Design And Construction Of Electric Arc Welding Machine
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Design And Construction Of Electric Arc Welding Machine
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TABLE OF CONTENT

CHAPTER ONE

  1. Introduction
    1. History
    2. Aims/objective
    3. Scope
    4. Principle of transformer Operation
    5. Equivalent Circuit of the Machine

 

CHAPTER TWO

  1. Literature Review
    1. Transformer Design
    2. Coil Design
    3. Core Design
    4. Specification for design

 

CHAPTER THREE

  1. Construction
    1. Lamination
    2. Transformer former
    3. Copper coils
    4.  Insulating Materials
    5. Methodology
    6. Test and Operating Conditions
    7. Operating Conditions
    8. Conclusion
    9. Recommendation

REFERENCES

CHAPTER ONE

 

HISTORY/INTRODUCTION

  1. The machine is specially designed for industrial and agricultural welding. It is only powered from A.C power source for all welding.

The unit is designed to operate on single phase 240v A.C. supply and it is mainly a transformer unit. It is capable of operating from 25 Amps socket for most of its output range. The current drawn form the mains supply may exceed the 25 Amps, hence the unit must be provided with 30A switch fuse input as those provided for electric cookers, heaters etc. this connection must be made to the dead side of a 30A circuit. The circuit should not be shared by any other appliance.

          The unit consists of the following main components single phase transformer (with tap changing secondary). The transformer is a step-down transformer with different tapping at H, M and L; welding tung cables.

          The transformer is a conventional-cooled, single phase transformer which has shell type of lamination core and insulated windings of copper cols. In addition, the windings are given double insulation with the use of varnish solution which helps to prevent short-circuiting in the windings.

With the help of Angle iron and lamination core, the core loss, iron loss in the machine is reduced to minimum. They also help to reduce humming in the machine. Hence, efficiency of the machine is greatly improved.

 

  1. AIMS AND OBJECTIVES

Sequel to the vast need and use of iron rods, metal bars and pipes, right from the domestic level up to industrial extent, the arc welding machine was built in order to ensure that the ulterior motive of the manufacturers of these products (iron rods, metal bars and pipes) by their manufacturers is being achieved as part f technological advancement. With the electric Arc welding machine, the difficulty of using iron rods, bars and pipes in construction works has been removed.

          Moreso, the Arc welding machine has also contributed a lot towards the economy of life in such a way that when products like machine tools, agricultural tools, machine parts, motor parts etc get broken, they could be restored to usage, or made functional once again through welding, by the use of the electric Arc welding machine. In that respect, the problem has been solved without going back to purchase a new one.

SCOPE

The machine is specially designed for industrial and agricultural welding. It is powered from single phase, 240v 50Hz power supply. It is operated from 30A socket.

During use; when tap changing, the entire machine should be off before tap changing the load terminal when welding.

          When there is low welding current and due to variation of power supply, a higher tap should  be  used to increase the welding current.

          This electric Arc welding machine is a  heavy duty welding machine which is capable of welding all or 12 gauges of electrodes, while in operation.

          For material cutting, the machine should be tapped at the highest tapping, although cutting is not very effective at low voltage supply.

 

PRINCIPLE OF TRANSFORMER OPERATION

An alternating voltage applied to P circulates an alternating current through P and this current produces an alternating flux in the iron core, the mean path of this flux being represented by the dotted line D. if the whole of the flux produced by P pass through S, the emf induced in each turn is the same for P and S. hence if N1 and N2 be the number of turns on P and S respectively (refer to fig. 2.0).

Total emf induced in S   =  N2  x  emf per turn  = N2

Total emf induced in P   =  N1  x  emf per turn  =  N1

When the secondary S is open circuit, its terminal voltage is the same as the induced emf. The primary current is then very small, so that the applied voltage V1­ is practically equal and opposite to emf induced in P, hence 

       V2    =  N2

                 V1       N1

Since the full load efficiency of a transformer is nearly 100 percent, I1V1   x  primary power factor  = I2V2   x  secondary power factor. But, the primary and secondary power factor at full load are nearly equal 

       I1    =  V2

                 I2       V1

When a load is connected across secondary terminals (short circuited), the secondary current  - by Lenz’s law produces a demagnetizing effect. Consequently, the flux and the emf induced in the primary are reduce slightly. But this small change may increase the difference between the applied voltage and the e.m.f induced in the primary from say 0.05% to say 1%, in which case the new primary current would be 20 times the no-load current. The demagnetizing ampere-turns of the secondary is thus nearly neutralized by the increase in the primary ampere-turns and since the primary ampere-turns on no load are very small compared with the full load ampere-turns.

  • full load primary ampere-turns  =  full load secondary ampere-turns.

i.e I1N2   =   I2N2

so that  I1   =   N2   =   V2

            I2        N1         V1

It will be seen that the magnetic flux forms the connecting link between the primary and secondary currents and that any variation of the secondary current is compared by a small variation of the flux and therefore of the e.m.f induced in the primary, thereby enabling the primary current to vary approximately proportional to the secondary current. This balance of primary and secondary ampere-turns is an important relationship whenever transformer action occurs.    

​Designed Diagram.....

RP  and RS are resistances equal to resistance of the primary and secondary windings of the machine.

          Similarly, inductive reactance XP  and XS represent the reactance of the windings due to leakage flux in the machine. The inductance reactor X is such that it takes a reactive current equal to the magnetizing current (IM) of the transformer. The core losses due to hysteresis and eddy currents are allowed for by a resistor R of such value that it takes a current IC equal to the core-loss component at the primary current, i.e IC2R is equal to the core loss of the actual transformer. The resultant of (IM) and IC is IO.



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