The metallurgical characteristics of non-precious alloys using Nd:YAG laser welding
© Lee et al. 2015
Received: 15 September 2015
Accepted: 4 November 2015
Published: 3 December 2015
This study aimed to determine the effect of hardness change according to penetration depth in the laser fusing zone and observed the correlation of the microstructure as an Nd:YAG laser was irradiated to Ni-Cr alloy for dental use by setting the spot diameter size with respect to defocusing distances. In all groups, the hardness depth profiles in the laser fusing zone and heat-affecteded zone (HAZ) had larger values than those of the base metal. In addition, the hardness values in places beyond the fusing zone and the HAZ were measured as being quantitatively lower.
The alloys used in this study were Verabond 2 V, Noritake Super, and Bellabond Plus, which are commercially used non-precious dental alloys. The specimens were cut to have a plate shape with a size of 0.5 × 3.0 × 2.5 mm. This was followed by setting the Nd:YAG laser output, pulse duration, and frequency to 60 W, 10 ms, and 5 Hz, respectively. The laser was then irradiated as the spot diameter condition varied between 0.5 mm and 1.4 mm in accordance with defocusing distance from 0.0 mm to 2.0 mm. After the laser irradiation, a cross-section of the fusing zone in the specimens was observed in terms of laser melted depth, hardness depth profile, and the microstructure of each alloy.
The observation result of the diffusion of the constituent elements and microstructure using field emission scanning electron microscopy, energy dispersive spectroscopy (EDS), and electron probe micro-analyzer showed that the fusing zone revealed a much finer dendritic form than the base metal due to the self-quenching effect after laser melting, while no change in constituent elements was found although some evaporation of the main elements was observed.
These results suggest that each Mo and Si combined inter-metallic compounds were formed on the interdendritic area. Through this study, the laser fusing zone had better hardenability due to the inter-metallic compound and grain refinement effect.
KeywordsNon-precious alloys Laser weld Hardness Microstructure
The importance of joining the connecting parts of casts for prosthesis manufacturing in the dental field has increased significantly. Welding is required when metals need to be joined for a variety of reasons, such as re-attachment of the severed prosthesis or fractures in order to fix the deformation or errors after casting during the manufacturing of the metal structures of the fixed prosthesis .
The soldering methods generally used in existing dental fields inevitably introduce gas into the soldering connecting part, thereby leaving bubbles and degrading the strength of the connecting parts; using gas also results in the formation of a wide heat-affected zone (HAZ), which can change the particle size of the joint metals and decrease their tensile strength. It can also cause increased corrosion due to the direct contact between the deposited metals and the other different types of soldering materials, resulting in the reduction in strength of the joint parts. These shortcomings in the existing soldering methods can be overcome using Nd:YAG laser welding [2, 3].
Since laser welding concentrates energy on a small area, it creates a small HAZ. It is also performed under an Argon atmosphere so that it has the advantage that oxidation is minimized in the area surrounding the diameter where the laser is irradiated . As such, laser welding has been proven to be a more effective technology than existing soldering methods [5, 6].
When laser welding is performed, some of the laser beams are reflected from the surface of the metal, while the rest of the beams are absorbed into the metal. Only those laser beams that are absorbed are used for material processing. The amount of laser beam absorbed into the surface of the metal can be different depending upon the wavelength of the laser beam surface roughness and the thermal conductivity of the metal. The absorbed part is changed into heat energy from the metal surface, thereby producing an important heat source for laser welding .
Once the laser heat source that is converged by the laser beam is irradiated to the surface in the pre-determined axis direction, only a local layer on the surface is heated by the thermal conductivity that occurs inside, and the heat on the surface is rapidly cooled down as soon as the laser beam is removed. Such a cooling process is known as self-quenching .
It has been known that the fusing zone and the surrounding HAZ experience changes in both their microstructure and hardness at the penetrated fusing zone due to the rapid cooling . While this type of change in the metallurgical characteristics due to laser irradiation has been reported, this study aims to discuss the metallurgical characteristics that are changed by Nd:YAG laser welding used in the casting of a dental alloy by setting a laser spot diameter size with respect to defocusing distances, which can be selected generally in the laser welding.
Materials and specimen preparation
Chemical compostion of dental alloys (wt. %)
Verabond 2 V
Material properties dental alloys
Verabond 2 V
Vickers hardness (Hv)
Yield strength (MPa)
Tensile strength (MPa)
Melting range (°C)
CTE(×10–6/°C) (25 °C ∼ 500 °C)
13.7 × 10–6 · K-1
13.4 × 10–6 · K-1
13.9 × 1010–6 · K-1
Once the specimens were cut to have an acryl plate shape with a size of 0.5 × 3.0 × 2.5 mm3, followed by investment and burnout according to manufacturer’s instruction, material casting was performed using a highfrequency casting machine (SuperCast 3; SEIT, Italy) within the cast temperature range for each alloy. After the casting was complete, the investment material was removed. Then, steam cleaning was performed on the specimens by spraying 110 μm Al2O3 from a distance of 10 mm with a pressure of 3 bar for 10 s.
Laser beam irradiation and measurement of penetration depth
The laser was irradiated to the center of the specimens under the same condition, with an output of 60 W, pulse duration of 10 ms, and frequency of 5 Hz set in the Nd:YAG.
Condition of laser irradiation test (n = 3)
Spot diameter (mm)
Pulse duration (ms)
In order to measure the laser melted depth, the fusing zone was cut into half using a metal cutting machine (Sapcom; Hyunyang Co., Ltd, Korea) to see the crosssection.
Once the cross-section of the specimen is placed facing the base, molding was performed using a mounting press (MOT-FTA-2; F-tech Co., Korea), and mirror polishing was conducted on #400, #800, #1200, and #1500 SiC paper using a polisher (POL-FTA-2; F-tech Co., Korea). The surface shape of the specimen irradiated after mirror polishing was observed using an optical microscope.
In addition, this study analyzed the experimental data of each material by using the statistical program called SPSS for Windows 18.0 (SPSS INC, Chicago, IL, USA) in order to identify the impact of change of laser diameter on penetration depth. The findings of penetration depth for the laser diameter of each group were recorded as mean and standard deviation. Moreover, this study examined each coefficient through simple regression analysis.
To observe the hardenability of the alloys for dental use irradiated by a laser, changes in hardness were examined. Hardness measurement was conducted for 10 s with a 200 gf load using a micro-vickers hardness tester (HM112; Mitutoyo, Japan). By setting the 35 μm inner side from the central surface of the laser fusing zone to the origin, every 100 μm of depth up to 1300 μm was measured.
To conduct metallographic observation after laser irradiation and alloy mirror polishing, the surface of the metal base was etched using a reagent of 7.5 mL HF, 2.5 mL HNO3, and 200 mL methanol, followed by observation of the specimen cross-sections using a scanning electron microscope (field emission scanning electron microscopy (FE-SEM); LEO SUPRA 55; Carl Zeiss, Germany). The acceleration voltage and current conditions of FE-SEM were 10 keV and 10 nA, respectively, and the main observation scale was within a range of 40–250. During the SEM analysis, the surface of the specimen was gold coated and analyzed with energy-dispersive spectroscopy (EDS) qualitatively (in-lens detector + secondary ion detector). In addition, element diffusion of the specimen was observed through a backscattered electron (BSE) detector (topography and composition image) by irradiating electron beams accelerated with 15–30 keV by an electron probe microanalyzer (EPMA) (JXA-8100; JEOL, Japan) to determine the zone change by means of the diffusion of the specimen elements due to laser welding.
Nd:YAG laser beam was irradiated to Ni-Cr alloys for dental use by changing the spot diameter between 0.5 and 1.4 mm, thereby measuring the laser melted depth as a result of experiment.
Penetration depth by change in laser spot diameter
laser melted depth of laser irradiation on cast plate specimens (mm)
Penetration depth [Mean ± SD]
Verabond 2 V
1.27 ± 0.08
1.25 ± 0.08
1.03 ± 0.06
1.17 ± 0.11
1.16 ± 0.09
0.9 ± 0.11
1.09 ± 0.19
0.78 ± 0.15
0.58 ± 0.04
0.73 ± 0.04
0.64 ± 0.05
0.46 ± 0.04
0.53 ± 0.21
0.48 ± 0.07
0.31 ± 0.10
Hardness depth profile analysis
Comparison of laser melted depth profiles according to spot diameters
Equation (y = aχ + b)
−0.851 × + 1.792
Verabond 2 V
−0.924 × + 1.767
−0.847 × + 1.486
Where, y represents laser melted depth, whereas χ represents spot diameter of laser.
No significant difference between the samples. Also, laser melted depth becomes shallower when laser diameter becomes larger.
This study reviewed hardness change according to penetration depth in the laser fusing zone and also observed the microstructure while irradiating an Nd:YAG laser to an Ni-Cr alloy for dental use with a variety of spot diameter sizes.
The results revealed that as the laser sport diameter size became smaller, the penetration depth increased and a keyhole shape was displayed distinctively in all three different types of alloys. The reason for this result is that the focused spot diameter increased as the laser melted diameter decreased, and the temperature of the fusing metal exceeded the boiling point, resulting in fusion as the laser density supply was raised .
The change in hardenability according to penetration depth showed that the dominant factor that determines the hardness of the alloys was not decided by a hardenability function in general but by the penetration depth of heat due to laser beam irradiation .
That is, high hardness can be achieved because the microstructure of the base metal was modified by the laser irradiation . The hardness values displayed at the fusing zones of all specimens were larger than those provided by the manufacturer of the alloys as well as those at the casting state. On the other hand, a low hardness value was found around the base metal, except in the fusing zone and HAZ. This result was found because a major structural change in grain refinement occurred in the proximity of where fusion was generated due to a high temperature, thereby creating the FG HAZ and IC HAZ of the grain in the HAZ. The lower hardness values found in the base metal beyond the fusing zone and the HAZ were found because that area was not directly affected by the laser heat source, so the area had the characteristics of the SC HAZ.
The grain refinement in the welding area was found because the grain refinement effect due to a cooling speed difference by the thermal stress occurred in the surface and the inside at the time of heating and cooling rather than a cooling speed difference due to the structure-sensitive property. Such grain refinement effect caused an increase in the dislocation density, thereby showing high hardness in contrast with the base metal. The reason for the formation of the fusing zone and the HAZ was that the laser-irradiated area in the alloy was heated rapidly followed by rapid selfquenching due to the surface heat conducted to the inside after a laser beam was passed through, creating nonequilibrium solidification rather than equilibrium solidification.
This study aimed to observe a correlation between hardness change and changes in metallurgical characteristics during laser welding. When a laser is irradiated to a unit area with the same energy, the penetration depth is dependent on the characteristics of alloy such as specific values of thermal conductivity and diffusion rate of the alloy, reflectivity during laser welding, and an optical absorption rate. The effect of these factors cannot be determined by the results of the experiment in this study only.
Therefore, additional experiments are necessary to understand the effect of the thermal conductivity and diffusion rate of the alloy due to laser welding in the future in parallel with identification of corrosion in the fusing zone.
The laser melted depth of all alloys increased when the diameter size of laser spot got smaller. The hardness value of melting area and heat-affected area was 50 % higher than the hardness value of base metal.
Although there was no change in ingredient of both fusing zone and base metal, there was intermetallic compound combined with Mo and Si elements in the interdendritic area.
As a result of this study, it was possible to understand that hardenability gets better by intermetallic compound and grain refinement effect on the laser fusing zone.
This research was supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (2012–0531).
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