# I. Introduction ue to their compactness and their ability to transmit high loads at high speeds, gears are widely used in automotive and aerospace applications through speed reducers, power transmissions in wind turbines, etc. In gear drives energy efficiency improving may require reducing power losses. Power losses in gears (gearboxes, reducers, etc.) can be grouped into two categories: power losses depending on the transmitted load (friction at the contact areas between the teeth and friction in the bearings, etc.) and those independent of the transmitted load (losses due to the trapping of the lubricant, the ventilation of the mobiles, etc.). Several researchers have been interested in load-dependent losses and enough models exist. The oil trapping in the inter-tooth space and the ventilation of the spindles are the two main sources of power dissipation in the case of losses independent of the loads. Very few studies and models exist on the loss of power by lubricant trapping and by consequent on the modeling of lubricant leakage surfaces. The vast majority of studies concerning the modeling of lubricant trapping in the inter-tooth space are empirical, numerical, and semi-analytical and based on approximations and estimations. Using NASA research center test rig, Anderson and al. [2], Krantz [3], Rohn and Handschuh [4] have developed several empirical formulas. Empirical formulations for the particular case of trapping losses in gears are based on the gears geometric parameters and include those of Terekhov [5], Wolfan Mauz [6], Butsch M. [7] and Maurer J. [8]. The empirical models developed provided global formulas for the estimation of pressing torque or power loss. It is necessary to point out that these formulas are only valid for external gearing and remain linked to the sensitivity and precision of the equipment used for the tests. Generally they are of very low precision with quite important deviations. As an example we can quote the model of Mauz [6], which indicates an uncertainty between 5 and 15% if the resisting torque is higher than 5 Nm and an uncertainty up to 50% for lower torque values. It is therefore necessary to set up another quite precise model. Many researchers have developed numerical models to understand the behavior of inter-tooth spaces during movement in order to estimate the power lost by trapping. Pechersky and Wittbrodt [9] used an approximation of the tooth profile expression to calculate the leakage surfaces. Diab Y. and al [10][11] have numerically evaluated the radial leakage surfaces (considered here as minimum distances between the tip corner of the gear and the profile) and they obtained the axial leakage surfaces by The first experimental studies on this subject permitted to make a difference between load-depending and load-independing losses. Devin R. and Hilty B. [1], made experimental investigations of load-independent losses caused by planetary gear sets and conclude that for high speeds (? 6000 r pm) the losses independent of the load become the major contributor. These experimental works allowed to develop and validate empirical, numerical and semi-analytical models. numerical integration. Abdelilah Lasri and al [12][13][14] used a numerical approximation to evaluate the radial surfaces (considered here as the minimum distance between the tooth profiles) and they obtained the axial leakage surfaces by numerical integration. David C. Talbot [15] calculates the power lost by trapping in planetary gears by discretizing in time and space the Conservation of Mass, Momentum and Energy equations. The leakage surfaces are obtained by numerical approximation through the surfaces meshing. Seetharaman and Kahraman [16] were inspired by the work of Pechersky and Wittbrodt [9] to establish a semi-analytical formulation for calculating leakage surfaces. However, several approximations are made there, namely a Taylor approximation of order 1 of the involute profileequation, the cancellation of certain portions of the surface, the use of approximate values of certain distances, etc. From the vectors ray approach, Massimo Rundo [17] established an analytical formula for trapped volume in crescent pumps. It is necessary to note that in this approach the length variation of the vector ray for an infinitesimal rotation is neglected. In addition, this formula is limited only to the portion where teeth profiles are in contact. For an efficient contribution to the power losses by the lubricant trapping of as well as the wear of the elements with a view to improve the energy performances in gears transmissions, it is essential to completely lift the veil on the inter-tooth zone during meshing. From the work of Seetharaman and Kahraman [16], we will establish a purely analytical model of the evolution of the radial and axial leakage surfaces as a function of the angle of rotation in a spur gear. This work has as particularity the use of the exact expression of the tooth profile in the calculations and the authenticity of the analytical expressions of the developed surfaces. This work is divided into three main parts. The first part is devoted to the modeling of the tooth profile and the associated parametric equations. The second part deals with the calculations of the leakage surfaces from the tooth profile equations, with the radial leakage surface being considered as the minimum distance between the tooth profiles. The last part focuses on the results interpretation and the model validation. The model validation consist of a superposition of our results with those of A. Lasri and al [13] and Diab and al [10]. # II. Material a) Trapping Phenomenon The lubricant used in gear transmissions to reduce corrosion, friction, cool the elements, etc., is trapped in the inter-tooth space during movement and becomes the seat of energy losses. Lubricant trapping is the jamming of the lubricant in the inter-tooth space during the meshing phase. The fraction of lubricant trapped in the inter-tooth space (in yellow in figure 1) is expelled under pressure radially toward the neighbouring pockets and or axially toward the outside of the gear during this phenomenon. The opposite phenomenon is reproduced during the unmeshing phase. The geometry of the inter-tooth space relates to the type of tooth (straight, helical, hypoid, etc.) which constitutes the gear's wheels. In the particular case of spur gears, the axial leakage area remains constant over the tooth width. However, in the case of helical gear, the axial leakage area is variable over the tooth width. The radial and axial leakage surfaces vary according to the angle of rotation. The further away from the initial position, the surfaces increase. Here, the initial position is the meeting point between the two pitch circles. The Figure 2 below illustrates the behavior of the leakage surfaces as a function of the angle of rotation from a) to h). The pinion (driver) is associated to a fixed reference ??? ð??"ð??" , ?? ð??"ð??" , ?? ð??"ð??" , ?? ð??"ð??" ? and mobile reference (?? 1 , ?? 1 , ?? 1 , ?? 1 ), which revolves around (?? ð??"ð??" , ?? ð??"ð??" ) by an angle ?? 1 . Similarly, the gear (driven) is associated to fixed reference (?? ?? , ?? ?? , ?? ?? , ?? ?? ) and mobile reference (?? 2 , ?? 2 , ?? 2 , ?? 2 ) , which revolves around (?? ?? , ?? ?? ) by an angle ?? 2 . Such as In our calculations, the initial position is the position where the tooth profiles of the driving and driven gears meet at point I (the contact point between the pitch circles). ?? 2 =?(?? 1 /?? 2 ) ?? 1 =?(?? 1 /?? 2 ) ?? 1 =?(?? ??1 /?? ??2 ) ?? 1 . # d) Geometry of a Spur Gear Tooth The tooth shapes of spur gears are relative to the number of teeth. Generally, for a tooth, there will be the involute zone and the circular zone. In a specific interval of the rotation angle, the profiles of the teeth meet, and consequently the radial leakage surfaces remain zero. Figure 5 below is a particular case. On this figure, C1 and C2 are the two contact points of the tooth profiles. The simulation of the equations and the model obtained was carried out with the MATLAB R2016A application installed in an HP computer, AMD A6-3400 APU HD Graphics 1.40 GHz; 6 GB of RAM. # III. Method a) Hypothesis Our study was carried out under the following assumptions: -The portion of tooth between the addendum circle and the base circle is in involute. -The shape of the tooth portion after the base circle varies depending on the tooth number. -Radial distances are minimum distances between adjacent profiles. -The direction of rotation of positive angles is the trigonometric direction and, the direction of rotation of negative angles is the anti-trigonometric direction. -In our calculations, the initial position (?? ?? =0) is the position where the two adjacent profiles meet at the common point of the pitch circles. However, for the presentation and the comparative study of the results, we bring the initial position back to the position where (O 1 O 2 ) passes simultaneously through the midpoints of the gear top land and the pinion root. # b) Calculation Algorithm From the geometric parameters of a gear tooth, the parametric equations of the half tooth profile are established. The complete gear tooth is obtained by axial symmetry of this half tooth, followed by N-1 successive rotations of the primary tooth with respect to the axis of the gear and respective angles 2*??*k/N, 1?k?N-1. Where N is the number of teeth. From the initial position, the coordinates of the boundary points of the leakage surfaces are calculated as a function of the rotation angle. From the properties of the involute of a circle, we calculate the radial distances as a function of the rotation angle and by surface integration, we obtain the radial surfaces. The figure 7 below is the algorithm that succinctly presents our working methodology. # 1) Tooth tip equation The tooth tip is a fraction of the tip circle (see figure 4). By applying the parametric equation of a circle with radius ?? ?? (tip radius) centered in the point ?? 1 , the parametric equation of the half of the geartooth tip is given in the coordinate system (o, x, y) by the relation (1) below: With ?? ?????? ? q ? ?? ?????? , ?? ?????? = mes (???, ???? ?????? ) and ?? ?????? = ?? 2 # 2) Equations of the involute portion (AB) By applying the properties of the involute of the circle, the parametric equations of the portion (AB) in the fixed frame (O,x,y) are given by the relation (2) below: with 0? ?? ? [ ?? ?? 2 ?? ?? 2 ? 1] 1/2 # 3) Equations of the portion between the base circle and the root circle On the figure 6, 0? ?? ? ?? ??????(3) with ?? ?????? = ?? ?? -? ?? . By application of the geometric construction properties (see [20]) ??=arccos(2rb*rp/(???? 2 + ???? 2 )). In the cas of gears with pressure angle ?? = 20°, when ?? ?????? ? arccos(2rb*rp/ (???? 2 + ???? 2 ) ) then we take ??=k*((??/N)-? ?? ); 0 ?? ?? : Two possibilities emerge. ? If arccos(2?? ?? *?? ?? /(?? ?? 2 + ?? ??2 )) ? ?? ?????? : In this case, this portion will consist of two (02) types of profiles, namely the arc of a circle BD followed by the root circle. ? If ?? ?????? 0 and S r2 =0), -When we are at the left of the initial position with ?? 1 and ?? 2 does not exist (S r1 >0 and S r2 >0), -When we are at the right of the initial position and only ?? 2 exists (S r1 =0 and S r2 >0), -When we are at the right of the initial position with ?? 1 and ?? 2 does not exist (S r1 >0 and S r2 >0), The relations below give the expressions of the radial leakage surfaces in each of these cases cited above. # At the right of the initial position ? Case where S r1 =0 and S r2 > 0: (tan(?? 0 )-? ( ?? ?? 1 ?? ?? 1 ) 2 ? 1 < ?? 1 < (? ?? ??2 ?? ??1 )(?tan(?? 0 ) ? 2?? 2 + ? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 )) According to figure 5, where b is the face of the tooth width. with ?? 2 ?? 1 = ??? 1 ?? 2 2 ? ???? 1 2 , ?? 1 ?? 1 =???? 1 ?? 1 , with mes(???, ?? 1 ?? 2 ??????????? ) =arccos(((x?? 2 -0)(1-0))/?? 1 ?? 2 ) and mes(???, ?? 1 ??? 1 ???????????? )= arccos(((x??? 1 -0)(1-0))/?? 1 ??? 1 ). ? ? ? ???? 2 = rb1 * (?1 + ?? ??2 2 ) sin(?Arctan(?? ??2 ) + ?? ??2 ? inv(?? 0 ) + 2?? 1 ? ?? 1 ) ???? 2 = rb1 * (?1 + ?? ??2 2 ) cos(?Arctan(?? ??2 ) + ?? ??2 ? inv(?? 0 ) + 2?? 1 ? ?? 1 ) (23) ? ? ? ???? 1 = rb2 * (?1 + ?? ? ??1 2 ) sin(Arctan(?? ? ??1 ) ? ?? ? ??1 + inv(?? 0 ) ? ? ? ?? 2 ) ???? 1 = rb2 * (?1 + ?? ? ??1 2 ) cos(Arctan(?? ? ??1 ) ? ?? ? ??1 + inv(?? 0 ) ? ? ? ?? 2 ) (24) ? ? ? ???? 2 = rb2 * (?1 + ?? ? ??2 2 ) sin(?Arctan(?? ? ??2 ) + ?? ? ??2 ? inv(?? 0 ) + ? ? 2?? 2 ? ?? 2 ) ???? 2 = rb2 * (?1 + ?? ? ??2 2 ) cos(?Arctan(?? ? ??2 ) + ?? ? ??2 ? inv(?? 0 ) + ? ? 2?? 2 ? ?? 2 ) (25) S r2 = ?? * ?? 2 ?? 1 (26) ?? 2 ?? 1 =?? 2 ?? 1 -?? 1 ?? 1 (27) ?? 1 =mes(?? 1 ?? 2 ??????????? ,?? 1 ?? 1 ?????????? ) -mes(?? 1 ?? 2 ??????????? ,?? 1 ??? 1 ???????????? ) and mes(?? 1 ?? 2 ??????????? ,?? 1 ?? 1 ?????????? ) =arccos( ???? 1 ?? 1 ?? 2 ) mes(?? 1 ?? 2 ??????????? ,?? 1 ??? 1 ???????????? ) = mes(???, ?? 1 ?? 2 ??????????? ) -mes(???, ?? 1 ??? 1 ???????????? ) (28) Establishment of an Analytical Model for Determining Leakage Surfaces in an External Tooth Spur Gear # Global Journal of Researches in Engineering (A ) Volume Xx XII Issue II V ersion I ? Case where S r1 >0 and S r2 > 0: (?? 1 < tan(?? 0 )-? ( ?? ?? 1 ?? ?? 1 ) 2 ? 1 ) According to figure 6, ?? 2 ?? 2 =??? 2 ?? 2 2 ? ???? 2 2 ,?? 2 ?? 2 =???? 2 ?? 2 , ?? 2 =mes(?? 2 ?? 2 ?????????? ,?? 2 ?? 2 ?????????? ) -mes(?? 2 ?? 2 ?????????? ,?? 2 ?? 2 ????????? ) with mes(?? 2 ?? 2 ?????????? ,?? 2 ?? 2 ?????????? ) = Arccos( ???? 2 ?? 2 ?? 2 ). mes(???, ?? 2 ?? 2 ?????????? )= arccos(((x?? 2 -0)(1-0))/ ?? 2 ?? 2 ) and mes(???, ?? 2 ?? 2 ????????? )= arccos(((x?? 2 -0)(1-0)) /?? 2 ?? 2 ) Sr1 is given by the relation ( 27) # At the left of the initial position ? Case where S r1 > 0 and S r2 = 0: ( (?tan(?? 0 ) + 2?? 1 + ? ( ?? ?? 1 ?? ?? 1 ) 2 ? 1 ) > ?? 1 >- ?? ??2 ?? ??1 (tan(?? 0 )-? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 ))) Like the previous cases, with ??? 2 ??? 1 = ? ?? 1 ??? 2 2 ? ???? 1 2 , ??? 1 ??? 1 =???? 1 ??? 1 , ??? 1 =mes(?? 1 ??? 2 ???????????? , ?? 1 ??? 1 ???????????? ) -mes(?? 1 ??? 2 ???????????? ,?? 1 ??? 1 ?????????? ) and mes(?? 1 ??? 2 ???????????? ,?? 1 ??? 1 ???????????? ) =arccos( ???? 1 ?? 1 ??? 2 ) mes(???, ?? 1 ??? 2 ???????????? ) =arccos(((x??? 2 -0)(1-0))/?? 1 ??? 2 ) and mes(???, ?? 1 ??? 1 ?????????? )=arccos(((x??? 1 -0)(1-0))/?? 1 ??? 1 ) ? Case where S r1 > 0 and S r2 > 0 (?? 1 > ?tan(?? 0 ) + 2?? 1 + ? ( ?? ?? 1 ?? ?? 1 ) 2 ? 1 ) with ??? 2 ??? 2 = ??? 2 ??? 2 -??? 2 ??? 2 ,??? 2 ??? 2 = ? ?? 2 ??? 2 2 ? ???? 2 2 , ??? 2 ??? 2 =???? 2 ?? 2 and ??? 2 =mes(?? 2 ??? 2 ???????????? ,?? 2 ??? 2 ???????????? ) -mes(?? 2 ??? 2 ???????????? ,?? 2 ??? 2 ??????????? ), mes(?? 2 ??? 2 ???????????? ,?? 2 ??? 2 ???????????? ) =arccos( ???? 2 ?? 2 ??? 2 ) mes(???,?? 2 ??? 2 ???????????? )=arccos(((x??? 2 -0)(1-0))/?? 2 ??? 2 ) and mes(???, ?? 2 ??? 2 ??????????? )= Arccos(((x??? 2 -0)(1-0)) /?? 2 ??? 2 ) Sr1 is given by relation (33) iii. Calculation of Axial Leakage Surfaces Case where S r1 = 0 and S r2 = 0: ((? ?? ??2 ?? ??1 )(?tan(?? 0 ) ? 2?? 2 + ? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 ) ? ?? 1 ? - ?? ??2 ?? ??1 (tan(?? 0 )-? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 )) ? Case where ?? ?? < ?? ?? According to figure 5 and figure 6: S r1 = ?? * ?? 2 ?? 2 (29) ?? 2 ?? 2 = ?? 2 ?? 2 -?? 2 ?? 2 (30) mes(?? 2 ?? 2 ?????????? ,?? 2 ?? 2 ????????? ) =mes(???, ?? 2 ?? 2 ?????????? ) -mes(???, ?? 2 ?? 2 ????????? )(31)S r1 = ?? * ??? 2 ??? 1 (32) ??? 2 ??? 1 =??? 2 ??? 1 -??? 1 ??? 1(33) (34)S r2 = ?? * ??? 2 ??? 2(35) (36) Surface axiale= S?? 1 ?? 1 ??? 1 ?? 2 ?? 1 ??? 1 ?? 1 = S?? 1 ?? 1 ?? 1 ??? 1 ?? 2 ?? 1 ? S?? 1 ?? 1 ?? 1 ??? 1 ?? 2 ?? 1 (37) mes(?? 1 ??? 2 ???????????? ,?? 1 ??? 1 ?????????? ) = mes(???, ?? 1 ??? 2 ???????????? ) -mes(???, ?? 1 ??? 1 ?????????? ) mes(?? 2 ??? 2 ???????????? ,?? 2 ??? 2 ??????????? )=mes(???,?? 2 ??? 2 ???????????? ) -mes(???,?? 2 ??? 2 ??????????? ) Avec triangle_?? 1 ?? 2 ?? 2 ?? 1 =0.5?? 1 ?? 2 *E*sin(?? ??2 )et triangle_?? 1 ?? 1 ?? 2 ?? 1 =0.5*?? 1 ?? 1 *E*sin(?? ??1 ) S?? 2 ?? 2 ??? 1 ?? 1 ?? 2 =0.5*?? ??2 2 *(2*?? ???? 2 ),S?? 2 ?? 1 ?? 1 ?? 2 =0.5*?? ??2 2 (( ? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 ) 3 -?? ??2 3 )/3 and S?? 2 ?? 2 ??? 1 ?? 2 =0.5*?? ??2 2 *(( ? ( ?? ?? 2 ?? ?? 2 ) 2 ? 1 ) 3 -??? ??2 3 )/3 with S?? 1 ?? 1 ?? 1 ?? 1 =0.5*rb1 2 *(?? ??1 3 )/3, SO 1 B 1 B? 1 O 1 =(rc1+rp1)*o1c*sin(?)-rc1 2 *(qmax-qmin)+ rp1 2 *(q2max-q2min) ?? 1 c= ?(?? ?? ? 0) 2 + (?? ?? ) 2 q2max=(?/2)-(?+? s ) and q2min=(?/2)-(?/N1) qmin= Arccos((1*(?? ?? -?? ?? )+0*(?? ?? -?? ?? ))/EB) and qmax=qmin+acos(((?? ?? -?? ?? )*(?? ?? -?? ?? )+(?? ?? -?? ?? )*(?? ?? -?? ?? ))/rc1 2 ) SO 1 B? 1 C 2 O 1 =0.5*rb1 2 *(? C2 3 )/3. ? Case where ?? ?? ? ?? ?? According to figures 5 and 6 Figure 8 below is a detailed view of the half of the tooth profile taken from the simulation result for the specific case of gear 1 in table 1. S?? 1 ?? 1 ?? 1 ??? 1 ?? 2 ?? 1 =triangle_?? 1 ?? 2 ?? 2 ?? 1 -triangle_?? 1 ?? 1 ?? 2 ?? 1 -S?? 2 ?? 2 ?? 1 ??? 1 ?? 1 ?? 2 (38) S?? 2 ?? 2 ?? 1 ??? 1 ?? 1 ?? 2 = S?? 2 ?? 2 ??? 1 ?? 2 + S?? 2 ?? 2 ??? 1 ?? 1 ?? 2 + S?? 2 ?? 1 ?? 1 ?? 2 (39) S?? 1 ?? 1 ?? 1 ??? 1 ?? 2 ?? 1 = S?? 1 ?? 1 ?? 1 ?? 1 + S?? 1 ?? 1 ??? 1 ?? 1 + S?? 1 ??? 1 ?? 2 ?? 1 (40) Surface axiale = S?? 1 ?? 1 ?? 1 ??? 2 ?? 1 ??? 1 ?? 1 = S?? 1 ?? 1 ?? 1 ??? 1 ?? 2 ?? 1 -S?? 1 ?? 1 ?? 1 ?? 1 ??? 2 ?? 1 (41) S?? 1 ?? 1 ?? 1 ?? 1 ??? 2 ?? 1 = S?? 1 ?? 1 ??? 2 ?? 1 + S?? 1 ?? 1 ?? 1 ??? 1 + S?? 1 ?? 1 ?? 1 ?? 1(42)with S?? 1 ?? 1 ??? 2 ?? 1 =0.5*rb1 2 *((? C2 3 ) -? rp 1 3 )/3,S?? 1 ?? 1 ?? 1 ??? 1 =rp1 2 *(q3max-q2min)) and q3max=Arctan(yp1/xp1) S?? 1 ?? 1 ?? 1 ?? 1 =0.5*rp1 2 *(? ??1 3 -? rp 1 3 )/3 with ? rp 1 =?( ?? ?? 1 ?? ?? 1 ) 2 ? 1 The particularity here is the presence of a straight part on our teeth, namely the segment [BC]. Figure 9 below is a detailed view of the half of the tooth profile taken from the simulation result for the specific case of gear 2 in table 1. The profile is made up of the tooth top, the involute part, the circular part, and tooth root. Here, the straight part no longer exists. A detailed view of the half of the tooth profile resulting from the simulation result for the particular case of gear 3 of table 1 is represented in figure 10 below. Case of the gearing system of table 2 The result of our model for calculating the pockets volumes corresponding to the gearing system of table 2 has generated the curve of figure 12 # b) Results of Calculations of Radial and Axial Leakage Surfaces To validate our model, the simulation of our equations and formulas developed above (equations ( 13) to (42)) on Matlab 16 was carried out with the particular case of a gear whose characteristics are grouped in table 2 below. The application of our model for calculating of the radial leakage surfaces 1 and 2 relative to the gear of table 2 has generated the curves of figure 11 # c) Results Interpretation The curves of Figure 11 justify the similarity of the radial and axial leakage surfaces on each side of the initial position (?? 1 =0). This result agrees with the surfaces evolution of figure 2. we observe that On figures 2.a) to 2.h) the axial surface reaches its minimum at the initial position (?? 1 =0). This observation agrees with the curve of figure 12. More we move away from the initial position (?? 1 =0), the pockets volumes increase. This result agrees with the observation of figures 2.a) to 2.h). The curves in figure 11 show that at the left of the initial position, the radial leakage surface one is always greater than the radial leakage surface two and, at the right of the initial position, it is the opposite phenomenon. This result agrees with the observations of figure 2. In figure 11, the two profiles bordering the radial surface 1 (?? ??1 ) meet when ?? 1 belongs in the interval [-3,75°; 6,5°]. For the radial surface 2 (?? ??1 ), this phenomenon occurs in the interval [-6,5°; 3,75°]. # V. Model Validation The validation of our model follows from a comparative study between the results of our model and the results of Abdelilah Lasri and al [13] and Diab Y. and al [10] for the same gear system. We have superimposed the curves of our model and those of the reference models. a) Superposition of the Radial Surfaces Curves of our Model and those Resulting from the Model of Abdelilah Lasri [13] Figure 13 below is the result of the superposition of the radial leakage surfaces (Sr1 and Sr2). In this figure, the leakage surfaces curves of our model are in blue colour and the curves of Abdelilah Lasri's model [13] are in red. Rotation angle of driver gear in degree pocketVolume in m b) Superposition of Pocket Volume Curves from our Model and those from the Diab's Model [10] Figure 14 below is the result of the superposition of pocket volumes. On this figure, the curve of pocket volumes from our modelis blue and the Diab's model curve [10] is black. The curves of the figures 13 and 14 and the relative deviations between the results from our model and the reference models allow us to state with certainty that the model developed in this work is valid and meets our set objectives. The model developed in this work allows us to calculate the exact values of the axial and radial leakage surfaces of the lubricant in a gear. # VI. Conclusion A better optimization of the power losses by the lubricant trapping in the inter-tooth space requires a preliminary work of total lifting of the veil on the gear inter-tooth space during the movement. In this perspective, we have established a purely analytical model allowing to accurately evaluating the radial and axial leakage surfaces of the lubricant in the inter-tooth space of external spur gears. This model was developed based on the parametric equations of a tooth profile and the exploitation of the involute properties, followed by the surface integrations delimited by the contour representing their exact boundary. The results are presented as curves of the evolution of the leakage surfaces (radial and axial) as a function of the driving gear's rotation angle. The curve of the evolution of the axial leakage surfaces as a function of the rotation angle is a symmetrical parabola, and the two curves of the evolution of the radial leakage surfaces are symmetrical (relative to each other). These results agree with the observation of the lubricant behavior in the inter-tooth space during gear movement. Far from numerical approximations, this model is an analytical formula allowing us to evaluate the exact leakage surfaces directly, according to the geometrical parameters of the gears. 1![Figure 1: Inter-tooth space and trapped lubricant b) Evolution of Radial and Axial Leakage SurfacesThe radial and axial leakage surfaces vary according to the angle of rotation. The further away from the initial position, the surfaces increase. Here, the initial position is the meeting point between the two pitch circles. The Figure2below illustrates the behavior of the leakage surfaces as a function of the angle of rotation from a) to h).](image-2.png "Figure 1 :") ![Establishment of an Analytical Model for Determining Leakage Surfaces in an External Tooth Spur Gear Global Journal of Researches in Engineering (A ) Volume Xx XII Issue II V ersion I](image-3.png "pinion") 2![Figure 2: Evolution of the leakage surfaces as a function of the rotation angle c) Coordinate System Linked to GearsThe pinion (driver) is associated to a fixed reference ??? ð??"ð??" , ?? ð??"ð??" , ?? ð??"ð??" , ?? ð??"ð??" ? and mobile reference (?? 1 , ?? 1 , ?? 1 , ?? 1 ), which revolves around (?? ð??"ð??" , ?? ð??"ð??" ) by an angle ?? 1 . Similarly, the gear (driven) is associated to fixed reference (?? ?? , ?? ?? , ?? ?? , ?? ?? ) and mobile reference (?? 2 , ?? 2 , ?? 2 , ?? 2 ) , which revolves around (?? ?? , ?? ?? ) by an angle ?? 2 . Such as?? 2 =?(?? 1 /?? 2 ) ?? 1 =?(?? 1 /?? 2 ) ?? 1 =?(?? ??1 /?? ??2 ) ?? 1 . Figure3below illustrates all these different references.](image-4.png "Figure 2 :") ![Figure 3 below illustrates all these different references. a) Location ?? 1 =0,4287 rad e) Location ?? 1 =-?? 1 =-0,0713 rad b) Location ?? 1 =0,3558 rad f) Location ?? 1 =-1493 rad c) Location ?? 1 =0,2392 rad g) Location ?? 1 =-0,3658 rad d) Location ?? 1 =0 rad h) Location ?? 1 = -0,4458 rad](image-5.png "") 3![Figure 3: Tracking of gear system](image-6.png "Figure 3 :") 4![below shows the detailed geometry of a 25-tooth gear.](image-7.png "Figure 4") 4![Figure 4: Geometry of an external spur gear e) Leakage Surface and Border Points at a given LocationIn a specific interval of the rotation angle, the profiles of the teeth meet, and consequently the radial leakage surfaces remain zero. Figure5below is a particular case. On this figure, C1 and C2 are the two contact points of the tooth profiles.](image-8.png "Figure 4 :") ![Gear pitch circles 1&2Establishment of an Analytical Model for Determining Leakage Surfaces in an External Tooth Spur Gear Global Journal of Researches in Engineering (A ) Volume Xx XII Issue](image-9.png "") 5![Figure 5: Leakage surface at a location where profiles are in contactWhen the profiles are not in contact, the radial leakage surfaces are non-zero and, consequently the axial leakage surface has as its boundary the tooth profiles and the minimum distances between the adjacent profiles. The figure6below is an illustration of this situation.](image-10.png "Figure 5 :") 6![Figure 6: Radial and axial leakage Surfaces at a location where profiles are not in contact f) Information Technology ToolsThe simulation of the equations and the model obtained was carried out with the MATLAB R2016A application installed in an HP computer, AMD A6-3400 APU HD Graphics 1.40 GHz; 6 GB of RAM.](image-11.png "Figure 6 :") 7![Figure 7: A calculation algorithm](image-12.png "Figure 7 :") ![i. Case where arccos(2r b *r p /(r b 2 + r p 2 )) ? ? max Equation of segment [BC] in (o, x, y) As a reminder, segment [BC] only exists when N<25 teeth. This segment equation requires knowledge of the coordinates of points B and C. According to figure 5, the coordinates of point B are given by the relation (4) below: With ? ?? = inv(?? 0 ) + ?? 1 and ??=k*((??/N)-? ?? ); 0