical coordinate system is established in the step (5), and the cyclic loading is finished until the solving times N is more than or equal to N;
(7) And (4) processing results: checking the numerical model result, if the result is correct, ending the temperature prediction, otherwise, adjusting or regenerating the grid and continuing to apply the convection boundary condition and the subsequent steps.
CN201811586365.1A 2018-12-25 2018-12-25 Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model Active CN109858079B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201811586365.1A CN109858079B (en) 2018-12-25 2018-12-25 Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201811586365.1A CN109858079B (en) 2018-12-25 2018-12-25 Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model

Publications (2)

Publication Number Publication Date
CN109858079A CN109858079A (en) 2019-06-07
CN109858079B true CN109858079B (en) 2022-10-04

Family

ID=66892130

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201811586365.1A Active CN109858079B (en) 2018-12-25 2018-12-25 Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model

Country Status (1)

Country Link
CN (1) CN109858079B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112861337B (en) * 2021-02-01 2024-04-30 中国科学院宁波材料技术与工程研究所 Surface temperature prediction method for heated carbon fiber heating wire

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN203156587U (en) * 2013-01-25 2013-08-28 河南富耐克超硬材料股份有限公司 Cup-shaped grinding wheel
CN108151885A (en) * 2017-12-15 2018-06-12 湖南科技大学 Non-circular profile Work piece high-speed grinding temperature Forecasting Methodology based on variable heat source model

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN203156587U (en) * 2013-01-25 2013-08-28 河南富耐克超硬材料股份有限公司 Cup-shaped grinding wheel
CN108151885A (en) * 2017-12-15 2018-06-12 湖南科技大学 Non-circular profile Work piece high-speed grinding temperature Forecasting Methodology based on variable heat source model

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
大平面砂轮磨齿的温升分析;李国龙等;《重庆大学学报》;20140915(第08期);全文 *
杯形砂轮平面磨削温度场的有限元分析;田晓等;《精密制造与自动化》;20040525(第02期);全文 *
高硬度涂层磨削温度场的数值仿真和实验研究;许黎明等;《上海交通大学学报》;20111115(第11期);全文 *

Also Published As

Publication number Publication date
CN109858079A (en) 2019-06-07

Similar Documents

Publication Publication Date Title
Sato et al. Temperature variation in the cutting tool in end milling
Richardson et al. Modelling of cutting induced workpiece temperatures for dry milling
Cui et al. An investigation of tool temperature in end milling considering the flank wear effect
CN104268343A (en) Method of cutting force prediction and temperature prediction for end-milling cutting
CN101804581A (en) Implementation method of automatic compensation for thermal deformation of machine tool
Holtermann et al. Modelling, simulation and experimental investigation of chip formation in internal traverse grinding
CN108151885A (en) Non-circular profile Work piece high-speed grinding temperature Forecasting Methodology based on variable heat source model
CN108188821B (en) A kind of Ball-screw in NC Machine Tools feed system Thermal Error prediction technique
Yi et al. The temperature field study on the three-dimensional surface moving heat source model in involute gear form grinding
Al Huda et al. Investigation of temperature at tool-chip interface in turning using two-color pyrometer
CN105328511A (en) Cutting online-temperature collecting method used for porous material
CN109858079B (en) Cup-shaped grinding wheel plane grinding temperature prediction method based on non-uniform heat source model
Cui et al. Analysis of transient average tool temperatures in face milling
CN113297761B (en) Thermal deformation test compensation method for numerical control machine tool
Huang et al. Utilization of heat quantity to model thermal errors of machine tool spindle
CN113688534A (en) Research method for searching optimal milling parameter based on multi-feature fusion model
Ding et al. Investigation of the grinding temperature and energy partition during cylindrical grinding
Dai et al. Research on temperature field of non-uniform heat source model in surface grinding by cup wheel
CN103639895A (en) Grinding temperature measurement method based on heat transferring inverse problem
Yu et al. Toward the temperature distribution on ball bearing inner rings during single-grit grinding
CN105058163B (en) Thermal Error measurement apparatus and measuring method during gear grinding machines working condition
CN101908084B (en) Method for reconstructing temperature field of 1000MW supercritical turbo rotor groove face
Kukiełka Numerical simulations of the thread rolling process as ecological and economical research tool in the implementation of modern technologies
CN106289842B (en) A kind of numerical control machine heat Modal Parameters Identification
Arunaganesan et al. Data acquisition system based on 8051 microcontroller for cutting tool temperature measurement

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant