The Euler ecuation about the condition of unslip of theband on motor drum is:28μ ⋅αk f ⋅ S 4 = S 1 ⋅ e [N] (7)where k f [‐] is the safety coefficient for unslip onmotor drum (k f =1,2…1,3), e is the base of naturalslogarithms, μ [‐] is the friction coefficient between theband and the driven drum (μ=0,25…0,35) and α[rad]it is the angle of wrap up for the band on motor drum.With relations (1),…, (4) and (6) may be get:⋅[ qb⋅( 1+kî) + kî⋅qrg+ qî+ qrp][ q ⋅( 1−k) + q ]⎧w⋅cosβ⎫kf⋅L⋅⎨⎬sin b î îS⎩+β ⋅⎭1 = [N] (8)μ⋅αe −k⋅kSS +fic4 = k î ⋅S1[N] (9)k fThe reduce resistant moments for motor shaft may beobtioned with:( S −S)4 1 DTMrr= ⋅ [Nm] (10)η ⋅i2Rwhere the tensions in band S 1 and S 2 are fromexpressions (8) and (9).For horizontal transport conveyers, without deviationdrums when β=0 and from expressions (8) and (9)result:k f ⋅L⋅w⋅[ q b ⋅( 1+k î ) + k î ⋅q rg + q î + q rp ]S1 =[N] (11)eμ ⋅α− k f ⋅k î( 1+k )⎪⎧⎡qb⋅ î ⎤⎪⎫S4 = L ⋅⎨kî ⋅S1+ w ⋅ ⎢⎥⎬[N] (12)⎪⎩ ⎣+ kî⋅qrg+ qî+ qrp⎦⎪⎭The reduce resistance moments at motor shaft, maybe determinate with the formula (10) where S 1 and S 2are given by expression (11) and (12).The reduce resistance moments at shaft of drivenmotor, may be determinate for the belt transportconveyer with deviation drum is presented in fig.2.Fig.2. Belt inclinated transport conveyerwith deviation drumACTA TECHNICA CORVINIENSIS – Bulletin of EngineeringThe tensions in band, in points 1,…,8, for β>0 are:S 1 = S x [N] (13)SS 2 ≈ S 1 [N] (14)3 k î 1 ⋅ S 2= [N] (15)( q + q )S4= S3+ b rg ⋅L2⋅w⋅cosβ[N] (16)−q⋅L⋅sinβS = S +87b2S = î ⋅ [N] (17)5 k 1 S4S 6 ≈ S 5 [N] (18)S = î ⋅ [N] (19)7 k 2 S6( q + q + q )+b( q + q ) ⋅L⋅sinβbîîrp1⋅L1⋅wcos⋅ β[N] (20)where k î1 [‐] it is the band loading coefficient becausethe band passing over deviation drums (k î1 =1,02…1,03)and k î2 [‐] it is the band loading coefficient over returndrum (k î2 =1,07…1,09).The band loading that passing over deviation drumshave some coefficients values, because the angles ofwrap up of band on these drums are equal.The condition by unslip of band on motor drum is:μ ⋅αk f ⋅ S 8 = S 1 ⋅e(21)With these expressions (13),…,(21) may be get thenext ecuations:Sk f ⋅S A1 =e⋅α−k2⋅k î ⋅k î 1 2 fμ [N] (22)S = 28 S1⋅ k î 1 ⋅ k î 2 + S A [N] (23)where S A has this formula:⎛qb⋅( L1+ kî1⋅kî2 ⋅L2) ⎞SA= w⋅cosβ⋅⎜⎟qrgkî1kî2 L2L1( qîqrp)⎝+ ⋅ ⋅ ⋅ + ⋅ +⎠ (24)+ sinβ⋅ L ⋅ q + q −k⋅k⋅q⋅L( ( ))1bîî1For horizontal transport conveyer (β=0) with banddeviation drums, the tensions S 1 and S 8 from the bandare:k f ⋅SBS1 = [N] (25)μ ⋅α2e − k ⋅k⋅kî1î2bî 2S = 2S1⋅ k î 1 ⋅ k î 2 + S B8 [N] (26)where S B may be calculate with:S B⎡⎤⎢q b ⋅( L1+ k î 1⋅k î 2 ⋅L2)= w ⋅ ⎢ + q rg ⋅k î 1⋅k î 2 ⋅L2⎢(27)⎣+ L1⋅2( ) ⎥ ⎥⎥ q î + q rp ⎦For these two situations (β>0 and β=0) the reducedresistant moments at motor shaft may be computewith:( S8− S1) DTMrr= ⋅ [Nm] (28)η ⋅i2Rf2012. Fascicule 3 [July–September]
ACTA TECHNICA CORVINIENSIS – Bulletin of EngineeringIn the relations (10) and (28) i is the transmition ratioof reduction devices:Ωmi = (29)ΩTwhere Ω m [s ‐1 ] and Ω T [s ‐1 ] are the angular speeds of themotor and the driven drum.THE NECESSARY POWER CALCULATION FOR DRIVING THE BELTTRANSPORT CONVEYERSThe necessary power for driving the belt transportconveyer may be calculate with:− 3P = M ⋅ Ω ⋅ 10 ;PPTTT==MMrrrrrr⋅ i ⋅m⋅ i ⋅ ΩvRbTT⋅ 10⋅ 10− 3− 3; [kW] (30)where v b [m/s] is the band speed and R T [m] is the rayof driven drum.May be choise a motor which has the nominal speed n n[rot/min]:30⋅Ω nmn ≥ (31)πand the power:Pn ≥ P T(32)In continuation it is checking if the starting motormoment M p [Nm] is bigger than the reduced resistantmoment M rr [Nm] at shaft of driven motor. For this,from the motor catalog, it is determining the variationof the motor moment in function with the slip s[‐].The motor moment is giving by simplification ecuationof Kloss:⋅MkM = 2 s s(33)k+skswhere: M k [Nm] is the critical motor moment, s k [‐] ‐the slip at the critical moment and s[‐] is the motorslip. These size are calculating with:M = λ ⋅ M ;ssskkk= sMMkknPn= λ ⋅Ωn30 ⋅P= λ ⋅nkπ ⋅nn2n ⋅( λ + λ − 1 );n0− n=n0nΩ 0 − Ω n=Ω0n0− ns = ;n⋅;2( λ + λ − 1 );2⋅( λ + λ − 1 )0Ω 0 − Ωs =Ω0(34)(35)(36)n0− nnsn= ;n0(37)Ω 0 − Ω nsn=Ω 0In this relations:λ[‐] is the motor overload coefficient gave it in themotor catalog,P n [W] is the motor nominal power,n 0 [rot/min] and Ω 0 [s ‐1 ] are the syncronic speed,respective the angular speed proper at this speed,n n [rot/min] and Ω n [s ‐1 ] are the nominal speed,respective the angular speed,n [rot/min] and Ω [s ‐1 ] are the momentan speed,respective the angular speed ands k [‐], s n [‐] and s[‐] are the slip proper for the criticalmoment M k , nominal moment M n and currentmoment M.The motor starting moment M p [Nm] are calculatingwith sympliphicate formula of Kloss for s=1:Mp⋅M⋅s= 2 (38)1+k k2skThe motor may win the dynamic moment M d [Nm] if:M p >M rr (39)If this condition is not carries out, may be choise amotor with bigger power.CONCLUSIONSThis paper introduces on the base of investigationdone it on spatiality literature [1‐7], a quick calculationof necessary power for drive with triphasic cageinduction motors the inclined or horizontal belttransport conveyer, with and without deviationdrums.For inclined or horizontal belt transport conveyerwithout deviation drums, the necessary power ofdriven motor are calculating with (30), (8), (9), (11),(12) and (10), and for inclined or horizontal transportconveyer with deviation drums, the necessary powerof driven motor are calculating with (30), (28), (24),(22), (23) or (27), (26), (25) and (28) with carry out ofinequality (39), for these two constructive types.In this work may be establish the algorithm and thecomputing program of power driven motor for belttransport conveyer with small and medium capacity.REFERENCES[1.] N.V. Boțan ‐ The Base of Computing Electrical Drives(in Romanian), <strong>Technica</strong>l House, Bucharest, Romania,1970 (Bazele calculului acționărilor electrice, EdituraTehnică, Bucureşti, România, 1970).[2.] Al. Fransua, C. Saal, and I. Țopa ‐ Electrical Drives (inRomanian), Didactical and Pedagogical House,Bucharest, Romania, 1975 (Acționări electrice, EdituraDidactică şi Pedagogică, Bucureşti, România, 1975).2012. Fascicule 3 [July–September] 29
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