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BELTING                                                                              J 3010/6/1




      UNIT 6


BELTING




                                 OBJECTIVES




General Objective     : To understand and apply the concept of belting

Specific Objectives : At the end of this unit you will be able to:

                            state the difference between open and close belt.

                            explain that power transmitted by the flat belt and V belt.

                            explain that ratio tension for flat and V belt.

                            calculate power transmitted by the belt with consider
                             centrifugal force.
BELTING                                                                           J 3010/6/2




                                     INPUT



     6.0   INTRODUCTION



                                    In factories, the power has to be
                                    transmitted from one shaft to another,
                                    then belt driving between pulleys on
                                    the shafts may be used.




           The pulley rotating shaft is called driver. The pulley intended to rotate is
           known, as follower or driven. When the driver rotates, it carries the belt that
           grip between its surface and the belt. The belt, in turn, carries the driven
           pulley which starts rotating. The grip between the pulley and the belt is
           obtained by friction, which arises from pressure between the belt and the
           pulley.



           (a)     Types of belts

                           The flat belt is mostly used in the factories and work shops,
                   where a moderate amount of power is to be transmitted, from one
                   pulley to another, when the two pulleys are not more than 10 m a part.

                           The V-belt is mostly used in the factories and work shops
                   where a great amount of power is to be transmitted, from one pulley
                   to another, when the two pulleys are very near to each other.
BELTING                                                                                   J 3010/6/3




                            The types of belts:-

                           a.        flat belt
                           b.        V belt




     6.1       LENGTH OF AN OPEN BELT DRIVE



                                A


                                                                                 B
                       K
                                α1                                                    α2 C
                      O1                                                    O2
           F
                                                                                 r2
                                r1
                                                                                      D

                           E



                                                 d


                     Fig.6.1 Open belt drive


               O1 and O2 =       Centers of two pulleys
               r1 and r2   =     radius of the larger and smaller pulleys
                      d    =     Distance between O1 and O2
                      L    =     Total length of the belt.
               Angle AO1O2        = α1
               Angle BO2C         = α2
               Angle AFE          = θ1 (radian)
                   Angle BCD      = θ2 (radian)
BELTING                                            J 3010/6/4




            We know that the length of the belt,
              L = Arc AFE + ED + Arc DCB + BA

                        r1  r2
            Cos α1 =
                           d
                             r r
                  α1 = cos-1 1 2
                                d




             θ1 = 2π - 2α1
                = 2 (π - α1) (radian)

              θ2 = α1 = 2 α2 (radian)

            Arc AFE = r1θ1
            Arc DCB = r2θ2

          And ED = BA = KO2
                         KO2
                Sin α1 =
                          d
                  KO2 = d Sin α1

          Finally the total of length of belt,

          L = Arc AFE + ED + Arc DCB + BA
            = r1θ1 + d Sin α1 + r2θ2 + d Sin α1
           = r1θ1 + r2θ2 + 2d Sin α1
BELTING                                                                             J 3010/6/5


     Example 6.1


     Find the length of belt necessary to drive a pulley of 480 cm diameter running
     parallel at a distance of 12 meter from the driving pulley of diameter 80 cm. This
     system is an open belt drive.

     Solution 6.1


                            A

                                                                           B
                        K

          F                 α1                                          O2 α2       C
                       O1
                                                                               r2
                            r1                                                  D



                             E

                                           d

                     Fig.6.2 Open belt drive

              O1 and O2 = Centers of two pulleys
              r1 and r2 = radius of the larger and smaller pulleys
                     d  = Distance between O1 and O2
                     L   = Total length of the belt.
                Angle AO1O2 = α1
                Angle BO2C    = α2
                Angle AFE     = θ1 (radian)
                Angle BCD      = θ2 (radian)

                Radius of smaller pulley = 80/2 = 40 cm.
                Radius of larger pulley = 480/2 = 240 cm.
                Distance between the pulleys, d = 12m = 1 200 cm



              We know that the length of belt is,
               L = Arc AFE + ED + Arc DCB + BA

                            r1  r2   240  40
                 Cos α1 =           =
                               d       1200
BELTING                                              J 3010/6/6


                     240  40
          α1 = cos-1
                       1200
              = cos-1 0.16667
              = 80º
           α1 = 1.396 radian

            θ1 = 2π - 2α1
               = 2 (π - 1.396 ) (radian)
               = 3.491 radian

            θ2 = 2α1 = 2 α2 (radian)
               = 2 (1.396 )
               = 2.792 radian

           Arc AFE = r1θ1
                   = 240 x 3.491
                   = 837.84 cm

          Arc DCB = r2θ2
                  = 40 x 2.792
                  = 111.68 cm


          And ED = BA = KO2
                          KO2
                Sin 80º =
                           d
                  KO2 = d Sin α1 = 1 200 x 0.98481
                       = 1181.77 m

          Finally the total of belt length is

          L = Arc AFE + ED + Arc DCB + BA
            = r1θ1 + d Sin α1 + r2θ2 + d Sin α1
           = r1θ1 + r2θ2 + 2d Sin α1
           = 240 x 3.491 + 40 x 2.792 +2 x 1181.77
           = 837.84 + 111.68 + 2363.54
           = 3313.06 cm
           = 33.13 m
BELTING                                                                                J 3010/6/7


     6.2   LENGTH OF CLOSE BELT DRIVE




                          K


                      A
                                                                      D


                                                                                   C
               O1       α1                                          α2        O2
      F
                                                                              r2
                          r1
                                                                          B


                               E

                                             d


                                     Fig.6.3 Cross belt drive


           O1 and O2 =         Centers of two pulleys
             r1 and r2 =       radius of the larger and smaller pulleys
                  d    =       Distance between O1 and O2
                  L    =       Total length of the belt.
           Angle AO1O2          = α1
           Angle DO2O1          = α2
           Angle AFE            = θ1 (radian)
           Angle BCD            = θ2 (radian)

           We know that the length of the belt is
            L = Arc AFE + ED + Arc DCB + BA

                          r1  r2
            Cos α1 =
                             d
                                r r
                    α1 = cos-1 1 2
                                  d

             θ1 = 2π - 2α1
                = 2 (π - α1) (radian)

              θ1 = θ2
BELTING                                                                           J 3010/6/8


            Arc AFE = r1θ1
            Arc DCB = r2θ2

          And ED = BA = KO2
                        KO2
               Sin α1 =
                         d
                 KO2 = d Sin α1

          Finally the total of length belt,

          L = Arc AFE + ED + Arc DCB + BA
            = r1θ1 + d Sin α1 + r2θ2 + d Sin α1
            = r1θ1 + r2θ2 + 2d Sin α1




          Example 6.2

                   Find the length of belt for a cross belt drive system. The diameter of
                   the drive pulley is 480 cm which running parallel at a distance of 12
                   meter from the driving pulley which has a diameter of 80 cm.



          Solution 6.2
                         K


                              A
                                                                   D


                         α1                                       α2          C
      F       O1                                                       O2

                                                                       r2
                         r1
                                                                   B


                       E

                                          d



                                   Fig.6.4 Cross belt drive
BELTING                                                               J 3010/6/9




           O1 and O2 =     Centers of two pulleys
            r1 and r2 =    radius of the larger and smaller pulleys
                  d   =     distance between O1 and O2
                  L   =     Total length of the belt.
          Angle AO1O2       = α1
          Angle DO2O1      = α2
          Angle AFE        = θ1 (radian)
          Angle BCD         = θ2 (radian)

          Radius of smaller pulley        = 80/2  = 40 cm.
          Radius of larger pulley         = 480/2 = 240 cm.
          Distance between the pulleys, d = 12m   = 1 200 cm

          We know that the length of the belt,
          L = Arc AFE + ED + Arc DCB + BA

                     r1  r2 240  40
          Cos α1 =            =
                        d         1200
                             240  40
                α1 = cos-1
                               1200
                          -1
                   = cos 0.23333
                   = 76.5º
                α1 = 1.335 radian

           θ1 = 2π - 2α1
               = 2 (π - α1) (radian)
               = 2 (π - 1.335) (radian)
               = 3.613 radian

            θ1 = θ2

           Arc AFE = r1θ1
                   = 240 x 3.613
                   = 867.12 cm

           Arc DCB = r2θ2
                    = 40 x 3.613
                    = 144.52 cm
          And
               ED = BA = KO2
                        KO2
               Sin α1 =
                         d
                 KO2 = d Sin 76.5º =1 200 x 0.9724
             ED = BA = KO2 = 1166.88 cm
BELTING                                                           J 3010/6/10




          Finally the total of length belt,

           L=   Arc AFE + ED + Arc DCB + BA
            =   r1θ1 + d Sinα1 + r2θ2 + d Sin α1
            =   r1θ1 + r2θ2 + 2d Sin α1
            =   240 x 3.613 + 240 x 3.613 + 2 x 1 200 Sin 76.5º
            =    867.12 + 144.52 + 2333.76
            =    3345.4 cm
          L =    33.45 m
BELTING                                                                          J 3010/6/11




                          Activity 6A



     TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE WITH THE
     NEXT INPUT…!


     6.1   Two pulleys, one with a 450 mm diameter and the other with a 200 mm
           diameter are on parallel shaft of 1.95 m apart and are connected by a cross
           belt. Find the length of the belt required and the angle of contact between
           the belt and each pulley.

     6.2   It is required to drive a shaft B at 620 rpm by means of a belt from a parallel
           shaft A. A pulley of 30 cm diameter on shaft A runs at 240 rpm. Determine
           the size of pulley on the shaft B.

     6.3   Find the length of belt necessary to drive a pulley of 1.4 m diameter running
           parallel at a distance of 1.7 meter from the driving pulley of diameter 0.5 m.
           It is connected by an open belt.



                                         N1 d 2
                                            
                                         N 2 d1
                          N1 = speed diver in rpm
                          N2 = speed follower in rpm
                          d1 ,d2 = diameter pulley driver and
                                   follower.
BELTING                                                                   J 3010/6/12




                                 Feedback to Activity 6A



     Have you tried the questions????? If “YES”, check your answers now



            6.1    4.975 m; 199 or 3.473 radian.

            6.2.   11.6 cm

            6.3    6.51 m
BELTING                                                                         J 3010/6/13




                                   INPUT


     6.3   POWER TRANSMITTED BY A BELT




                                          Power = (T1 –T2) v
                                  Where, T1 =Tension in tight side
                                              in Newton.
                                        T2 = Tension in slack side.
                                         V = velocity of belt




           Fig. 6.5, shows the driving pulley (i.e., driver) A and the follower B.
           The driving pulley pulls the belt from one side, and delivers the same to the
           other.The maximum tension in the tight side will be greater than that
           slack side.




                                Fig. 6.5
                  Torque exerted on the driving pulley
                         = ( T1 - T2) r1
                  Torque exerted on the driven or follower
                         = ( T1 - T2) r2
                  Power transmitted = Force x distance
                                    = ( T1 - T2) v
BELTING                                                                       J 3010/6/14


          Example 6.3

          The tension in the two sides of the belt are 100 N and 80 N respectively. If
          the speed of the belt is 75 meters per second. Find the power transmitted by
          the belt.

          Solution 6.3

                 Given,
                 Tension in tight side,
                      T1 = 100 N
                 Tension in slack side,
                       T2 = 80 N
                 Velocity of belt, v = 75 m/s
                 Let P = Power transmitted by the belt
                 Using the relation,
                 Power = (T1 –T2) v
                        = ( 100 – 80) 75
                        = 1500 watt
                        = 1.5 kw.
BELTING                                                                           J 3010/6/15




                            Activity 6B




     TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE WITH THE
     NEXT INPUT…!

     6.4.   Find the tension in the tight side, if the tension in slack side 150 N. The speed
            of the belt is 58 meters per second and the power transmitted by this
            belt is 2 kw.

     6.5    Diameter of driver is 50 mm. If the driver transmits 8 kw when it is rotating
            at 300 rev/ min. Calculate velocity of driver.

     6.6    The tension in the two sides of the belt are 300 N and 180 N respectively. If
            the speed of the belt is 50 meters per second, find the initial tension and
            power transmitted by the belt.

     6.7    A 100 mm diameter pulley is belt-driven from a 400 mm diameter pulley.
            The 400 mm pulley rotates at 480 rev/min. The number of rev/sec of the
            100 mm diameter pulley is
            A. 2        B. 32            C. 120        D. 1920




                                            T1  T2
                                     T0 =
                                               2
                   Where,     T0 = Initial tension in the belt.
BELTING                                                                   J 3010/6/16




                       Feedback to Activity 6B



           Have you tried the questions????? If “YES”, check your answers now



     6.4   115.5 N

     6.5   0.785 m/s

     6.6   6 000 watt or 6 kw; 240 N

     6.7   B. 32
BELTING                                                                          J 3010/6/17




                                     INPUT




     6.4   RATIO OF TENSIONS.




                          Fig. 6.6

           Consider a driven pulley rotating in the clockwise direction as in fig 6.6.
           Let T1 = Tension in the belt on the tight side.
                T2 = Tension in the belt on the slack side.
                 ө = An angle of contact in radians (i.e , angle subtended by the arc
                       AB, along which the belt touches the pulley, at the centre)

           Now consider a small position of the belt PQ, subtending an angle  at the
           centre of the pulley as shown fig 6.6. The belt PQ is in equilibrium under the
           following force:
           i. Tension T in the belt at P.
           ii. Tension T + T in the belt at Q.
           iii. Normal reaction R, and
           iv. Frictional force F =  x R

           Where  is the coefficient of friction between the belt and pulley.
           Resolving all the forces horizontally and equating the same,
BELTING                                                                               J 3010/6/18


                                         
          R = ( T + T) sin      + T sin                  (6.1)
                              2             2
          Since the  is very small, therefore, substituting,
                   
          sin     =       in equation 6.1
               2      2
                                   
           R = ( T + T)          +T
                              2        2
                  T       T      T .
              =          +         +
                    2         2          2
                                     T 
              = T. ( neglecting              )       (6.2)
                                         2
          Now resolving the forces vertically,
                                                  
             x R = (T + T) cos            - T cos          (6.3)
                                       2             2
                                                                                
          Since the angle . is very small, therefore substituting cos            = 1 in
                                                                                 2
          equation 6.3 or,          xR      = T + T – T = T
                                               T
                                           R =             (6.4)
                                                 
          Equating the values of R from equation 6.2 and 6.4,
                              T
          Or        T. =
                                       
                        T
          Or                    =      .
                        T
          Integrating both sides from A to B,

                                
                       T
                  T1

                  T
                  T2
                               
                                0

                              T1
          or           loge      = 
                              T2
                              T1
                                 = e           ration of tension for flat belt
                              T2
                              T1
                                 = e /sin     ration of tension for V belt
                              T2
                                       where  = half angle of groove
BELTING                                                                        J 3010/6/19


          Example 6.4

          Find the power transmitted by a belt running over a pulley of 60 cm diameter
          at 200 rpm. The coefficient of friction between the pulley is 0.25, angle of lap
          160 and maximum tension in the belt is 250 KN.

          Solution 6.4

          Given,
          Diameter of pulley, d = 60 cm = 0.6 m
          Speed of pulley        N = 200 rpm
                                dN      x 0.6 x 200
          Speed of belt, v =          =                = 2 = 6.28 m/ sec
                                 60          60
          Coefficient of friction,
              μ = 0.25
                                               160 x 
                 Angle of contact,  = 160 =            = 2.7926 radian.
                                                 180
                 Maximum tension in the belt,
                          T1 = 250 kN
                 Let      P = power transmitted by the belt.
                 Using the relation,
                          T1
                               = e 
                          T2
                              = e 0.25 x 2.7926
                         T1
                              = 2.01
                         T2
                  T1       250
          T2 =         =        = 124.38 kN
                 2.01     2.01
          Now using the relation,
                P = (T1 –T2 ) v
                   = ( 250 - 124.38 ) 6.28
                   = 788.89 watt
                 P = 0.79 kw
BELTING                                                                          J 3010/6/20




                                   INPUT




     6.5   CENTRIFUGAL TENSION.




                                  Fig.6.7



           The tension caused by centrifugal force is called centrifugal tension. At lower
           speeds the centrifugal tension is very small, but at higher speeds its effect is
           considerable, and thus should be taken into account.
           Consider a small portion PQ of the belt subtending an angle d at the centre
           of the pulley as show in fig 6.7.

           Let       M = mass of the belt per unit length,
                     V = linear velocity of the belt,
                      r = radius of the pulley over which the belt runs,
                      Tc = Centrifugal tension acting tangentially at P and Q.
           Length of the belt PQ,
                          = r d
           Mass of the belt PQ,
                       M = M r d
           We know that centrifugal force,
                          = M v2/r
BELTING                                                                        J 3010/6/21


          Centrifugal force of the belt PQ
                              M x r.d v 2
                          =
                                   r
                          = M x d v 2
          The centrifugal tension (Tc) acting tangentially at P and Q keeps the belt in
          equilibrium.
          Now resolving the force (i.e, centrifugal force and centrifugal tension)
          horizontally and equating the same,
                       d
              2 Tc sin      = M x d v 2
                        2
          since angle d is very small, therefore, substituting
                    d        d
               sin        =
                     2         2
                   d
             2 Tc         = M x d v 2
                    2
                   Tc     = M x d v 2 / d
                    Tc    = M v2

          T1  Tc
                   e        ratio tension for flat belt.
          T2  Tc
          T1  Tc
                   e   / sin  ratio tension for V belt
          T2  Tc




          6.5.1   Condition for the transmission of maximum power

          The maximum power,
            When T c = ⅓T1

          It shows that the power transmitted is maximum ⅓ of the maximum tension
          is absorbed as centrifugal tension.
                  The velocity of belt for maximum transmission of power may be
          obtained from equation T1 = 3Tc = M v2.
BELTING                                                                        J 3010/6/22


                                3 T1
                         v2 =
                                 M
                                   T1
                         v =
                                  3M


          Example 6.5

          An open belt drive connects two pulleys 1.2 m and 0.5 m diameter, on
          parallel shafts 3.6 m apart. The belt has a mass of 0.9 kg/m length and the
          maximum tension in it is not exceed 2 kN. The larger pulley runs at 200
          rev/min. Calculate the torque on each of the two shafts and the power
          transmitted. Coefficient of friction is 0.3 and angle of lap on the smaller
          pulley is 168° ( 2.947 radian ).

          Solution 6.5

          Given
          Diameter of larger pulley,
                                d1 = 1.2 m
          Radius of the larger pulley,
                                  r1 = 0.6
          Diameter of smaller pulley,
                                  d2 =0.5 m
          Radius of the smaller pulley,
                                   r2 = 0.25 m
          Distance between two shaft,
                                  D = 3.6 m
          Mass of the belt per meter length,
                                  M = 0.9 kg/m
          Maximum Tension, T1 = 2 kN = 2 000 N
          Speed of the larger pulley
                                  = 200 rpm
          Velocity of the belt,
                                 x 1.2 x 200
                         V=                    = 12.57 m/s
                                      60
          T c = Mv2
              = 0.9 x 12.572
              = 142.2 N
BELTING                                                              J 3010/6/23




          e µθ = e 0.3 x 2.947
               = 2.421

          Using the relation,
                  T1  Tc
                            e
                  T2  Tc
                    2000  142.2
                                 = 2.421
                    T2  142.2
                      (T2 – 142.2) 2.421 = 1857.8
                                           1857.8
                            (T2 – 142.2) =        = 767.37
                                            2.421
                                      T2 = 767.37 + 142.2
                                      T2 = 909.57 N

          We know that the torque on the larger pulley shaft (TL),
                        TL = ( T1 – T2) r1
                             = ( 2000 – 909.57) 0.6
                             = 654.26 Nm.
          Torque on the smaller pulley shaft (Ts),
                         Ts = ( T1 – T2) r2
                             = (2000 – 909.57) 0.25
                             = 272.61 Nm.
          Power transmitted, P = ( T1 – T2)v
                               = ( 2000 – 909.57) 12.57
                                = 13706.71 watt
                                = 13.71 kw
BELTING                                                                           J 3010/6/24




                         Activity 6C




     TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE TO THE NEXT
     INPUT…!



     6.8     Two pulleys, one with a 450 mm diameter and the other with a 200 mm
             diameter are on parallel of shafts 1.95 m apart. What power can be
             transmitted by the belt when the larger pulley rotates at 200 rev/min, if the
             maximum permissible tension in the belt is 1 kN and the coefficient of
             friction between the belt and pulley is 0.25. Angle of contact between the belt
             and larger pulley is 3.477 radian.

     6.9    Find the power transmitted by a V drive from the following data:

            Angle of contact                =   84º
            Pulley groove angle             =    45º
            Coefficient of friction         =   0.25
            Mass of belt per meter length   =   0.472 kg/m
            Permissible tension             =   139 N
            Velocity of V belt              =   12.57 m/s.



     6.10    An open belt drive connects two pulleys 1.2 m and 0.6 m, on parallel shafts 3
            m apart. The belt has a mass 0f 0.56 kg/m and maximum tension is 1.5 kN. The
            driver pulley runs at 300 rev/min. Calculate the inertial tension, power
            transmitted and maximum power. The coefficient of friction between the belt
            and the pulley surface is 0.3.
BELTING                                                                   J 3010/6/25




                                    Feedback to Activity 6C



     Have you tried the questions????? If “YES”, check your answers now



      6.8   2 740 watt or 2.74 kw



     6.9     591 watt.



     6.10    1074.5 N ; 8.0 kw ; 17.54 kw.
BELTING                                                                           J 3010/6/26




                           SELF-ASSESSMENT 6



     You are approaching success. Try all the questions in this self-assessment section
     and check your answers with those given in the Feedback on Self-Assessment 6
     given on the next page. If you face any problems, discuss it with your lecturer.
     Good luck.

     1.     A pulley is driven by a flat belt running at speed of 600 m/min. The
            coefficient of friction between the pulley and the belt is 0.3 and the angle lap
            is 160°. If the maximum tension in the belt is 700 N, find the power
            transmitted by a belt.

     2.    A leather belt, 125 mm wide and 6 mm thick, transmits power from a pulley
           of 750 mm diameter which run at 500 rpm. The angle of lap is 150° and
            µ = 0.3. If the mass of 1 m3 of leather is 1 Mg and the stress in the belt does
           not exceed 2.75 MN/m2, find the maximum power that can be transmitted.

     3.    A flat belt, 8 mm thick and 100 mm wide transmits power between two
           pulleys, running at 1 600 m/min. The mass of the belt is 0.9 kg/m length. The
           angle of lap in the smaller pulley is 165° and the coefficient of friction
           between the belt and pulleys is 0.3. If the maximum permissible stress in the
           belt is 2 MN/m2, find

           (i)     Maximum power transmitted; and

           (ii)    Initial tension in the belt.

     4.     The moment on a pulley, which produces the rotation of the pulley is called:
            A. Momentum         B. Torque     C. Work         D. Energy

     5.     If T1 and T2 are the tension in the tight and slack sides of a belt and θ is the
            angle of contact between the belt and pulley. Coefficient of friction is μ, then
            the ratio of driving tension will be:
                 T                T              T                      T
            A. 2  e   B. 1  e   C. 1                 D. log10 1  
                 T1              T2              T2                     T2
BELTING                                                                    J 3010/6/27




                           Feedback to Self-Assessment 6




     Have you tried the questions????? If “YES”, check your answers now.



     1. 3.974 kw ( see example 6.4)



     2. 18.97 kw



     3.   (i) 14.281 kw

          (ii) 1.3221 kN

     4.   B. Torque

               T1
     5.   B.       e                         CONGRATULATIONS!!!!…..
               T2                               May success be with you
                                                always….

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J3010 Unit 6

  • 1. BELTING J 3010/6/1 UNIT 6 BELTING OBJECTIVES General Objective : To understand and apply the concept of belting Specific Objectives : At the end of this unit you will be able to:  state the difference between open and close belt.  explain that power transmitted by the flat belt and V belt.  explain that ratio tension for flat and V belt.  calculate power transmitted by the belt with consider centrifugal force.
  • 2. BELTING J 3010/6/2 INPUT 6.0 INTRODUCTION In factories, the power has to be transmitted from one shaft to another, then belt driving between pulleys on the shafts may be used. The pulley rotating shaft is called driver. The pulley intended to rotate is known, as follower or driven. When the driver rotates, it carries the belt that grip between its surface and the belt. The belt, in turn, carries the driven pulley which starts rotating. The grip between the pulley and the belt is obtained by friction, which arises from pressure between the belt and the pulley. (a) Types of belts The flat belt is mostly used in the factories and work shops, where a moderate amount of power is to be transmitted, from one pulley to another, when the two pulleys are not more than 10 m a part. The V-belt is mostly used in the factories and work shops where a great amount of power is to be transmitted, from one pulley to another, when the two pulleys are very near to each other.
  • 3. BELTING J 3010/6/3 The types of belts:- a. flat belt b. V belt 6.1 LENGTH OF AN OPEN BELT DRIVE A B K α1 α2 C O1 O2 F r2 r1 D E d Fig.6.1 Open belt drive O1 and O2 = Centers of two pulleys r1 and r2 = radius of the larger and smaller pulleys d = Distance between O1 and O2 L = Total length of the belt. Angle AO1O2 = α1 Angle BO2C = α2 Angle AFE = θ1 (radian) Angle BCD = θ2 (radian)
  • 4. BELTING J 3010/6/4 We know that the length of the belt, L = Arc AFE + ED + Arc DCB + BA r1  r2 Cos α1 = d r r α1 = cos-1 1 2 d θ1 = 2π - 2α1 = 2 (π - α1) (radian) θ2 = α1 = 2 α2 (radian) Arc AFE = r1θ1 Arc DCB = r2θ2 And ED = BA = KO2 KO2 Sin α1 = d KO2 = d Sin α1 Finally the total of length of belt, L = Arc AFE + ED + Arc DCB + BA = r1θ1 + d Sin α1 + r2θ2 + d Sin α1 = r1θ1 + r2θ2 + 2d Sin α1
  • 5. BELTING J 3010/6/5 Example 6.1 Find the length of belt necessary to drive a pulley of 480 cm diameter running parallel at a distance of 12 meter from the driving pulley of diameter 80 cm. This system is an open belt drive. Solution 6.1 A B K F α1 O2 α2 C O1 r2 r1 D E d Fig.6.2 Open belt drive O1 and O2 = Centers of two pulleys r1 and r2 = radius of the larger and smaller pulleys d = Distance between O1 and O2 L = Total length of the belt. Angle AO1O2 = α1 Angle BO2C = α2 Angle AFE = θ1 (radian) Angle BCD = θ2 (radian) Radius of smaller pulley = 80/2 = 40 cm. Radius of larger pulley = 480/2 = 240 cm. Distance between the pulleys, d = 12m = 1 200 cm We know that the length of belt is, L = Arc AFE + ED + Arc DCB + BA r1  r2 240  40 Cos α1 = = d 1200
  • 6. BELTING J 3010/6/6 240  40 α1 = cos-1 1200 = cos-1 0.16667 = 80º α1 = 1.396 radian θ1 = 2π - 2α1 = 2 (π - 1.396 ) (radian) = 3.491 radian θ2 = 2α1 = 2 α2 (radian) = 2 (1.396 ) = 2.792 radian Arc AFE = r1θ1 = 240 x 3.491 = 837.84 cm Arc DCB = r2θ2 = 40 x 2.792 = 111.68 cm And ED = BA = KO2 KO2 Sin 80º = d KO2 = d Sin α1 = 1 200 x 0.98481 = 1181.77 m Finally the total of belt length is L = Arc AFE + ED + Arc DCB + BA = r1θ1 + d Sin α1 + r2θ2 + d Sin α1 = r1θ1 + r2θ2 + 2d Sin α1 = 240 x 3.491 + 40 x 2.792 +2 x 1181.77 = 837.84 + 111.68 + 2363.54 = 3313.06 cm = 33.13 m
  • 7. BELTING J 3010/6/7 6.2 LENGTH OF CLOSE BELT DRIVE K A D C O1 α1 α2 O2 F r2 r1 B E d Fig.6.3 Cross belt drive O1 and O2 = Centers of two pulleys r1 and r2 = radius of the larger and smaller pulleys d = Distance between O1 and O2 L = Total length of the belt. Angle AO1O2 = α1 Angle DO2O1 = α2 Angle AFE = θ1 (radian) Angle BCD = θ2 (radian) We know that the length of the belt is L = Arc AFE + ED + Arc DCB + BA r1  r2 Cos α1 = d r r α1 = cos-1 1 2 d θ1 = 2π - 2α1 = 2 (π - α1) (radian) θ1 = θ2
  • 8. BELTING J 3010/6/8 Arc AFE = r1θ1 Arc DCB = r2θ2 And ED = BA = KO2 KO2 Sin α1 = d KO2 = d Sin α1 Finally the total of length belt, L = Arc AFE + ED + Arc DCB + BA = r1θ1 + d Sin α1 + r2θ2 + d Sin α1 = r1θ1 + r2θ2 + 2d Sin α1 Example 6.2 Find the length of belt for a cross belt drive system. The diameter of the drive pulley is 480 cm which running parallel at a distance of 12 meter from the driving pulley which has a diameter of 80 cm. Solution 6.2 K A D α1 α2 C F O1 O2 r2 r1 B E d Fig.6.4 Cross belt drive
  • 9. BELTING J 3010/6/9 O1 and O2 = Centers of two pulleys r1 and r2 = radius of the larger and smaller pulleys d = distance between O1 and O2 L = Total length of the belt. Angle AO1O2 = α1 Angle DO2O1 = α2 Angle AFE = θ1 (radian) Angle BCD = θ2 (radian) Radius of smaller pulley = 80/2 = 40 cm. Radius of larger pulley = 480/2 = 240 cm. Distance between the pulleys, d = 12m = 1 200 cm We know that the length of the belt, L = Arc AFE + ED + Arc DCB + BA r1  r2 240  40 Cos α1 = = d 1200 240  40 α1 = cos-1 1200 -1 = cos 0.23333 = 76.5º α1 = 1.335 radian θ1 = 2π - 2α1 = 2 (π - α1) (radian) = 2 (π - 1.335) (radian) = 3.613 radian θ1 = θ2 Arc AFE = r1θ1 = 240 x 3.613 = 867.12 cm Arc DCB = r2θ2 = 40 x 3.613 = 144.52 cm And ED = BA = KO2 KO2 Sin α1 = d KO2 = d Sin 76.5º =1 200 x 0.9724 ED = BA = KO2 = 1166.88 cm
  • 10. BELTING J 3010/6/10 Finally the total of length belt, L= Arc AFE + ED + Arc DCB + BA = r1θ1 + d Sinα1 + r2θ2 + d Sin α1 = r1θ1 + r2θ2 + 2d Sin α1 = 240 x 3.613 + 240 x 3.613 + 2 x 1 200 Sin 76.5º = 867.12 + 144.52 + 2333.76 = 3345.4 cm L = 33.45 m
  • 11. BELTING J 3010/6/11 Activity 6A TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE WITH THE NEXT INPUT…! 6.1 Two pulleys, one with a 450 mm diameter and the other with a 200 mm diameter are on parallel shaft of 1.95 m apart and are connected by a cross belt. Find the length of the belt required and the angle of contact between the belt and each pulley. 6.2 It is required to drive a shaft B at 620 rpm by means of a belt from a parallel shaft A. A pulley of 30 cm diameter on shaft A runs at 240 rpm. Determine the size of pulley on the shaft B. 6.3 Find the length of belt necessary to drive a pulley of 1.4 m diameter running parallel at a distance of 1.7 meter from the driving pulley of diameter 0.5 m. It is connected by an open belt. N1 d 2  N 2 d1 N1 = speed diver in rpm N2 = speed follower in rpm d1 ,d2 = diameter pulley driver and follower.
  • 12. BELTING J 3010/6/12 Feedback to Activity 6A Have you tried the questions????? If “YES”, check your answers now 6.1 4.975 m; 199 or 3.473 radian. 6.2. 11.6 cm 6.3 6.51 m
  • 13. BELTING J 3010/6/13 INPUT 6.3 POWER TRANSMITTED BY A BELT Power = (T1 –T2) v Where, T1 =Tension in tight side in Newton. T2 = Tension in slack side. V = velocity of belt Fig. 6.5, shows the driving pulley (i.e., driver) A and the follower B. The driving pulley pulls the belt from one side, and delivers the same to the other.The maximum tension in the tight side will be greater than that slack side. Fig. 6.5 Torque exerted on the driving pulley = ( T1 - T2) r1 Torque exerted on the driven or follower = ( T1 - T2) r2 Power transmitted = Force x distance = ( T1 - T2) v
  • 14. BELTING J 3010/6/14 Example 6.3 The tension in the two sides of the belt are 100 N and 80 N respectively. If the speed of the belt is 75 meters per second. Find the power transmitted by the belt. Solution 6.3 Given, Tension in tight side, T1 = 100 N Tension in slack side, T2 = 80 N Velocity of belt, v = 75 m/s Let P = Power transmitted by the belt Using the relation, Power = (T1 –T2) v = ( 100 – 80) 75 = 1500 watt = 1.5 kw.
  • 15. BELTING J 3010/6/15 Activity 6B TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE WITH THE NEXT INPUT…! 6.4. Find the tension in the tight side, if the tension in slack side 150 N. The speed of the belt is 58 meters per second and the power transmitted by this belt is 2 kw. 6.5 Diameter of driver is 50 mm. If the driver transmits 8 kw when it is rotating at 300 rev/ min. Calculate velocity of driver. 6.6 The tension in the two sides of the belt are 300 N and 180 N respectively. If the speed of the belt is 50 meters per second, find the initial tension and power transmitted by the belt. 6.7 A 100 mm diameter pulley is belt-driven from a 400 mm diameter pulley. The 400 mm pulley rotates at 480 rev/min. The number of rev/sec of the 100 mm diameter pulley is A. 2 B. 32 C. 120 D. 1920 T1  T2 T0 = 2 Where, T0 = Initial tension in the belt.
  • 16. BELTING J 3010/6/16 Feedback to Activity 6B Have you tried the questions????? If “YES”, check your answers now 6.4 115.5 N 6.5 0.785 m/s 6.6 6 000 watt or 6 kw; 240 N 6.7 B. 32
  • 17. BELTING J 3010/6/17 INPUT 6.4 RATIO OF TENSIONS. Fig. 6.6 Consider a driven pulley rotating in the clockwise direction as in fig 6.6. Let T1 = Tension in the belt on the tight side. T2 = Tension in the belt on the slack side. ө = An angle of contact in radians (i.e , angle subtended by the arc AB, along which the belt touches the pulley, at the centre) Now consider a small position of the belt PQ, subtending an angle  at the centre of the pulley as shown fig 6.6. The belt PQ is in equilibrium under the following force: i. Tension T in the belt at P. ii. Tension T + T in the belt at Q. iii. Normal reaction R, and iv. Frictional force F =  x R Where  is the coefficient of friction between the belt and pulley. Resolving all the forces horizontally and equating the same,
  • 18. BELTING J 3010/6/18   R = ( T + T) sin + T sin (6.1) 2 2 Since the  is very small, therefore, substituting,   sin = in equation 6.1 2 2   R = ( T + T) +T 2 2 T  T  T . = + + 2 2 2 T  = T. ( neglecting ) (6.2) 2 Now resolving the forces vertically,    x R = (T + T) cos - T cos (6.3) 2 2  Since the angle . is very small, therefore substituting cos = 1 in 2 equation 6.3 or, xR = T + T – T = T T R = (6.4)  Equating the values of R from equation 6.2 and 6.4, T Or T. =  T Or = . T Integrating both sides from A to B,  T T1 T T2     0 T1 or loge =  T2 T1 = e  ration of tension for flat belt T2 T1 = e /sin  ration of tension for V belt T2 where  = half angle of groove
  • 19. BELTING J 3010/6/19 Example 6.4 Find the power transmitted by a belt running over a pulley of 60 cm diameter at 200 rpm. The coefficient of friction between the pulley is 0.25, angle of lap 160 and maximum tension in the belt is 250 KN. Solution 6.4 Given, Diameter of pulley, d = 60 cm = 0.6 m Speed of pulley N = 200 rpm  dN  x 0.6 x 200 Speed of belt, v = = = 2 = 6.28 m/ sec 60 60 Coefficient of friction, μ = 0.25 160 x  Angle of contact,  = 160 = = 2.7926 radian. 180 Maximum tension in the belt, T1 = 250 kN Let P = power transmitted by the belt. Using the relation, T1 = e  T2 = e 0.25 x 2.7926 T1 = 2.01 T2 T1 250 T2 = = = 124.38 kN 2.01 2.01 Now using the relation, P = (T1 –T2 ) v = ( 250 - 124.38 ) 6.28 = 788.89 watt P = 0.79 kw
  • 20. BELTING J 3010/6/20 INPUT 6.5 CENTRIFUGAL TENSION. Fig.6.7 The tension caused by centrifugal force is called centrifugal tension. At lower speeds the centrifugal tension is very small, but at higher speeds its effect is considerable, and thus should be taken into account. Consider a small portion PQ of the belt subtending an angle d at the centre of the pulley as show in fig 6.7. Let M = mass of the belt per unit length, V = linear velocity of the belt, r = radius of the pulley over which the belt runs, Tc = Centrifugal tension acting tangentially at P and Q. Length of the belt PQ, = r d Mass of the belt PQ, M = M r d We know that centrifugal force, = M v2/r
  • 21. BELTING J 3010/6/21 Centrifugal force of the belt PQ M x r.d v 2 = r = M x d v 2 The centrifugal tension (Tc) acting tangentially at P and Q keeps the belt in equilibrium. Now resolving the force (i.e, centrifugal force and centrifugal tension) horizontally and equating the same, d 2 Tc sin = M x d v 2 2 since angle d is very small, therefore, substituting d d sin = 2 2 d 2 Tc = M x d v 2 2 Tc = M x d v 2 / d Tc = M v2 T1  Tc  e ratio tension for flat belt. T2  Tc T1  Tc  e   / sin  ratio tension for V belt T2  Tc 6.5.1 Condition for the transmission of maximum power The maximum power, When T c = ⅓T1 It shows that the power transmitted is maximum ⅓ of the maximum tension is absorbed as centrifugal tension. The velocity of belt for maximum transmission of power may be obtained from equation T1 = 3Tc = M v2.
  • 22. BELTING J 3010/6/22 3 T1 v2 = M T1 v = 3M Example 6.5 An open belt drive connects two pulleys 1.2 m and 0.5 m diameter, on parallel shafts 3.6 m apart. The belt has a mass of 0.9 kg/m length and the maximum tension in it is not exceed 2 kN. The larger pulley runs at 200 rev/min. Calculate the torque on each of the two shafts and the power transmitted. Coefficient of friction is 0.3 and angle of lap on the smaller pulley is 168° ( 2.947 radian ). Solution 6.5 Given Diameter of larger pulley, d1 = 1.2 m Radius of the larger pulley, r1 = 0.6 Diameter of smaller pulley, d2 =0.5 m Radius of the smaller pulley, r2 = 0.25 m Distance between two shaft, D = 3.6 m Mass of the belt per meter length, M = 0.9 kg/m Maximum Tension, T1 = 2 kN = 2 000 N Speed of the larger pulley = 200 rpm Velocity of the belt,  x 1.2 x 200 V= = 12.57 m/s 60 T c = Mv2 = 0.9 x 12.572 = 142.2 N
  • 23. BELTING J 3010/6/23 e µθ = e 0.3 x 2.947 = 2.421 Using the relation, T1  Tc  e T2  Tc 2000  142.2 = 2.421 T2  142.2 (T2 – 142.2) 2.421 = 1857.8 1857.8 (T2 – 142.2) = = 767.37 2.421 T2 = 767.37 + 142.2 T2 = 909.57 N We know that the torque on the larger pulley shaft (TL), TL = ( T1 – T2) r1 = ( 2000 – 909.57) 0.6 = 654.26 Nm. Torque on the smaller pulley shaft (Ts), Ts = ( T1 – T2) r2 = (2000 – 909.57) 0.25 = 272.61 Nm. Power transmitted, P = ( T1 – T2)v = ( 2000 – 909.57) 12.57 = 13706.71 watt = 13.71 kw
  • 24. BELTING J 3010/6/24 Activity 6C TEST YOUR UNDERSTANDING BEFORE YOU CONTINUE TO THE NEXT INPUT…! 6.8 Two pulleys, one with a 450 mm diameter and the other with a 200 mm diameter are on parallel of shafts 1.95 m apart. What power can be transmitted by the belt when the larger pulley rotates at 200 rev/min, if the maximum permissible tension in the belt is 1 kN and the coefficient of friction between the belt and pulley is 0.25. Angle of contact between the belt and larger pulley is 3.477 radian. 6.9 Find the power transmitted by a V drive from the following data: Angle of contact = 84º Pulley groove angle = 45º Coefficient of friction = 0.25 Mass of belt per meter length = 0.472 kg/m Permissible tension = 139 N Velocity of V belt = 12.57 m/s. 6.10 An open belt drive connects two pulleys 1.2 m and 0.6 m, on parallel shafts 3 m apart. The belt has a mass 0f 0.56 kg/m and maximum tension is 1.5 kN. The driver pulley runs at 300 rev/min. Calculate the inertial tension, power transmitted and maximum power. The coefficient of friction between the belt and the pulley surface is 0.3.
  • 25. BELTING J 3010/6/25 Feedback to Activity 6C Have you tried the questions????? If “YES”, check your answers now 6.8 2 740 watt or 2.74 kw 6.9 591 watt. 6.10 1074.5 N ; 8.0 kw ; 17.54 kw.
  • 26. BELTING J 3010/6/26 SELF-ASSESSMENT 6 You are approaching success. Try all the questions in this self-assessment section and check your answers with those given in the Feedback on Self-Assessment 6 given on the next page. If you face any problems, discuss it with your lecturer. Good luck. 1. A pulley is driven by a flat belt running at speed of 600 m/min. The coefficient of friction between the pulley and the belt is 0.3 and the angle lap is 160°. If the maximum tension in the belt is 700 N, find the power transmitted by a belt. 2. A leather belt, 125 mm wide and 6 mm thick, transmits power from a pulley of 750 mm diameter which run at 500 rpm. The angle of lap is 150° and µ = 0.3. If the mass of 1 m3 of leather is 1 Mg and the stress in the belt does not exceed 2.75 MN/m2, find the maximum power that can be transmitted. 3. A flat belt, 8 mm thick and 100 mm wide transmits power between two pulleys, running at 1 600 m/min. The mass of the belt is 0.9 kg/m length. The angle of lap in the smaller pulley is 165° and the coefficient of friction between the belt and pulleys is 0.3. If the maximum permissible stress in the belt is 2 MN/m2, find (i) Maximum power transmitted; and (ii) Initial tension in the belt. 4. The moment on a pulley, which produces the rotation of the pulley is called: A. Momentum B. Torque C. Work D. Energy 5. If T1 and T2 are the tension in the tight and slack sides of a belt and θ is the angle of contact between the belt and pulley. Coefficient of friction is μ, then the ratio of driving tension will be: T T T T A. 2  e   B. 1  e   C. 1   D. log10 1   T1 T2 T2 T2
  • 27. BELTING J 3010/6/27 Feedback to Self-Assessment 6 Have you tried the questions????? If “YES”, check your answers now. 1. 3.974 kw ( see example 6.4) 2. 18.97 kw 3. (i) 14.281 kw (ii) 1.3221 kN 4. B. Torque T1 5. B.  e CONGRATULATIONS!!!!….. T2 May success be with you always….