transformer design report

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DESIGN OF SINGLE-  PHASE TRANSFORMER BY: KUNTAL MONDAL. Co-worker: MANAS KUMAR MANDAL. Dept. of Electrical Engg, 3 rd Year, Jadavpur University. 1

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8/3/2019 Transformer Design Report

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DESIGN OF SINGLE- 

PHASE TRANSFORMER

BY: KUNTAL MONDAL.

Co-worker: MANAS KUMAR MANDAL.

Dept. of Electrical Engg, 3rd Year,Jadavpur University.

8/3/2019 Transformer Design Report

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# SPECIFICATION:

  1.5 K VA, 230/110 V, Sinewave 50 Hz, air-cooled, plain tank, ambient 40ºC, temperature rise 50ºC.

#STEP-1: (Calculation of primary and secondary

KVA) V P IP =V S IS =KVA.

IS =1.5×10³/110 A=13.16 A.

IP = V s Is  /V P =(110×13.6)/220 A=6.18 A.

 Actual value of primary current, IP ’=1.02× IP  ; for the no-load current 

=1.02×6.18 A=6.93 A.

Primary KVA= V P  IP ’= 1.526KVA.Secondary KVA=1.5 KVA.

#STEP-2: (Calculation of volts per

turn)Volts per turn, Et =K×Q½.

Where, Q=average of total KVA of secondary & primary =(1.5+1.526)/2 KVA=1.513 KVA.

K=emperical constant=1.1 for shell type=0.8 for core type.

We choose core type construction.

→ Et =0.8×1.513½ =0.98

#STEP-3: (Net iron area)  Net iron area, Ai =Φm  /Bm =(Et ×10 )/(4.44×f×B m  ) cm².

Factor 4.44→sinewave.4.0→squarewave.

 The value of Bm depends on core material.We choose freshCRGO as core material. Bm =1.5 Wb/m².

→ Ai =(0.98×10 )/(4.44×50×1.5) cm²

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=29.43 cm². 

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#STEP-4: (Gross-iron area)Gross-iron area, Agi = Ai  /K i cm².Where, K i →iron space factor 

=actual area of iron in core/mechanical area of core=0.95 for CRGO.

→Agi =29.43/0.95 cm²=31cm².

#STEP-5: (Type of core)Normally,we prefer circular winding. So,we select stepcore for getting circular winding.

#STEP-6: (Calculation of actual core

dimension)

(a) If d=diameter of the circumscribing circle of core,

then, d> (4Agi / Π)½ =( 4×31/  Π)½ =6.28 cm.From table,we select minimum diameter d in cm =7.5 cm.

So, corresponding maximum number of steps= 4.

(b) Now, if  Agi’ be the gross core area given as per unit value of the area of circumscribing circle, thencorresponding to each Agi’ we calculate the numericalvalue of diameter of circumscribing circle d, using d=(4 Agi / ΠAgi’)½.

From table, corresponding to 4 steps Agi’=0.886.  →d={(4×31/( Π×0.886)}½=6.674 cm. 

(c) The dimensions a1 ,a2 ,a3 ,a4 (thickness of steps) arethe width of the laminations per step size, are given as per unit value of diameter d of circumscribing circle in the table.

So, multiplying with d we get actual dimensions as,a1 =6.22cm. a2 =5.33 cm.a3 =4.04 cm. a4 =2.39 cm.

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#STEP-7:From the new sectional dimensions of core, we

calculate the resulting gross-core area Agi using geometry as shown:

 

K 1 =(d²-a1 ²)½=2.42 cm.

K 2 =(d²-a2 ²)½ =4.056 cm.

K 3 =(d²-a3 ²)½ =5.31 cm.

K 4 =(d²-a4 ²)½ =6.231 cm..

 Agi( new )= [a1 K 1 +a2 (K 2 -K 1  )+a3 (K 3 -K 2  )+ a4 (K 4 -K 3  )]

=[6.22×2.24+5.3×1.636+4.04×1.254+2.39×0.92

1] cm² = 31cm².

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This Agi( new ) is almost equal to Agi obtained in step-4.

   Ai( new )= K i × Agi( new )= 0.95×31cm²= 29.43 cm².

 New flux density, Bm( new)= Ai( old  )×Bm( old)/ Ai( new )

=(29.43×1.5)/29.43 Wb/m²=1.5 Wb/m².

New value of d=(4 Agi / ΠAgi’)½ ={(4×31)/( Π×0.934)} ½cm

→d (new)=6.674cm. 

#STEP-8:

 (Window Space Factor)Window space factor, K w =8/(30+’KV’) ;where,’KV’is thehighest kilo

=8/(30+0.220) volts ratingin transformer.

=0.264 .

#STEP-9: (Current Density)The value of current density δ depends on the type of 

cooling,the permitted temperature rise,the maximumambient temperature,the class of insulation and the size of the transformer.

For air natutal cooled without radiators, δ =100 to 300 A/cm².

We take, δ =200 A/cm².

#STEP-10: (Window area required)

  The window area required, Aw =(Q×10 )/(2.22×f×

Bm

K w ×δ× Ai ) 

→ Aw =(1.513×10 )/ 

(2.22×50×1.5×0.264×200×29.43) cm²=58.47cm².= Hw ×W w.

  Where, Hw =Height of window.

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W w =Width of window.

 #STEP-11: (Finding H w  and W w )Assuming, the ratio Hw  /W w =4.

Hw =4W w  

→ W w =3.82 cm.

→ Hw =15.29 cm.

#STEP-12: (Number of turns on LV winding) 

NLV =(ELv ×10 )/(4.44× Bm×f× Ai );where, ELv  is thelow

volt age rating.

=(110×10 )/(4.44× 1.5×50×29.43 )= 113.

#STEP-13: (Number of turns on HV winding)

NHV =NLV ×EHv  / ELv =must be integer.

→ NHV =60×1.5×10³ / 110 =226.

#STEP-14: (Area of primary & secondary

conductor)  Primary current= IP.

Secondary current= IS.

Cross-sectional area of primary conductor, aP  = IP ×10² / δmm²  =6.93×1

0² / 200 mm²  =3.465 mm ². 

Cross-sectional area of secondary conductor, aS  = IS ×10² / δmm²

=13.63

×10² / 200 mm²

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=6.815mm ². 

#STEP-15: (Selection of conductor)We use round enamel coated copper conductor.

SWG Bare copper Bare copper Overall Dia.(mm) for 

area(mm ²  )  Dia.(mm) syn.Enamel

14  3.243  2.0322.15211 6.818 2.943.086

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#STEP-16: (Coil ratings)The transformer is core type.then there will be two

identical coils. one on each limb. hence, each coil will consist of half the primary and half the secondary winding. the two

half primary winding on each coil are connected in series.hence each is rated half the voltage and current.

#STEP-17: (Which  winding is to be started 

first)We place the HV (primary) windings on the outside per 

limb to reduce insulation cost.

#STEP-18: (calculation of dimensions of 

former)The inner windings are to be supported on a ‘former’ or ‘bobbin’ when being wound.

#length or height of the ‘former’ or ‘bobbin’ = (Hw  - 0.5)cm

= (15.29 –0.5) cm

= 14.79cm.

#the thickness t b of the ‘former’ or ‘bobbin’= (2+0.5 ’KV’)mm.

Where, ‘KV’ is the numerical value of the kilo-volts ratingof the inner winding with respect to earth.

  t b = (2+0.5×0.110) mm=2.055 mm.

# c/s dimensions of the ‘former’ or ‘bobbin’:In case of circular winding:

•Inner diameter of the ‘former’:

  Di = (d+0.5) cm ; d→dia. of core circumscribingcircle.

= (6.674 + 0.5) cm= 7.174cm.

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•Outer diameter of the ‘former’:

  Do =[Di +(2×t b  )] cm=[7.174+(2×0.2055)] cm=7.585 cm.

 

#STEP-19: (Calculation of available length of 

winding)  The winding can not be spread over the entire lengthof the ‘bobbin’ or ‘former’ since there must be adequateclearance from the two ends to prevent flash-over fromwinding to the yoke (which is earthed). The clearance oneach side is given by an empirical formula:

l= (5+ 0.9’KV’) mm ; where,’KV’ is the kilo-volts

rating of the inner winding w.r.to

earth.= (5+ 0.9×0.110) mm=5.099 mm.

It is desirable that the heights of both the primary and secondary windings be equal in order to minimize theleakage reactance between them and also to minimize themechanical forces between them at the time of short-circuit 

current flow. Therefore, the LV winding must have aclearance more than what its voltage alone demands.Hence, the available length of the winding is:

L=length or height of ‘former’ or ‘bobbin’ - twice end clarance

=14.79 cm – (2×5.099) mm=13.77 cm.

# STEP-20: (First or inner winding of a coil is ‘LV’

type)

(a) This implies a cylindrical or helical type of winding.

(b) Dimension of insulated conductor:-

For round enamelled copper conductor:SWG=11,14.

Bare copper diameter=2.946,2.032 mm.

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Overall dia. for synthetic enamel coated conductor=3.086,2.152 mm.This is the axial space taken by the conductor per turn.

(c)Calculation of number of turns that can be fitted in one

layer:-For primary 

Turns per layer=(Available length of winding/Axial space of Conductor per turn) – 1

=(13.77/0.215) – 1=63(smaller integer).

For secondary Turn per layer=43

(d) turns per coil for LV winding=113.

So, turns per layer < turns per coil.We accommodate turns per coil in multiple layers

# STEP-21: The inner winding is not ‘HV’ type.

#STEP-22: (Calculation of the radial

‘thickness’or’depth’ of each layer of the ‘inner’ winding)

The radial ‘thickness’ or ‘depth’ of each layer is due to

the overalldimension of the insulated conductor in the radial directioni.e. for circular conductors, it is the overall dimension added with the thickness of inter-layer insulation, whose typicalvalues are 5 to 10 mil. This is necessary to prevent inter-layer short-circuit, since insulation is often damaged duringwinding due to bending and hitting with mallet. We haven’t used any inter-layer insulation.

Thus, overall radial depth of winding=Number of layers×[radial dimension of insulated conductor+thicknessof inter-layer insulation]For lv 

=3×3.086 mm=9.258 mm.For hv 

=4×2.152mm=8.688mm.

#STEP-23: (cooling duct before start of outer winding)

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Duct radial width= 10 to18 mm ; for oil cooling= 15 mm ; we choose to provide

suitable cooling at the same time not much increase inleakage reactance between the windings.

# STEP-24: (For ‘outer’ or ‘second’ winding)

# ‘length’ or ‘height’ of the ‘former’ or ‘bobbin’= (Hw  - 0.5)cm

=

(15.29 – 0.5) cm= 14.79

cm.

#the thickness t b of the ‘former’ or ‘bobbin’= (2+0.5 ’KV’)mm

=(2+0.5×1.5) mm

= 2.11 mm.# c/s dimensions of the ‘former’ or ‘bobbin’:

In case of circular winding:•Inner diameter of the ‘former’:

  Di = (7.585+4×.215+0.5) cm 

Di=8.445cm

 

•Outer diameter of the ‘former’:

 

=[8.445+(2×0.211)] cm  Do=8.867 cm 

# STEP-25: (Design of ‘outer’ winding)

(a) The HV rating = .220KV < 3 KV.This implies a cylindrical or helical type of winding.

(b) Dimension of insulated conductor:- As before, axial space taken by the conductor per turn =

2.152mm.(c) № of turns that can be fitted in one layer 

=(13.77/0.215) – 1=63(smaller integer 

(d) Turns per coil for HV winding = 226.So, turns per layer < turns per coil. We accommodate turns

 per coil in multiple layer.

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The vacant space available per layer is left at the twoends to reduce the possibbility of flash-over due to highvoltage.

(e) Calculation of the radial ‘thickness’ or ‘depth’ of each layer of 

The outer winding:-Similarly, as obtained for inner winding, overall radial depthof windin =4×2.152mm=8.688mm

#STEP-26:   The clearance required is given by:-Clearance = (5+0.9 ’KV’)×0.1 cm ; where,’KV’ is thenumerical value

= of the kilo-voltsdifference

between twoouter winding

voltages.

#STEP-27: (Yoke dimensions)   Assuming identical c/s as in limb, the yoke may haveidentical steps as the limb. For CRGO material, to obtain lowloss in the core structure, it is essential that the laminationsare to be assembled using mitred joints.

#STEP-28: (Calculation of resistance and copper loss

of eachwinding)

 

•For inner(primary) winding:- 

Winding resistance=[Mean turn length(cm)×№ of turns inwinding

×Resistivity] /  Area of conductor(cm²)

 A mean turn is one hypothetically placed in the radial mid- position.

Mean turn length = Π × (7.585 + 0.925/2) cm= 25.28cm.

Number of turns in winding = 113.

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Ambient temperature, T a = 40ºC.

Temperature rise, T r = 50ºC.

Resistivity of copper:-

at 20 ºC, ρ= 0.017593 Ω-mm²/m.

area of bare conductor = 6.818 mm².

→winding resistance at 20 ºC = (0.2528×113×0.017593) / 6.818 Ω= 0.074 Ω.

winding resistance at ( T a+ T r  )ºC,i.e.,90

ºC=.074×[1+0.003929(90-20)]=0.094 Ω.

→copper loss in secondary winding = (Is ² × 1.95) watt = (13.63² × .094)

watt 

= 17.46 W .

•For outer(primary) winding:-Mean turn length = Π × (8.445 + 0.868/2) cm

= 27.9 cm.Number of turns = 226.

winding resistance at 20 ºC = (0.279×226×0.017593) / 3.243 Ω

= 0.34 Ω.

winding resistance at ( T a+ T r  )ºC,i.e.,90ºC=0.34×[1+0.003929(90-20)]

= 0.43 Ω.

Copper loss in secondary winding = (Ip ’² × 0.43) watt = (6.93² ×0.43) watt = 20.81W .

→ Total copper loss =ΣCu loss in two windings

= (17.46 + 20.81) KW =38.29W .

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