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Erschienen in: Chinese Journal of Mechanical Engineering 1/2023

Open Access 01.12.2023 | Original Article

Design of Linear Functional Noncircular Gear with High Contact Ratio Used in Continuously Variable Transmission

verfasst von: Yanan Hu, Chao Lin, Chunjiang He, Yongquan Yu, Zhiqin Cai

Erschienen in: Chinese Journal of Mechanical Engineering | Ausgabe 1/2023

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Abstract

Continuously variable transmission (CVT) of noncircular gear has the technical advantages of large bearing capacity and high transmission efficiency. The key technology of CVT with noncircular gear has been broken through some countries, and is in the stage of deep application research. Although the characteristics and design methods of noncircular gear pairs have been continuously studied in China, the noncircular gear CVT is still in the preliminary exploration and research stage. The linear functional noncircular gear pair, whose transmission ratio is a linear function in the working section, to realize continuously variable transmission was the research object in this paper. According to the required transmission ratio in the working section, the transmission ratio function in the non-working section was constructed by using a polynomial. And then the influence of pitch curve parameters in the working section on which in the non-working section was also analyzed to obtain the pitch curve suitable for transmission of this gear pair. In addition, for improving the stability and bearing capacity of gear transmission, the noncircular gear pair transmission with high contact ratio was designed. Furthermore, the accurate value of the contact tooth length was calculated based on the gear principle and the characteristics of the involute tooth profile, from this the contact tooth length error was calculated by comparing the accurate value with its actual value obtained by the rolling experiment. Finally, an indirect method to verify the contact ratio by detecting the contact length error of the tooth profile was proposed.

1 Introduction

Although continuously variable transmission (CVT) technology has been used in vehicles for only several decades, its advantages over traditional transmission are obvious: it has a wider range of working speed ratio; and it is easier to form an ideal match with the engine, so as to improve the combustion process, and further reduce fuel consumption and emissions; it has higher transmission efficiency, less power loss, and higher economy [1]. Generally, three main transmission modes can be adopted to realize infinitely variable speeds, namely, liquid transmission, electric transmission, and mechanical transmission. Different from the liquid transmission mode with a higher sliding rate, and the electric transmission mode with lower efficiency and unstable operation at low speed, in this respect, mechanical continuously variable transmission can easily realize effective transmission under special work conditions, such as high load, due to the equipment of more compact structure [2].
Furthermore, the transmission mechanism of mechanical CVT mainly includes belt transmission [3], chain transmission [4], and gear transmission [5]. Among them, belt CVT and chain CVT are the most common CVTs used in vehicles due to their simple structure, small size, and lightweight [6]. Despite these advantages, their limited torque capacity and low transmission efficiency cannot be ignored.
With the development of the design and manufacturing technology of noncircular gear, combined with the characteristics of noncircular gear transmission with non-uniform speed ratio, which belongs to conjugate meshing transmission [79], continuously variable transmission can be realized by using the transmission characteristics of noncircular gear, which is expected to improve the power and torque transmitted [10].
Many scholars have done a lot of research on the transmission technology of noncircular gears to solve many problems gradually, such as the geometric design of pitch curves, and the configuration and processing of gear teeth. Recently, the transmission technology of noncircular gear pairs has entered a new practical period [11]. Emura and Arakawa [12] utilized a noncircular gear for steering mechanism analysis. Song et al. [13] put forward that the gear-shifting process structure using a noncircular gear drive instead of a friction drive. Detailed descriptions of the gear trains for tracking the motions of the Mercury planet and of the Moon are herein presented by Addomine et al. [14]. In these gear trains, noncircular gears have been used to account for the apparent irregular motion of the planets. In addition, some scholars also use noncircular gear transmission in continuously variable transmission and have achieved some good results. Dooner et al. [15] recommended a continuously variable device of noncircular gears with a serrated transmission ratio. CVT could be realized within a specified range when controllable phase shift and planetary additive differential were used between noncircular gear devices [16].
For one noncircular gear pair, the shape and closure of the pitch curve have a decisive influence on the motion requirements. The pitch curves also have sharp points that require complex modification but can be continuous if the design is reasonable. Among them, the range of transmission ratio of the adder is limited. While the subtractor has a power cycle, its range of transmission ratio is arbitrary [17]. The pitch curves of noncircular gears were identified to be closed by the residue theorem [18]. Moreover, a general mathematical model for designing the pitch curve with minimal rotary inertia of the noncircular gear was proposed by resorting to the kinematics principle and calculus of variations [19]. And to realize a specific variable transmission ratio mechanism, a set of noncircular planetary gears consisting of an external pair and an internal pair with variable pitch lines was designed [20].
As for the contact ratio of gear transmission, it is closely related to mesh stiffness, which is an important parameter of gear transmission design and analysis [21]. As an index to measure the bearing capacity and transmission smoothness of gears, the higher the contact ratio is, the better the transmission smoothness is [9].
In other ways, Zheng et al. [22] put forward a new application of noncircular gears, which is an indexing mechanism using noncircular gears. He et al. [23] also provided a new generation method for noncircular gear, through which the generated gear may embody the advantages of localized tooth contact and good lubrication in practice. Based on the gear with rack and geared segment, Alexandru et al. [24] presented the geometric and functional characteristics of a gear with ascending variable ratio. This gear can be used for the steering boxes of some low-power vehicles (without a servo system).
Starting with the required transmission ratio, the influence of linear functional working pitch curve parameters on the non-working pitch curve was mainly studied in this paper. And the parameters of the linear functional noncircular gear pair suitable for transmission were obtained. By the way, an indirect method to verify the contact ratio by detecting the contact length error of the tooth profile was proposed, and the high contact ratio of the noncircular gear pair was verified. The research in this paper will contribute to reducing the transmission chain and simplifying the noncircular gear design used for CVT.

2 Design of Pitch Curve of Noncircular Gear in CVT

2.1 Realization of Infinitely Variable Transmission Using Noncircular Gears

The constant transformation from the input shaft to the output shaft can be realized by continuously variable noncircular gear transmission through the continuous and alternating transmission of power in the range of 0 to 360° by the multi-branch loop to obtain a constant speed ratio. Each branch loop is a three-element planetary row for differential coupling of two-order parallel noncircular gear pairs with non-uniform output speed, and then the constant speed ratio within a certain angle range is obtained through the controllable overrunning clutch. Rotation shafts of this branch are free rotation without power transmission, ranging in another rotation angle. Accordingly, the speed ratio can be continuously adjusted by changing the phase angle of two parallel noncircular gear pairs, like gear 1 and gear 2.
The continuously variable noncircular gear transmission system model and skeleton of the scheme mechanism are shown in Figure 1. As shown in Figure 1, 1–3 and 2–4 gear pairs are two noncircular gear pairs, while the rest are cylindrical gear pairs. This system with a constant transmission ratio involves the transmission unit superposition of two branch noncircular gear pairs with variable phases. During the working process, a constant speed input of component 1 will be converted to the linear function output speed of component 3 and component 4, through the first level transmission of the noncircular gear pair. And the constant output speed can be obtained in a limited range of angles after the output speed of components 3 and 4 is differential coupling. It is noted that the single-branch noncircular gear pair unit can only achieve stable speed at a limited angle. Once the three branches with second-order noncircular gear pairs are properly arranged around the central axis, and the minimum working angle of each branch per cycle is 120°, as a result, constant speed output will be obtained during the random angle range.
The output rotational speed of the noncircular gear pair designed by the pitch curve is shown in Figure 2(a). Namely, the single noncircular gear pair can’t provide a steady output rotational speed. And then, the differential mechanism, that is the double-row 2K-H type epicyclical gear train with a specific number of teeth shown in Figure 1, can realize the constant synthesis speed and the stable output within the limited angle. Therefore, the design of the pitch curve of each noncircular gear pair is greatly important, which directly affects the transmission ratio. Typical pitch curves of noncircular gear pairs include elliptic gear, eccentric gear, etc. And the pitch curves of the noncircular gear pair are determined according to the transmission ratios in this paper. If the transmission ratios are too complex, it will cause the values of m and n in Eq. (3) to be difficult, or even have no solution, and Eq. (3) is used to calculate the total transmission ratio. Consequently, the linear function, that is the first-order function, is chosen as the mathematical formula for the transmission ratio of noncircular gear pair. And a noncircular gear pair with the transmission ratio of the first functional form is named linear functional noncircular gear transmission.
Further, in the transmission system, gear 1 and gear 2 are fixed on the input shaft, and transmission ratios \(m_{ij}\) (i=1, 2; j=3, 4) of noncircular gear pairs 1–3 and 2–4 in working section \(\left[ {0,t} \right]\) are
$$ m_{31} = \frac{{\omega_{3} }}{{\omega_{1} }} = f\left( {\theta_{1} } \right) = k_{1} \theta_{1} + b_{1} ,\begin{array}{*{20}c} {} & {} \\ \end{array} \theta_{1} \in \left[ {0,t} \right], $$
(1)
$$ m_{42} = \frac{{\omega_{4} }}{{\omega_{2} }} = g\left( {\theta_{1} } \right) = k_{2} \left( {\theta_{1} - \theta } \right) + b_{2} ,\begin{array}{*{20}c} {} & {} \\ \end{array} \theta_{1} \in \left[ {0,t} \right], $$
(2)
where, \(\theta_{1}\) is the rotational angle of gear 1 and gear 2. \(\theta\) is the phase angle between gear 1 and gear 2, and t is the maximum rotational angle at working section in a period; k and b represent the slope value and the intercept value of linear function, respectively.
By designing the double-row 2K-H type epicyclical gear train with a specific number of teeth, the following relation, which is the total transmission ratio, can be achieved:
$$ m_{61} = m\left( {k_{1} \theta_{1} + b_{1} } \right) + n\left( {k_{2} \theta_{2} + b_{2} } \right) = c. $$
(3)
When a fixed rotational speed is inputted by shaft 1, shaft 6 will output a constant rotational speed, and the rotational speeds of each level in the gear transmission system are shown in Figure 2.
As shown in Figure 2, the continuously variable velocity outputting can be realized at phase angle \(\theta\) using the second-order noncircular gear pair. And then the constant rotational speed can be outputted by output shaft 6, as the phase angle between two noncircular gear pairs is \(\theta\). And the wider range of constant rotational speed outputting can be achieved during each period with decreased phase angle.

2.2 Transmission Ratio of Noncircular Gear in Non-working Section

Obviously, the two pitch curve sections of the noncircular gear are different during a period, that is, the transmission ratio in the working section is a linear function, \(\theta_{1} \in \left[ {0,t} \right]\), or that presents a complex curve in non-working section, \(\theta_{1} \in \left( {t,T} \right]\). Empirically, polynomial has been used to construct the transmission ratio function in non-working section outside the given interval in a transmission ratio period. Supposing the transmission ratio of noncircular gear pair in one period is expressed as follows.
$$ m_{31} = \frac{{n_{3} }}{{n_{1} }} = \left\{ \begin{gathered} m_{1} \left( {\theta_{1} } \right) = k_{1} \theta_{1} + b_{1} ,{\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \theta_{1} \in \left[ {0,t} \right], \hfill \\ m_{2} \left( {\theta_{1} } \right) = \sum\limits_{i = 0}^{6} {\left( {a_{i} \theta_{1}^{i} } \right),} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} \theta_{1} \in \left( {t,T} \right], \hfill \\ \end{gathered} \right. $$
(4)
where, \(a_{i}\) is the polynomial coefficient.
The first-order and second-order noncircular gears are driving and driven parts, respectively. It is reported by Huang et al. [25] that the values of \(a_{i} (i = 1,....,7)\) can be calculated by 7 independent equations including 1 closed condition and 6 boundary conditions, as shown in Eq. (5).
$$\left\{ \begin{gathered} \int_{t}^{T} {m_{2} } (\theta _{1} )\,{\text{d}}\theta _{1} = \,\frac{{2\uppi }}{{n_{2} }} - \int_{0}^{t} {m_{1} (\theta _{1} )\,{\text{d}}\theta _{1} } {\kern 1pt}, \hfill \\ m_{1} (t) = m_{2} \left( t \right), \hfill \\ m_{1} ^{\prime } (t) = m_{2} ^{\prime } \left( t \right), \hfill \\ m_{1} ^{{\prime \prime }} (t) = m_{2} ^{{\prime \prime }} \left( t \right), \hfill \\ m_{1} (0) = m_{2} \left( T \right), \hfill \\ m_{1} ^{\prime } (0) = m_{2} ^{\prime } \left( T \right), \hfill \\ m_{1} ^{{\prime \prime }} (0) = m_{2} ^{{\prime \prime }} \left( T \right), \hfill \\ \end{gathered} \right.$$
(5)
where, \(n_{2}\) represents the order of noncircular gear. And so far, the transmission ratio of noncircular gear pair in the first period has been determined.

2.3 Influence Parameters of Pitch Curve of Noncircular Gear Pair

Due to the pitch curves form of two noncircular gear pairs is the same as Eq. (4) but some parameters are discrepant. Then, the transmission characteristics of noncircular gear pairs with linear functional transmission ratio are discussed based on the example of gear pairs 1–3. And the pitch curve of the noncircular gear pair can be obtained according to the centrode. Furthermore, in the working section \(\theta_{1} \in \left[ {0,t} \right]\), the radius vectors of the pitch curves, can be expressed as:
$$ r_{1} (\theta_{1} ) = E\frac{{m_{21} }}{{m_{21} + 1}} = E\frac{{k_{1} \theta_{1} + b_{1} }}{{k_{1} \theta_{1} + b_{1} + 1}}, $$
(6)
$$\left\{ \begin{gathered} r_{2} (\theta_{1} ) = E - r_{1} (\theta_{1} ) = \frac{E}{{k_{1} \theta_{1} + b_{1} + 1}}, \hfill \\ \theta_{2} (\theta_{1} ) = \int_{0}^{{\theta_{1} }} {\left( {k_{1} \theta + b_{1} } \right)} \text{d}\theta = \frac{{k_{1} }}{2}\theta_{1}^{2} + b_{1} \theta_{1} , \hfill \\ \end{gathered} \right.$$
(7)
where,\(r_{1} (\theta_{1} )\) is the radius vector of driving gear, which numbered 1; \(r_{2} (\theta_{1} )\) is the radius vector of driven gear, which numbered 2, and \(\theta_{2} (\theta_{1} )\) is the rotational angle of driven gear; the center distance between two gears is E. According to Eq. (5), \(k_{1}\) and \(b_{1}\) will be two important parameters of transmission ratio in non-working section. By analyzing the influence of the parameters \(k_{1}\) and \(b_{1}\) on the pitch curve in non-working section of noncircular gear pair with linear functional transmission ratio, the optimal pitch curve can be acquired further.
(1) The influences of parameter \(b_{1}\) on transmission ratio of noncircular gear pair, when \(k_{1}\) is constant.
Taking 1–3 gear pairs as an example, the value of period T is \(\uppi \), and the maximum rotational angle t in working section during a period is \(2/3\uppi \). When \(k_{1}\) is \(3/4\uppi \) , the influence of parameter \(b_{1}\) with variable value on transmission ratio is analyzed.
As shown in Figure 3, with the value of \(b_{1}\) increases in the interval of \( \left[ {0.5,2.1} \right] \), the amplitude of transmission ratio first decreased and then increased, and the transmission ratio curve in non-working section is first convex and then concave. Nevertheless, it seems clear that the transmission ratio curve changes gently with the rotation angle around the value of 1.75 for \(b_{1}\). And the transmission in this situation will be more suitable, because the instantaneous velocity and acceleration are smaller, and the minimum radius of curvature of pitch curve is larger. The corresponding transmission ratio and pitch curve of noncircular gear pair are shown as red curve in Figure 3(a) and (b), respectively.
The interval length y of codomain of transmission ratio can be calculated as Eq. (8).
$$y = m_{31\max } - m_{31\min }.$$
(8)
According to the above results, when the transmission ratio with the most appropriate linear function parameters is obtained, the interval length of the codomain of the transmission ratio is the narrowest. Therefore, the minimum interval length of the codomain of the transmission ratio under different parameters can help us to get the value of \(b_{1}\) that best fits for transmission, at a certain value of \(k_{1}\).
(2) The influences of \(k_{1}\) on transmission ratio of noncircular gear pair, when \(b_{1}\) is constant.
Similarly, when \(b_{1}\) is 0.5, with different values of \(k_{1}\), the influences of \(k_{1}\) on transmission ratio are analyzed as shown in Figure 4.
With the increase of \(k_{1}\) from \(3/4\uppi \) to \(19/4\uppi \), the amplitude of the transmission ratio first decreases and then increases. The transmission ratio curve in the non-working section is first convex and then concave. And around the value of \(9/2\uppi \) for \(k_{1}\), the transmission ratio curve is the gentle, that is, the interval length y of codomain of transmission ratio is narrow, which is suitable for transmission. Then, while \(k_{1}\) is \(9/2\uppi \) and \(b_{1}\) is 0.5, the transmission ratio function curve is relatively smooth, and the transmission ratio and centrode of noncircular gear pair are shown as blue curve in Figure 4.
(3) The combined influences of \(k_{1}\) and \(b_{1}\) on transmission ratio of noncircular gear pair
According to the above analysis, each value of \(k_{1}\) must correspond to an optimal value of \(b_{1}\) for transmission, so a series of values of \(k_{1}\) and corresponding \(b_{1}\) can be obtained. When the maximum rotational angle \(\Phi_{2}\) in working section of the driven gear is equal to the product of the maximum rotational angle \(\Phi_{1}\) of the driving gear and its order \(n_{1}\), that is \(\Phi_{2} = \Phi_{1} \times n_{1}\), the optimal transmission ratio curve of the non-working section can be acquired. Furthermore, when the transmission ratio of the gear pair in the working section is expressed as \(m_{21} = k_{1} \varphi_{1} + b_{1}\), and the transmission ratio curve of non-working section constructed by the six-order polynomial meets the condition that \(k_{1}\uppi + 3b_{1} = 6\), the optimal transmission ratio curve in non-working section will also be obtained. At this point, the range of transmission ratio of noncircular gear pair in the working section is \(\left[ {b,4 - b} \right]\); in addition, with a certain value of \(k_{1}\), \(b_{1}\) is \(2 - \left( {\uppi /3} \right)k_{1}\); and the range of transmission ratio is \(\left[ {2 - \left( {\uppi /3} \right)k_{1} ,2 + \left( {\uppi /3} \right)k_{1} } \right]\).
The comparisons of pitch curves of noncircular gear pairs with different transmission ratio parameters are shown in Figure 5. With \(k_{1}\) gradually increasing, even if the most appropriate \(b_{1}\) is taken to make the minimum fluctuation of the transmission ratio curve, and the transmission ratio function at this point is smooth, the minimum curvature radius of the pitch curve is so small that the teeth are subjected to extra bending stress, resulting that the teeth are prone to bending and fracture, which is not suitable for transmission.

3 The Contact Ratio of Noncircular Gear Pair

The contact ratio of one noncircular gear pair is the length ratio between the effective meshing curve and the pitch of the gear base circle, which significantly affects the meshing performance of noncircular gear transmission. It was reported by Wu et al. [9], the contact ratio of a noncircular gear pair can be expressed as follows:
$$ \varepsilon = \frac{{u_{1} + u_{2} }}{{\uppi m\cos \alpha_{0} }}, $$
(9)
where, \( u_{i} = \sqrt {\left( {\rho _{i} + h_{{ai}} } \right)^{2} - \left( {\rho _{i} \cos \alpha _{0} } \right)^{2} } - \rho _{i} \sin \alpha _{0} ,^{{}} \left( {i = 1,2} \right) \); \(\rho_{1}\) and \(\rho_{2}\) are the curvature radius of the pitch curves at the meshing point P; \(\alpha_{0}\) is the tangent angle between meshing curve and the pitch curve at meshing point P, that is, the tooth profile angle of rack cutter.
According to Eq. (9), some main parameters that affect the contact ratio of involute noncircular gear transmission are center distance \(E\), transmission ratio coefficient \(k_{1}\) and \(b_{1}\), addendum coefficient \(h_{a}^{*}\), modification coefficient \(x\), module \(m\), and tooth profile angle of the rack cutter \(\alpha_{0}\). Considering that the center distance \(E\) and the expected transmission ratio function \(m_{21}\) are unchanged, the pitch curve of modified gear pair should be same as that of the original gear pair. To satisfy the above-mentioned conditions, when one noncircular gear with positive addendum modification has been designed, the other one must be processed by negative addendum modification. Furthermore, the absolute value of the modification coefficient of the two gears should be equal. So only the height modification method with the modification coefficient \(x_{2} = - x_{1}\) and total modification coefficient \(\Sigma \;x = x_{1} + x_{2} = 0\) can be used [9]. As shown in Figure 6, zero modification has little effect on the contact ratio of noncircular gear.
Therefore, for a noncircular gear pair with a determined pitch curve, the main parameters affected by the contact ratio are as follows: tooth profile angle of rack cutter \(\alpha_{0}\), modification coefficient \(h_{a}^{*}\) and module \(m\). When parameters of noncircular gear pair according to the optimality principle are selected as: \(k_{1} = {3 \mathord{\left/ {\vphantom {3 {4\uppi }}} \right. \kern-0pt} {4\uppi }}\), \(b_{1} = 1.75\), \(E = 180{\text{ mm}}\), the influence of other parameters on the contact ratio of linear functional noncircular gear pair is shown in Figure 7.
As shown in Figure 7, for a certain noncircular pitch curve, with the increase of the addendum coefficient \(h_{a}^{*}\) or the number of teeth z, the decrease of tooth profile angle \(\alpha_{0}\) of the rack cutter or the modulus m, the minimum contact ratio of the noncircular gear pair in the working section will increase. In this paper, it is defined as high contact ratio while the minimum instantaneous contact ratio is greater than 2. When parameters are taken as the surface above plane \(\varepsilon = 2.0\) shown in Figure 7(b), gear transmission with high contact ratio can be achieved.
With respect to different linear functional pitch curves, the influence of the transmission ratio coefficient on contact ratio is shown in Figure 8. It is obvious that the curvature variations in the working section increase with the transmission ratio coefficient \(k_{1}\) increasing, and the smaller minimum contact ratio is also acquired.

4 Involute Profile of Noncircular Gear

Based on the pitch curve of the noncircular gear, the involute tooth profile of the noncircular gear can be obtained. The design of a noncircular gear tooth profile is to determine its geometric parameters and make it have reasonable meshing performance. For example, the tooth profile of the noncircular gear is required to ensure that the two calculated curves are pure rolling (i.e. transmission according to the required transmission ratio) with an appropriate pressure angle. Indeed, the noncircular gear pair transmission is directionality when it has meshed correctly. While the driving gear rotates clockwise, the transmission ratio of the gear pair is a required linear function. At this time, both the driving gear and the driven gear mesh with the right tooth profile. Therefore, the right tooth profile of the driving gear will be taken as the research object in this paper, and for simplicity, the following tooth profiles without special descriptions are called the right tooth profile of a driving gear.

4.1 Involute Profile of Driving Gear

In noncircular gear pair transmission, coordinate system \(S_{1} (O_{1} - x_{1} y_{1} z_{1} )\) is rigidly connected to the driving gear, and its initial position is shown in Figure 9. In the initial position, polar axis of the driving gear coincides with the y-axis of the fixed coordinate frame \(S_{0} (O - xyz)\), and the \(x_{1}\)-axis of coordinate system \(S_{1}\) is parallel to the x-axis of the fixed coordinate frame with a spacing of \(r_{1} (0)\). To simplify calculation, the right profile of the 1# tooth passes through the instantaneous center \(O\) at the initial position, then \(O\) must be a point on the meshing curve.
As shown in Figure 9, one right tooth profile on the driving gear intersects with pitch curve at point \(P_{0}\). \(M\) is the point on this tooth profile outside the pitch curve, and \(M^{\prime}\) is the point on this tooth profile within the pitch curve. Taking the point M for example, the normal \(n_{M} n_{M}\) of point \(M\) intersects the pitch curve at point P, which is the instantaneous center of the gear pair when point M is the meshing point. Moreover, the tangent of point P on the pitch curve is named \(\tau_{P} \tau_{P}\). In the coordinate system \(S_{1}\), the equation of the tooth profile \({\varvec{r}}_{1R}\) is
$${\varvec{r}}_{1R} = \varvec{O_{1} M} =\varvec{ O_{1} P} +\varvec{ PM},$$
(10)
where, \({\varvec{O}}_{{\varvec{1}}} {\varvec{P}} = {\varvec{r}}_{1} \left( {\phi_{1} } \right)\), and in terms of involute property,
$$x_{1} = \left| {{\varvec{PM}}} \right| = \cos \alpha_{n} \cdot \int_{{\Phi_{1} }}^{{\phi_{1} }} {\sqrt {{r^{\prime}_{1}}^2 \left( \phi \right) + r_{1}^{2} \left( \phi \right)} \text{d}\phi }.$$
(11)
It is noteworthy that https://static-content.springer.com/image/art%3A10.1186%2Fs10033-023-00896-4/MediaObjects/10033_2023_896_Figa_HTML.gif while the point \(M^{\prime}\) on this tooth profile is within the pitch curve owing to \(\phi_{1}^{\prime } < \Phi_{1}\).
In addition, at the meshing point P, the angle \(\lambda_{1}\) between the radial vector \( \user2{O}_{\user2{1}} \user2{P}{\text{(}}\,\user2{ = }\,\user2{r}_{1} (\phi _{1} )) \) of the pitch curve and the normal \(n_{M} n_{M}\) of the right tooth profile is
$$ \lambda_{1} = \alpha_{n} + \mu_{1} , $$
(12)
where, \(\mu_{1}\) is the angle between the radial vector \({\varvec{r}}_{1} \left( {\phi_{1} } \right)\) of the pitch curve and the positive direction of tangent vector \({\varvec{\tau}}_{p}\) at point P, and the measuring direction of angle \(\lambda_{1}\) is same as that of angle \(\mu_{1}\); the angle \(\alpha_{n}\) represents the tooth profile angle of cutter.
Further, the radial vector of the tooth profile \({\varvec{r}}_{1R}\) in the coordinate system \(S_{1}\) can be obtained as
$$ \begin{gathered} {\varvec{r}}_{1R}^{(1)} = \left[ {\begin{array}{*{20}c} {x_{1R} } \\ {y_{1R} } \\ \end{array} } \right] = \left[ {\begin{array}{*{20}c} {\left| {{\varvec{r}}_{1R} } \right|\sin \phi_{M} } \\ {\left| {{\varvec{r}}_{1R} } \right|\cos \phi_{M} } \\ \end{array} } \right] \hfill \\ {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} {\kern 1pt} = \left[ {\begin{array}{*{20}c} { - r_{1} \left( {\phi_{1} } \right)\sin \phi_{1} \pm x_{1} \sin \left( {\phi_{1} + \lambda_{1} } \right)} \\ {r_{1} \left( {\phi_{1} } \right)\cos \phi_{1} \mp x_{1} \cos \left( {\phi_{1} + \lambda_{1} } \right)} \\ \end{array} } \right], \hfill \\ \;\;\;\;\;\;\;\; \hfill \\ \end{gathered} $$
(13)
where the above symbol is used for the point outside the pitch curve; and the below symbol is used for the point within the pitch curve.
Consequently, the polar coordinate equation of the right tooth profile of the driving gear is as follows:
(1)
While the point \(M\) on the tooth profile is outside the pitch curve
$$ \left\{ \begin{gathered} r_{1R} \left( {\phi_{1} } \right) = \sqrt {r_{1}^{2} \left( {\phi_{1} } \right) + x_{1}^{2} + 2r_{1} \left( {\phi_{1} } \right)x_{1} \cos \lambda_{1} } , \hfill \\ \phi_{M} \left( {\phi_{1} } \right) = \arctan \frac{{ - r_{1} \left( {\phi_{1} } \right)\sin \phi_{1} + x_{1} \sin \left( {\phi_{1} + \lambda_{1} } \right)}}{{r_{1} \left( {\phi_{1} } \right)\cos \phi_{1} - x_{1} \cos \left( {\phi_{1} + \lambda_{1} } \right)}}. \hfill \\ \end{gathered} \right. $$
(14)
 
(2)
While the point \(M^{\prime}\) on the tooth profile is within the pitch curve
$$ \left\{ \begin{gathered} r_{1R} \left( {\phi_{1} } \right) = \sqrt {r_{1}^{2} \left( {\phi_{1} } \right) + x_{1}^{2} - 2r_{1} \left( {\phi_{1} } \right)x_{1} \cos \lambda_{1} } , \hfill \\ \phi_{M} \left( {\phi_{1} } \right) = \arctan \frac{{ - r_{1} \left( {\phi_{1} } \right)\sin \phi_{1} - x_{1} \sin \left( {\phi_{1} + \lambda_{1} } \right)}}{{r_{1} \left( {\phi_{1} } \right)\cos \phi_{1} + x_{1} \cos \left( {\phi_{1} + \lambda_{1} } \right)}}. \hfill \\ \end{gathered} \right. $$
(15)
In the same way, the polar coordinate equation of the right tooth profile of the driven gear also can be obtained.
 
(1)
While the point \(M\) on the tooth profile is outside the pitch curve
$$ \left\{ \begin{gathered} r_{2R} \left( {\phi_{1} } \right) = \sqrt {r_{2}^{2} \left( {\phi_{1} } \right) + x_{2}^{2} + 2r_{2} \left( {\phi_{1} } \right)x_{2} \cos \lambda_{2} } , \hfill \\ \phi_{2M} \left( {\phi_{1} } \right) = \arctan \frac{{ - r_{1} \left( {\phi_{1} } \right)\sin \phi_{2} - x_{2} \sin \left( {\phi_{2} + \lambda_{2} } \right)}}{{r_{2} \left( {\phi_{1} } \right)\cos \phi_{2} + x_{2} \cos \left( {\phi_{2} + \lambda_{2} } \right)}}. \hfill \\ \end{gathered} \right. $$
(16)
 
(2)
While the point \(M^{\prime}\) on the tooth profile is within the pitch curve
$$ \left\{ \begin{gathered} r_{2R} \left( {\phi_{1} } \right) = \sqrt {r_{2}^{2} \left( {\phi_{1} } \right) + x_{2}^{2} - 2r_{2} \left( {\phi_{1} } \right)x_{2} \cos \lambda_{2} } , \hfill \\ \phi_{2M} \left( {\phi_{1} } \right) = \arctan \frac{{ - r_{1} \left( {\phi_{1} } \right)\sin \phi_{2} + x_{2} \sin \left( {\phi_{2} + \lambda_{2} } \right)}}{{r_{2} \left( {\phi_{1} } \right)\cos \phi_{2} - x_{2} \cos \left( {\phi_{2} + \lambda_{2} } \right)}}. \hfill \\ \end{gathered} \right. $$
(17)
 

4.2 The Meshing Curve of Noncircular Gear Pair

As is known, each pair of conjugate tooth profiles of noncircular gear pair is generally different, so its meshing curve is also different [8].
As shown in Figure 10, at the initial position of noncircular gear pair transmission, one point M″ on the right tooth profile of the driving gear whose polar coordinates is (ϕM, r1R), and the normal of the right tooth profile and pitch curve intersect at P″. When the driving wheel has rotated angle θ1 clockwise, which θ1 is equal to ϕ1 with opposite direction, P″ turned to P, M″ turned to M, and the radial vector of pitch curve coincides with the y-axis of fixed coordinate frame S0 at this moment. According to the principle of gearing, when point P falls on the line between the centers of the two gears, point M on the tooth profile of the driving gear is tangent to the corresponding point on its conjugate tooth profile, and point M is one point on the meshing curve of this noncircular gear pair.
The rotating angle of driving gear θ1 is the angle between reference frame S0 and S1. The coordinate transformation matrix M01 from S1 to S0 is as follows:
$$ {\varvec{M}}_{01} = \left[ {\begin{array}{*{20}c} {\cos \theta_{1} } & {\sin \theta_{1} } & 0 \\ { - \sin \theta_{1} } & {\cos \theta_{1} } & {r_{1} \left( 0 \right)} \\ 0 & 0 & 1 \\ \end{array} } \right]. $$
(18)
By transforming the radial vector of the tooth profile r1R into the fixed coordinate frame S0, the meshing curve of the gear pair can be obtained by
$$ {\varvec{r}}_{M} = {\varvec{M}}_{01} {\varvec{r}}_{1R}^{(1)} = \left[ {\begin{array}{*{20}c} {\cos \theta_{1} } & {\sin \theta_{1} } & 0 \\ { - \sin \theta_{1} } & {\cos \theta_{1} } & {r_{1} \left( 0 \right)} \\ 0 & 0 & 1 \\ \end{array} } \right]\left[ {\begin{array}{*{20}c} {x_{1R} } \\ {y_{1R} } \\ 1 \\ \end{array} } \right]. $$
(19)
By the way, because θ1 is equal to ϕ1, the meshing curve of the noncircular gear pair in fixed coordinate frame S0 can be expressed as
$$ \left\{ \begin{gathered} x_{M} = x_{1R} \cos \phi_{1} + y_{1R} \sin \phi_{1} , \hfill \\ y_{M} = - x_{1R} \sin \phi_{1} + y_{1R} \cos \phi_{1} + r_{1} \left( 0 \right). \hfill \\ \end{gathered} \right. $$
(20)
While the number of teeth z1 and z2 are 46 and 23 respectively, the theoretical results of some meshing curves have been obtained by MATLAB, as shown in Figure 11. The azure curve is the meshing curve of 1# tooth, and above are the meshing curves from 2# tooth to 18# tooth, where, the teeth from 2# to 16# are fully on the working section, both the upper half of 1# tooth profile and lower half of 17# tooth profile are in the working section, and the 18# tooth is completely on the non-working section as the red curve in Figure 11.

4.3 The Length of Contact Profile of Driving Gear

The meshing process of one conjugate tooth profiles pair is from an addendum of driving gear peak contacting to an addendum of driving gear peak contacting. Therefore, in the fixed coordinate frame S0, the intersection point F of the meshing curve and the addendum curve of the driven gear is the starting point of the contact profile of the driving gear, and the intersection point A of the addendum curve and the tooth profile of the driving gear is the end point of the contact profile of the driving gear. 2# tooth is taken as an example as shown in Figure 12.
The addendum curve [9] of the driven gear in the reference system \(S_{2} \left( {O_{2} - x_{2} y_{2} z_{2} } \right)\), which is rigidly attached to the driven gear, can be presented as
$$ \left\{ \begin{gathered} r_{2A} \left( {\varphi_{2} } \right) = \sqrt {r_{2}^{2} \left( {\varphi_{2} } \right) + h_{a}^{2} + 2r_{2} \left( {\varphi_{2} } \right)h_{a} \sin \mu_{2} } , \hfill \\ \varphi_{2A} \left( {\varphi_{2} } \right) = \varphi_{2} - \arcsin \frac{{h_{a} \cos \mu_{2} }}{{r_{2A} \left( {\varphi_{2} } \right)}}. \hfill \\ \end{gathered} \right. $$
(21)
The following simultaneous equations can be used to get the intersection point of the tooth profile as Eq. (16) and the addendum curve as Eq. (21) of the driven gear.
$$ \left\{ \begin{gathered} r_{2R} \left( {\phi_{1} } \right) = r_{2A} \left( {\varphi_{2} } \right), \hfill \\ \phi_{2M} \left( {\phi_{1} } \right) = \varphi_{2A} \left( {\varphi_{2} } \right). \hfill \\ \end{gathered} \right. $$
(22)
Then a unique solution \(\left( {\phi_{1} ,\varphi_{2} } \right)\) can be obtained from the above equations. Substituting the solution into the tooth profile equation of the driven gear, the tooth addendum point \(F\left( {\phi_{2F} \left( {\phi_{1} } \right),r_{2F} \left( {\phi_{1} } \right)} \right)\) of the driven gear can be obtained. According to the principle of gears, the solution of \(\phi_{1}\) is the pitch curve angle \(\phi_{1F}\) when the tooth of the driving gear enters into meshing.
Similarly, the tooth addendum point \(A\left( {\phi_{1A} \left( {\phi_{1} } \right),r_{1A} \left( {\phi_{1} } \right)} \right)\) of the driving gear also can be obtained, and at this time, the value of \(\phi_{1}\) is the pitch curve angle \(\phi_{1A}\) when the tooth of driving gear is out of meshing. And the theoretical length of the contact profile of the tooth \(l_{1}\) can be obtained further as follows.
$$l_{1} = \int_{\phi_{1F}}^{\phi_{1A}} {\sqrt {x{^{\prime}}_{1R}^{{^{2} }} + y{^{\prime}}_{1R}^{2} \text{d}\phi_{1} } }.$$
(23)
As shown in Figure 13, the 2# theoretical contact tooth profile https://static-content.springer.com/image/art%3A10.1186%2Fs10033-023-00896-4/MediaObjects/10033_2023_896_Figb_HTML.gif of the driving gear has been obtained by MATLAB. In addition, according to the results of contact stress by ANSYS, there are double tooth-meshing areas and three tooth-meshing areas on the actual meshing curve https://static-content.springer.com/image/art%3A10.1186%2Fs10033-023-00896-4/MediaObjects/10033_2023_896_Figc_HTML.gif .

5 Experimental Verification

Combined with the above analysis, in order to achieve high contact ratio transmission, the noncircular gear pair parameters are selected as shown in Table 1.
Table 1
Parameter values of noncircular gear pair
Parameter
Value
\(k_{1}\)
\(3/4\uppi \)
\(b_{1}\)
1.75
\(E\)(mm)
172.32
\(m\)
5
\(z_{1}\)
46
\(z_{2}\)
23
\(\alpha\)
\(18^{ \circ }\)
\(h_{a}^{*}\)
1.15
The tooth profile curve of the noncircular gear pair obtained by simulating the machining process of the slotting cutter with MATLAB is shown in Figure 14. The tooth profile points of the noncircular gear pair obtained by MATLAB are imported into SolidWorks to establish the model, and the final model of the noncircular gear pair used for machining will be obtained after smoothing the tooth surface.
To measure the transmission ratio and the contact length of the tooth profile of the noncircular gear pair, after finishing the processing of the noncircular gear pair through the five-axis CNC machining center, the noncircular gear rolling test was arranged on the comprehensive experimental test platform of the noncircular gear transmission, and the experimental test platform is shown in Figure 15. By the way, to print the top line mark of the driving gear tooth more clearly on the driven gear tooth surface, the rotating speed of the input gear in this experiment is 60 r/min, which is slower than normal operation.
During this experiment, the input torque and speed provided by the drive motor drive the driving gear to rotate firstly, through gear meshing, the driven gear drives the magnetic particle loader to rotate subsequently. The input torque tachometer installed between the drive motor and gear case can measure the input torque, rotational velocity, and other parameters. The output torque tachometer installed between the magnetic particle loader and gear case can measure the output torque, rotational velocity, and other parameters. Finally, the input/output torque and rotational velocity are fed back to the operator console for post-processing. And these parameters including load torque and speed of the drive motor can be further adjusted by the operation console.
To minimize the influence of error caused by random signal interference on experimental results, the acquired experimental data must be processed. Therefore, the actual transmission ratio \(i^{\prime}_{12}\) is obtained from Eq. (24).
$$ i^{\prime}_{12} = \frac{{\omega_{1}^{\prime } }}{{\omega_{2}^{\prime } }} = \frac{{n^{\prime}_{1} }}{{n_{2}^{\prime } }}, $$
(24)
where, \(\omega_{1}^{\prime }\) and \(n_{1}^{\prime }\) are angular velocity and rotating speed of driving gear, respectively. \(\omega_{2}^{\prime }\) and \(n_{2}^{\prime }\) are angular velocity and rotating speed of driven gear, respectively.
Due to the involute profile of the noncircular gear, the contact ratio error can be reflected by the contact profile length error. As is known, the actual meshing curve of the noncircular gear pair is very important for reflecting the contact ratio of this gear pair. According to the actual meshing curve of the gear pair, the partial tooth profile that participates in meshing can be known, that is, the working section of the tooth profile. Therefore, it is proposed to confirm the error of contact ratio indirectly by measuring the error of the working section of the tooth profile. The partial tooth surface containing the tooth addendum of the driven gear was coated with a uniform layer of red lead powder, which is shown in Figure 16(a).
After the noncircular gear pair turned a cycle, the contact marks with red lead powder were left on the teeth surface of the driving gear, that is, the initial position of the contact tooth profile, which is shown in Figure 16(b). Then the contact mark on the driving gear surface was recorded by A4 paper; after being scanned into the computer, the error of the contact tooth profile length was obtained through data processing subsequently. 3# teeth of noncircular gear pair were taken as examples, and the contact area and tooth surface were shown in Figure 16(c), where l2 is the length of the experimental contact tooth profile, and l0 is the length of the tooth profile.
Further, the length error of contact tooth profile \(e_{\varepsilon }\) could be obtained by analyzing the length of experimental contact profile l2 and theoretical contact profile l1 according to Eq. (25).
$$ e_{\varepsilon } = \frac{{\left| {\Delta l} \right|}}{{l_{1} }} \times 100\% { = }\frac{{\left| {l_{1} - l_{2} } \right|}}{{l_{1} }} \times 100\% . $$
(25)
Next, the experimental results after being processed are quantitatively analyzed. Figure 17 shows the comparisons between the theoretical and experimental results of the transmission ratio and contact tooth profile length of the noncircular gear pair.
The results in Figure 17 show that: (1) Except for the errors caused by measurement and installation, the experimental value of the transmission ratio of the noncircular gear pair is basically consistent with the theoretical value, and the period of the experimental value is consistent with its theoretical value. Because the experiment was carried out under the condition of low speed and light load, the influence caused by the dynamic characteristics of the noncircular gear can be ignored, and the error between the experimental results and the theoretical results is relatively small. In the working section, the maximum error of the transmission ratio is \(6.18{\text{\% }}\), which in the non-working section is \(5.19{\text{\%}}\), and the maximum error mainly lies in the connection between the working section and the non-working section.
(2) It can be seen from the comparison results of the contact tooth profiles of noncircular gears that in a meshing period, the experimental values of the contact tooth profiles of noncircular gear are basically consistent with the theoretical values, which verifies the feasibility of the theoretical analysis method. The fluctuation amplitude of the experimental contact tooth profiles is greater than the theoretical results, and the experimental contact tooth profiles are lower than the theoretical values, while the maximum error in the working section is 5.4%. The main reason for this result is that in order to ensure the noncircular gear pair normal meshing, the proper backlash is required by slightly increasing the installment center distance, which makes the actual contact profile smaller. In addition, the gear machining accuracy is also an important factor leading to the actual contact profile length decreasing.

6 Conclusions

(1)
The linear functional noncircular gear pair is used to realize continuously variable transmission by means of branch-differential coupling, and the pitch curves of this gear pair are designed according to the required transmission ratio. The influence of the parameters of the linear function, k1 and b1, on the pitch curve of the noncircular gear pair with linear functional transmission ratio in the non-working section is analyzed; further, the most suitable pitch curve form is obtained, which each value of k1 must correspond to the best value of b1.
 
(2)
When the pitch curve in the non-working section constructed by a six-order polynomial meets the optimal conditions, the pitch curve is the smoothest. When k1 increases gradually, even if b1 is the most suitable value to make the variation trend of the pitch curve in the non-working section has the gentlest change trend, however, the minimum curvature radius of the pitch curve of driving/driven gear is too small. Thus, on the one hand, the strength of gear teeth is insufficient; on the other hand, the instantaneous speed and acceleration are too large, resulting in unstable transmission. Generally, this method can be used to design the noncircular gear pair which is suitable for CVT.
 
(3)
The larger the transmission ratio parameter k1 of the linear functional noncircular gear pair is, the larger the variation range in the working section is, and the smaller the minimum contact ratio is. Finally, by measuring the length error of contact tooth profile, the error of the contact ratio is detected indirectly, which could verify the correctness of the design of a high contact ratio of noncircular gear pair.
 

Acknowledgements

The authors sincerely thanks to Professor Jing Wei of Chongqing University for his critical discussion and reading during manuscript preparation.

Declarations

Competing Interests

The authors declare no competing financial interests.
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://​creativecommons.​org/​licenses/​by/​4.​0/​.
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Metadaten
Titel
Design of Linear Functional Noncircular Gear with High Contact Ratio Used in Continuously Variable Transmission
verfasst von
Yanan Hu
Chao Lin
Chunjiang He
Yongquan Yu
Zhiqin Cai
Publikationsdatum
01.12.2023
Verlag
Springer Nature Singapore
Erschienen in
Chinese Journal of Mechanical Engineering / Ausgabe 1/2023
Print ISSN: 1000-9345
Elektronische ISSN: 2192-8258
DOI
https://doi.org/10.1186/s10033-023-00896-4

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