Strojniški vestnik - Journal of Mechanical Engineering 61(2015)5, 303-310 © 2015 Journal of Mechanical Engineering. All rights reserved. D0l:10.5545/sv-jme.2014.2340 Original Scientific Paper Received for review: 2014-11-25 Received revised form: 2015-03-05 Accepted for publication: 2015-03-19 Numerical Calculation of Tooth Profile of a Non-circular Curved Face Gear Chao Lin* - Dong Zeng - Xianglu Zhao - Xijun Cao Chongqing University, The State Key Laboratory of Mechanical Transmission, China Based on the cylindrical coordinates and the space engagement theory, which utilize a cylindrical coordinate system, an arbitrary curve equation was obtained and a method of curve expansion was established. This allows any order of pitch curve of non-circular curved face gear and normal equidistant curve parameter equations to be derived. The tooth profile points of the non-circular curved face gear can be solved using the numerical calculation method where the tooth profile intersects with the pitch curve and normal equidistant curves of non-circular curved face gear. Finally the numerical method used to solve the tooth profile of the non-circular curved face gear was proved to be accurate and correct from the small error between measured data and the data of theoretical calculation. Keywords: non-circular curved face gear, cylindrical coordinates, pitch curve, numerical calculation of tooth profile, error analysis Highlights • Built a mathematical model and a expansion method of an arbitrary curve. • Derived equations of the pitch curve and the normal equidistant curves of the non-circular curved face gear. • Proposed a numerical method to calculate the tooth profile. • Measured the tooth profile and analyzed the error of the tooth profile to verify the numerical method. 0 INTRODUCTION The non-circular curved face gear drive is also called the orthogonal variable transmission ratio face gear drive. It is generated by replacing the spur pinion and its conjugated face gear of a conventional face gear drive by a non-circular gear and its conjugated face gear [1]. The transmission ratio is variable when the non-circular curved face gear engages with non-circular gear, since the teeth distributed on the cylindrical surface. This is the most significant feature compared to the conventional face gear. This type of gear drive has many possible applications in the field of engineering, textile, agriculture, etc. In 1940, Buckingham came up with the concept of the face gear in the paper [2], which he defined as a rack of changing tooth pitch and pressure angles; Litvin and his team made a strong contribution to the research about face gears on the basis of their predecessors' research. His book [3] gave in-depth research about the surface of the face gear in terms of the gear geometry and meshing principle; Ji et al and Zhu et al. did a lot of research on face gears in the field of tooth surface contact analysis, strength, coincidence degree theory, etc. [4]; Lin et al. were the first to propose a non-circular curved face gear and explored its tooth profile analysis, machining simulation, measurement, etc. and this study made significant achievements. To date there has been little research about the tooth profile of non-circular curved face gears [5] and [6]. The error of the tooth profile will not only impact on the instantaneous transmission accuracy but also cause plastic deformation on the tooth surface of intermeshing gear. There exist some methods for using the numerical method to solve the gear tooth profile, for instance, Xia et al., Li et al. and Tong et al. calculated the tooth profile of a bevel gear using the numerical method which was based on the spherical coordinates [7] to [9]. In the field of gear measurement, Guenther et al. and Zhang et al. put forward some new theories and methods of measuring and analyzing gears [10] to [12]. But, at present, there is no practical way of using the numerical method to solve the tooth profile of non-circular curved face gear. This paper presents a new general numerical method used to calculate the tooth profile of a non-circular curved face gear. This method will serve as an important reference basis in the field of modeling, processing, analyzing errors of measurement, and so forth. 1 PARAMETERS OF THE CURVE IN THE CYLINDRICAL COORDINATE SYSTEM The non-circular curved face gear is a kind of cylindrical gear. In order to describe and calculate the parameters of the gear more accurately, this paper prepared a study of the angle and the expansion of the curve under the cylindrical coordinate system. *Corr. Author's Address: Chongqing University, The State Key Laboratory of Mechanical Transmission, Shapingba District sand 174 Center Street, Chongqing, China, linchao@cqu.edu.cn 303 Strojniski vestnik - Journal of Mechanical Engineering 61(2015)5, 303-310 Fig. 1. Parameters of the curve in the cylindrical coordinate system As shown in Fig. 1, O —XYZ is the cylindrical coordinate system, r is one curve on the cylindrical surface, Mand N are any two points on the curve. 9 is the rotation angle which is from the positive X axis to the point. h is the distance between the point and the bottom surface, y is the central angle of the point on the curve, R is the cylindrical radius. 1.1 Basic Description of the Curve Assume that the equation of any curve is: r = ( cos0 R sin0 h (0). The arc length between points M and N is: Lm = J?VR 2 + h'2 (0) (1) (2) where h'(9) is the derivative of h(9). The central angle of one point on the curve can be defined as the angle between the line which links that point to the center of the circle in the bottom surface and the bottom surface. According to the geometric relationship the formula is: h (0) Y = arctan - 1.2 Expansion of the Curve R (3) The line linking all points on the curve to the center of the circle in the bottom surface will compose a conical surface. As shown in Fig. 1, there are countless tangent planes through point N. However, there exists a unique tangent plane that is vertical to the Z axis. There exists one point K on the line intersected by the tangent plane and the cylindrical surface where LM = LN . At the same time the plane OKN is an MN NK * expansion of the plane OMN. To solve Eq. (2), we get: L- = L- = {e\lR2 + h'2 (0) d0. (4) NK MM J0] V V ) v ' Thus the expansion angle fi corresponding to the curve MN is: B = . 1 - f\/R2 + h'2 (0) dd. (5) yjR2 + h2 (0) J°i V 2 PITCH CURVE OF THE NON-CIRCULAR CURVED FACE GEAR 2.1 Equation of the Pitch Curve According to the meshing relationship of the non-circular curved face gear pair, a coordinate system can be established. 2 ' h ) Fig. 2. Meshing coordinate of the non-circular curved face gear As shown in Fig. 2, the axis of the non-circular gear is orthogonal to axis of the non-circular curved face gear. As shown in Fig. 2, O1 -X1Y1Z1 is the fixed coordinate system of the non-circular gear. O2-X2Y2Z2 is the fixed coordinate system of the non-circular curved face gear. The point P is on the pitch curve of non-circular gear and the point P2 is on the pitch curve of non-circular curved face gear. When Pi coincides with P2, the non-circular gear turns at an angle of ^ , and the non-circular curved face gear turns at an angle of £,2 . The radius of the pitch curve of the non-circular curved face gear is R, and the radius vector of the non-circular gear is r(^1) . Under the conditions of Fig. 2, the distance between the axis of the non-circular gear and the bottom surface of Y 304 Lin, C. - Zeng, D. - Zhao, X. - Cao, X. Strojniski vestnik - Journal of Mechanical Engineering 61(2015)5, 303-310 the face gear is E. I is the pitch curve of non-circular curved face gear. According to the theory of non-circular gears, the equation for the pitch curve of the non-circular gear is: ) = - e*) 1 - e cos (n1E,1)' (6) where, £ is the polar angle of the elliptic gear, a is half of the longer axis of the ellipse, e is the eccentricity of the ellipse, n1 is the order of the non-circular gear. When the parameters in Eq. (6) were chosen as follows: a = 35 mm, e = 0.1 and n1 changes from 1 to 4. The pitch curve of the non-circular gear can be shown in Fig. 3. n1 is the order of the non-circular gear, n2 is the order of non-circular curved face gear, i12 is the transmission ratio of the non-circular curved face gear pair and i12= R / r(£). By substituting the equations above into Eq. (8), the pitch curve of the non-circular curved face gear can be obtained. cos y ^-^sin 2n ^ Í; 2 ^ Í; 2n 2n = h (Í2 ) = E - r (£) (9) n 2 x r. 2.2 Tooth Modulus Angle of the Pitch Curve Plane As shown in Fig. 4, based on the method of the expansion of the curve, tooth 1 and tooth 2 represent any 2 teeth on the pitch curve of the non-circular curved face gear. Point M and point N are the points on the right tooth profile of tooth 1 and tooth 2. There is a complete tooth profile between M and N. By expanding the tooth profile on the tangential circle of the pitch curve, the point K on the tangential circle can be_obtained. When the arc length of MN is equal to KN, the plane OKN is the expansion plane of the one tooth profile. In the meshing process of the non-circular gear and non-circular curved face gear, the center distance is fixed. From the geometric relationship shown in Fig. 2, Eq. (7) is correct at any point in time. E = h (¿2) + r (¿¿) = a + ae, (7) where, h(£2) is the distance between the point on the pitch curve and the bottom surface when the non-circular face gear turns an angle £2. By substituting Eq. (6) and Eq. (7) into Eq. (1), the pitch curve of the non-circular curved face gear can be obtained. x = R cos^2 y = R sin ^2 , = h ) = E - r ) (8) where, *=¿ i»-1 ;=j: f ;^ i;' m Tangential circle Pitch curve R ■ Fig. 4. Tooth modulus angle of the non-circular curved face gear When the angle ft = nftm , ftm is the modulus angle of the tooth. The tooth profile of the non-circular curved face gear changes when the direction of the tooth width changes and so does the modulus angle. Numerical Calculation of Tooth Profile of a Non-circular Curved Face Gear 305 r 2 12 Strojniski vestnik - Journal of Mechanical Engineering 61(2015)5, 303-310 2.3 Addendum Angle and Dedendum Angle As shown in Fig. 5, the addendum line, pitch curve and dedendum line of the non-circular curved face gear are on the cylindrical surface n. The tangential plane through the center point O of the bottom surface intersects with the addendum line, pitch curve and dedendum line at points M, P and N. MN is the tangent section on the cylindrical surface. Angles MOP and PON are defined as the addendum angle and the dedendum angle. And, \af = a = hh • ß a a rm (+ c) (10) where, h*a is the addendum coefficient, c* is the dedendum coefficient. pm is the modulus angle. So the addendum and dedendum of the non-circular curved face gear are: \ha = R tan (y + aa )• h (ç2 ) \hf = Rtan( -af )• h(Ç2)' (11) where, y is the center angle, R is the radius of the pitch curve of non-circular curved face gear, aa is the addendum angle of non-circular curved face gear, and Of is the dedendum angle of non-circular curved face gear. Fig. 5. Addendum angle and dedendum angle (1 addendum line, 2 pitch curve, and 3 dedendum line) 3 USING THE NUMERICAL METHOD TO SOLVE TOOTH PROFILE The fundamental theory of the numerical method in solving the tooth profile of non-circular curved face gear is derived from the generating process of the non-circular curved face gear. The generating process is shown in Fig. 6. XS rx2 Fig. 6. Coordinate system of generating process As shown in Fig. 6, Ok-XkYkZk is rigidly connected to the frame of the cutting machine. Ok'- Xk Yk'Zk is rigidly connected to the cutter. Likewise O2 -X2 Y2 Z2 is rigidly connected to the frame of the cutting machine. O2 -X2Y2 Pk' , the tooth profile of the cutter gear is transferred to the following coordinates of the non-circular curved face gear. Thus, the intersections are calculated through the equations of the line of the points obtained above and the equidistant curve equation of the pitch curve of the non-circular curved face gear. As shown in Fig. 8a, the left tooth profile of the cutter has four points, which equidistant from one another. , P2 , Pf, P4 are obtained by transforming the points to the coordinates O2<-X2