Fusion welding processes are widely used for fabrications in many engineering applications such as aerospace, automobile and ship building industries. Oxy-Acetylene Welding (OAW) is the most commonly used gas welding process because of its high flame temperature. Gas welding is a welding process that melts and joins the metals by heating them with flame caused by the reaction between a fuel gas and oxygen [1] .

The main advantage of the OAW process is that the equipment is simple, portable and inexpensive. The total heat input per unit length of the weld in OAW process is rather high, resulting in large Heat Affected Zone (HAZ) which causes severe distortion [2] . Shielded Metal Arc Welding (SMAW) is a process that melts and joins metals by heating them with an arc established between a stick-like covered electrode and the metals. The welding equipment is also simple, portable and inexpensive [3] .

One of the limitations of the two welding processes mentioned above as reported by Sindo [1] is the low power density of the heat source. The power density increases from a gas flame to an electric arc and a high- energy beam, and as the power density of the heat source increases, the heat input to the work piece that is required for welding decreases. The portion of the work piece material exposed to a gas flame heats up so slowly that before any melting occurs, a large amount of heat is already conducted away into the bulk of the work piece. Excessive heating can cause damage to the work piece, including weakening and distortion [4] . However, control of welding parameters such as welding current, voltage and speed can reduce the amount of heat input into the weld. Besides, edge preparation prior to welding can significantly affect the quality of the weld.

In view of the fact that arc welding processes like SMAW offer a wide spectrum of thermal energy for joining different thicknesses of steel, it was considered important that undertaking the present study would be very beneficial in gaining an understanding of the mechanical properties of low-carbon steel that influence the service performance of the welded joints under different heat input combinations i.e. low heat input and high heat input [5] [6] .

The chemical composition of steel has impact on the weldability and the mechanical properties of the material. According to Monika et al. [7] , several elements are purposefully added in the production of structural steel, but other undesirable elements may equally be present arising from the scrap materials charged during the steel- making process. Carbon, manganese, tungsten and other elements increase strength and may increase the risk of cold cracking and therefore higher preheat and inter pass temperatures, better hydrogen control and sometimes post heat are necessary to avoid cracking [7] .

Ueji [3] noted that weld fusion zone microstructure of low-carbon steel depends on the chemical composition of the material and the cooling rate. For steels, the required critical cooling rate for achieving martensite in the microstructure can be estimated using the following equation

where is the critical cooling rate in kmol/hr.

Volume of melted metal is a function of heat input which in turn is governed by the welding parameters such as welding current and welding time. Increasing current decreases the fusion zone size while increasing time increases the fusion zone size [8] [9] .

Ultrafine grained refinement from conventional grained size (10 µm) to less than 1 µm provides a preferable high strength to metallic materials used for structural applications as reported by Lowe and Zhu [10] . Ultrafine grained steel structural component in engineering application can be done by welding to produce complex structure which is difficult to manufacture directly. The major disadvantage of fusion welding of this ultrafine grained steel is the occurrence of grained growth during welding leading to reduction in strength [3] . Careful control of welding parameters can reduce the amount of heat input into the weld thereby avoiding the excessive grained growth and allotropic transformation in metals, thus improving the mechanical properties of the welded steel metal.

This work is therefore aimed at investigating the effects of welding current and voltage at two different edge preparations on the mechanical properties of low-carbon steel, using oxy-acetylene and shielded metal arc welding processes.

Figure 4 clearly shows the mechanical properties of the welded steel at fixed Voltage (220 V) and varying Current in Straight Edge preparation welded sample. It was discovered that current adjustment affects the weld bead size, appearance, penetration and strength of the weld. There was a decrease in Hardness and Tensile strength of the welded steel as the current was increased. With increased current, the heat generated increased causing the grain to recrystallized and grow in size. Increased in grain size increases the impact strength (toughness) of the weld but reduction in hardness and tensile strength of weldment and heat affected zone as depicted by the graph. This was in agreement with [4] . Similarly, the amount of heat input from the heat source is given by

.

This shows that as the current increases more heat is produce into the weld causing more expansion and contraction between the weldment and the base metal. This increased the residual stresses resulting in lower mechanical properties.

Figure 5 shows the mechanical properties of the welded steel at fixed voltage (220 V) and varying current in the V groove edge welded sample. From this plot, the hardness as well as the tensile strength of the weldment and heat affected zone decreased with an increase in the current. This again is due to increase in heat input into the weldment. The heat persisted for a period of time and is quickly conducted away into the base metal as a result of low power density of the welding process (SMAW) as reported by Sindo [1] . Consequently, the based metal was affected due to high heat input into the weld resulting in grain size increased. This case is also similar

to what happened in Figure 4. The only exception is that Figure 5 is with V-grooved edge with high amount of weldment deposit. This increased the residual stresses in the weldment and heat affected zone. Residual stresses can significantly affect the engineering properties of the material and this has contributed to reduction in strength and hardness of the weldment and heat affected zone as shown in the Figure 5.

In Figure 6, the current was fixed at 100 A while the voltage was varied from 100 V to 200 V. The hardness and the tensile strength of the weldment and the heat affected zone reduced as the voltage increases. This is similar to that of Figure 4 and Figure 5 as they all conformed to the mathematical model equation relating heat source and welding parameters (current and voltage) [5] [6] . Besides it is difficult to maintain constant gap between the arc and the weldment in manual welding, and as such the system is self-adjusting such that increase in voltage will not cause significant increase in welding current as reported by Tariq in his lecture 2014 at King Fard University of Petroleum Saudi Arabia.

Figure 7 shows similar phenomenon as that in Figure 6, though the edge preparation differences caused significant changes in the mechanical properties. It was observed in Figure 6 that the tensile strength at 100 A is about 500 N/mm² while the corresponding tensile strength in Figure 7 is about 420 N/mm². This is because grove edge accommodates more weld deposit than straight edge and therefore the bonding strength should have been better than that of straight edge. As reported in several literature, the more the weld deposit, the higher the expansion and contractions consequently increase in residual stresses in the weldment and the heat affected zone. Gery et al. [4] noted that, residual stresses can significantly affect the mechanical properties of the weldment. It was also noted that the impact strength is slightly higher in Figure 7 than in Figure 6 with the similar reasons explained above.

Figure 8 and Figure 9 depict fixed current and voltage with different edge preparation. The phenomenon in both figures was almost the same as there were no changes in the heat input into the weldment. However differ-

ences in edge preparations caused slight disparity in the values of the mechanical properties of the two types of preparation under study. Tensile strength is higher in V-grooved edge in Figure 9 than that of straight edge in Figure 8 as the effect of bonding is dominant over the residual stress due to constant heat input into the weldment. Similarly, the impact strength (toughness) also improved slightly in V-grooved edge in the Figure 9 than the corresponding impact in Figure 8.

In Figure 10 and Figure 11, the same scenario is exhibited except that the electrode is of different compositions. It was discovered that the use of different electrode at constant current and voltage did not have any significant changes in the tensile strength and hardness of the welded steel. However there is a noticeable improvement in the impact strength in V-grooved edge in Figure 11 than that of Figure 10.

Figure 12 and Figure 13 shows the mechanical properties of the welded steel at fixed current and voltage for different cooling medium with straight edge and V-grooved edge preparations respectively. The cooled in still air samples has a lower tensile strength, and higher hardness values as shown in Figure 12. This may be due to a slow rate of cooling in draft air than that of still air. Low cooling rate led to grain growth of the welded joint [3] [8] [9] . In Figure 13, it was observed that there was decrease in the hardness value of the sample cooled in the still air, and this can be attributed to decrease in the concentration of hydrogen on the joint surface that caused long time or delay in cooling rate.

Figure 14 shows the comparison of the mechanical properties of samples welded with oxy-acetylene in straight edge and V-Beveled edge preparations. From this figure, the tensile strength and the hardness values of the two types of preparations were totally different. As compared to SMAW, the mechanical properties of OAW as reported in Figure 10 is lower than that of SMAW shown in Figure 4 and Figure 5 respectively. This is due low power density of OAW process.

The results of microstructural examination revealed that all the welded joints contain pearlite and ferrite phases.

Figure 15(a) shows the structure of the Base Metal of the Low Carbon Steel used for this study. The structure consists of about 80% to 85% ferrite (white) and about 15% to 20% pearlite (black).

It was observed that the grain-refined area exhibits extremely small ferrite grains, clearly indicating that very fine ferrite and pearlite is formed due to the heating and cooling cycles of the SMAW process [7] .

Figure 15(a) and Figure 15(b) show the microstructures of the Weld Zone of samples welded at Constant Voltage and varied Current setting, representing a grain-coarsened area, which exhibits predominantly White Ferrite (WF) and pearlite.

Figure 16(a) and Figure 16(b) show the structure of the samples welded at constant current, and varied Voltage setting. It was observed that a large amount of pearlite is present in the ferrite matrix. As the current was increased, the pearlites become finely distributed within the coarse matrix with an increase in the proportion of the ferrite to pearlite.

Figure 17(a) and Figure 17(b) compare the prepared straight edge and the prepared V-grooved edge and it was discovered that ferrite phase were more than pearlite phase in their microstructure which also indicates

higher ductility in Figure 17(a); this is in agreement with the work of [5] [6] .

Examination of the Welded Zones in Figure 18(a) and Figure 18(b) also revealed the effect of electrode size on the microstructure. The observed structure is of coarse pearlite in ferrite matrix which became more coarse as the grain size increased. This observation explained the decrease in the hardness and tensile strength values as the heat energy input was increased.

Microstructure for samples welded with fixed voltage and current setting for different cooling medium were shown in Figure 19(a) and Figure 19(b). These plates revealed the effects of cooling rate after welding on the properties of the steel. Cooling in still air produces coarse grain structure of both ferrite and pearlite while cooling in draft air produces fine grain size. This is due to slow cooling of the weldment in still air [3] .

Figure 20(a) and Figure 20(b) revealed fine-grain microstructure of weldment of sample with Oxyacetylene welding procedure. Fine grain ferrite and pearlite were observed in this area as compared to the base metal microstructure (Figure 19(a)). However, as observed from Figure 21(a) and Figure 21(b) better grain refinement were noticed than in Figures 20(a) and Figure 20(b). This clearly indicates that during the heating and cooling cycles, a very fine grain structure is formed in the FZ. This area is generally termed as the grain-refined area.

From the observation of the plates, the microstructures with higher concentration of the pearlite phase will have more hardness and strength but with lower ductility. Ferrite crystals were formed as a result of transformation in low-carbon steel upon cooling from the austenitic state. It is not possible to state the relationship mathematically, but since the ferrite grains are nucleated and grow; their size will depend on time and temperature,

especially on the cooling rate.

The following conclusion can be drawn from the present study:

Ÿ Adequate edge preparation of the weldment enhances the strength of the welded steel. This may be due to the high diffusion of the weld metal which in turn may enhance bonding of the two metal pieces.

Ÿ The hardness, tensile and impact strength of the welds are functions of the microstructure; therefore these properties are structural sensitive.

Ÿ It was observed that the strength and hardness of the joint increase with the decrease in heat input.

Ÿ The toughness increases while the hardness and tensile strength of the joint decrease.

M. A. Bodude,I. Momohjimoh, (2015) Studies on Effects of Welding Parameters on the Mechanical Properties of Welded Low-Carbon Steel. Journal of Minerals and Materials Characterization and Engineering,03,142-153. doi: 10.4236/jmmce.2015.33017