Skip to main content

Winding Pitches

Now we will consider the definitions of different types of winding pitches, required in the design of the armature winding.
1.1 Back Pitch 
       The distance which is measured interns of armature conductors i.e. between top and bottom coil sides of a coil measured around the back of the armature i.e. away from the commutator is called back pitch and is denoted by . It is measured interms of coil sides.
Note : Since it is difference between odd and even number, it is always odd number.
       The size of the coil is decided by the back pitch. The back pitch is normally equal to coilsides per pole. It is shown for lap and wave type of winding in the Fig. 1.
Fig. 1
       The back pitch for the winding shown in the Fig. 1 is yb = 14 - 1 = 13 as coilsides 1and 14 are of coil number 1.
1.2 Front Pitch
       It is defined as the distance measured between two coilsides which are connected to some commutator segment. It is denoted by yf. The front pitch for the winding shown in the Fig. 1 is  yf = 14 - 3 = 11. This is front pitch for lap winding while for wave winding yf = 27 - 14 = 13. The front pitch for both lap and wave type winding is odd. If for a lap winding the connections are traced then the movement is backwards (coil side 14 to coil side 3). Hence the type of winding can be determined from front pitch and it does not affect the size of coils.
1.3 Winding Pitch
       It is defined as the distance between the starts of two consecutive coils measured in terms of coil sides. It is denoted by Y.
       For lap winding,       Y = yb - yf
       For Wave winding,   Y = yb + yf
       For the lap winding shown in the Fig. 1 the winding pitch is Y = 13 - 11 = 2 while for wave winding Y = 13 + 13 = 26. It is also the distance round the armature between two consecutive conductors. Practically, coil pitches or winding pitches as low as eight tenths of a pole pitch are employed without much reduction in emf.
Note : Fractional pitches windings are intentionally used so as to achieve saving in copper of the end connections and for improvement in commutation.
1.4 Commutator Pitch
       It is defined as the distance between the two commutator segments to which the two ends i.e. starts and finish of a coil are connected. It is measured in terms of commutator segments and it is denoted by yc. For the windings shown in the Fig. 1.
       yc = 2 - 1 = 1     for simplex lap winding
       yc= 12 - 1 = 11 for simplex wave winding
       For lap winding is the difference between yb and yf while for wave winding yc is the sum of yb and yf. The number of bars between the coil leads is commutator pitch. In general yc is the 'plex' of lap wound armature. It is 1, 2, 3 for simplex, duplex, triplex lap windings respectively.
       On tracing through simplex lap winding,a segment adjacent to the first one is reached after traversing through one coil. For simplex wave winding, the adjacent segment is reached after traversing through P/2 coils.

Comments

Popular posts from this blog

Transformer multiple choice questions part 1

Hello Engineer's Q.[1] A transformer transforms (a) frequency (b) voltage (c) current (d) voltage and current Ans : D Q.[2] Which of the following is not a basic element of a transformer ? (a) core (b) primary winding (c) secondary winding (d) mutual flux. Ans : D Q.[3] In an ideal transformer, (a) windings have no resistance (b) core has no losses (c) core has infinite permeability (d) all of the above. Ans : D Q.[4] The main purpose of using core in a transformer is to (a) decrease iron losses (b) prevent eddy current loss (c) eliminate magnetic hysteresis (d) decrease reluctance of the common magnetic circuit. Ans :D Q.[5] Transformer cores are laminated in order to (a) simplify its construction (b) minimize eddy current loss (c) reduce cost (d) reduce hysteresis loss. Ans : B Q.[6] A transformer having 1000 primary turns is connected to a 250-V a.c. supply. For a secondary voltage of 400 V, the number of secondary turns should be (a) 1600 (b) 250 (c) 400 (d) 1250 A...

Condition for Maximum Power Developed In Synchronous Motor

The value of δ for which the mechanical power developed is maximum can be obtained as, Note : Thus when R a is negligible, θ = 90 o for maximum power developed. The corresponding torque is called pull out torque. 1.1 The Value of Maximum Power Developed        The value of maximum power developed can be obtained by substituting θ = δ in the equation of P m .        When R a is negligible,     θ = 90 o  and cos (θ) = 0 hence, . . .               R a = Z s cosθ   and X s = Z s sinθ        Substituting   cosθ = R a /Z s in equation (6b) we get,         Solving the above quadratic in E b we get,        As E b is completely dependent on excitation, the equation (8) gives the excitation limits for a...

Effect of Slip on Rotor Parameters : Part2

Effect of Slip on Rotor Parameters 2. Effect of Slip on Magnitude of Rotor Induced E.M.F        We have seen that when rotor is standstill, s  = 1, relative speed is maximum and maximum e.m.f. gets induced in the rotor. Let this e.m.f. be,                 E 2 = Rotor induced e.m.f. per phase on standstill condition         As rotor gains speed, the relative speed between rotor and rotating magnetic field decreases and hence induced e.m.f. in rotor also decreases as it is proportional to the relative speed N s - N. Let this e.m.f. be,                E 2r = Rotor induced e.m.f. per phase in running condition  Now        E 2r α N s while E 2r α N s - N        Di...