IN-SITU MECHANICAL PROPERTY DETERMINATION USING SMART OPTICAL MONITORING DURING ADDITIVE MANUFACTURING

Abstract

Mechanical properties of materials fabricated with additive manufacturing process are determined through optical monitoring in real time. A plasma generated in a zone where a laser interacts with deposited material is monitored using optical emission spectroscopy to generate one or more plasma spectral lines. The emission lines are analyzed to determine the hardness, micro-hardness, yield/residual stress, tensile strength, or other mechanical characteristics of the material. The composition may be an alloy such as an aluminum-magnesium alloy, including 7000 series aluminum alloys. The mechanical property may be derived from a change in a ratio of the plasma spectral lines, including a change in a ratio of ionic and neutral magnesium (Mg) associated with a 7000 series aluminum alloy. The apparatus and methods are extendable to other alloys and compositions.

Claims

1. In an additive manufacturing process wherein a laser beam is used to heat a material to form a melt pool that solidifies to form a desired composition, and wherein a plasma is generated in a zone where the laser interacts with the material, the improvement comprising: monitoring the plasma, in situ, using optical emission spectroscopy to generate one or more plasma spectral lines; and analyzing the plasma spectral lines to determine a mechanical property of the composition.

2. The improvement of claim 1, wherein the mechanical property is the hardness of the composition.

3. The improvement of claim 1, wherein the mechanical property is the micro-hardness of the composition.

4. The improvement of claim 1, wherein the mechanical property is the yield stress of the material.

5. The improvement of claim 1, wherein the mechanical property is the tensile strength of the material.

6. The improvement of claim 1, wherein the composition is an alloy.

7. The improvement of claim 1, wherein the composition is an aluminum-magnesium alloy.

8. The improvement of claim 1, wherein the mechanical property is derived from a change in a ratio of the plasma spectral lines.

9. The improvement of claim 8, wherein the mechanical property is derived from a change in a ratio of ionic and neutral spectral lines.

10. The improvement of claim 9, wherein: the composition is a 7000 series aluminum alloy; and the mechanical property is derived from a change in a ratio of ionic and neutral magnesium (Mg).

11. The improvement of claim 10, wherein the mechanical property is the hardness of the alloy.

12. The improvement of claim 10, wherein the mechanical property is the micro-hardness of the alloy.

13. The improvement of claim 10, wherein the mechanical property is the yield stress of the alloy.

14. The improvement of claim 10, wherein the mechanical property is the tensile strength of the alloy.

15. The improvement of claim 10, wherein the mechanical property is the thermal residual stress of the alloy.

16. The improvement of claim 1, wherein the determination of the mechanical property is determined in real time.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0010] FIG. 1 illustrates the components of a Smart Optical Monitoring System (SOMS);

[0011] FIG. 2 depicts the use of SOMS for additive manufacturing (AM) processes;

[0012] FIG. 3 is a plot that shows the ratio of Ionic Mg(II) @280.27 nm/Neutral Mg(I) @285.20 nm (1.sup.st layer);

[0013] FIG. 4 is a plot that shows the ratio of Ionic Mg(II) @280.27 nm/Neutral Mg(I) @285.20 nm (3.sup.rd layer);

[0014] FIG. 5 is a plot that shows the ratio of Mg(II) @280.27 nm/Mg(I) @285.20 nm (with no powder, AA7075 substrate);

[0015] FIG. 6 is a graph that illustrates Micro-Hardness and Electron Temperature vs. Intensity Ratio (Mg(II)/Mg(I));

[0016] FIG. 7(a) is a graph that shows Vickers hardness versus yield stress relationship drawn from the data of Flynn [17-18]; and

[0017] FIG. 7(b) is a graph that illustrates Tensile strength versus Vickers hardness for 7010 plate and forging [17].

DETAILED DESCRIPTION OF THE INVENTION

[0018] A smart sensor has been developed in conjunction with this invention that provides in-situ and reliable prediction of the components of 7000 series aluminum alloys, including composition, phase transformation, and manufacturing defects in accordance with industrial standards. Features were implemented for automatic defect detection and robust composition detection. For composition analysis, methods to improving the accuracy of the composition measurements have also been identified and investigated.

[0019] Furthermore, monitoring the emission lines ratio of ionic and neutral Mg, and the changes in the values of the emission line ratio, a difference in the hardness of the target material, thereby the change of strength of material can be estimated. By fine-tuning the emission lines ratio, thermal residual stress may be estimated to achieve mitigating effects.

Mechanical Properties: Relationship Between Intensity Ratio and Micro-Hardness

[0020] It has been empirically demonstrated that hardness and strength of material (e.g. UTS) have a linear relationship. Hardness is not really an intrinsic property of a material. Rather, the hardness value depends more on the technique and attributes of the material (e.g. strain hardening, microstructure) than on fundamental physical properties. However, measurements were made and reported that there is a correlation between the ionic to atomic spectral lines emission ratios and the surface hardness of solid steel targets. In 2006, Tsuyuki [2] published a paper showing a correlation between concrete compressive strength and shock speed, and that there is a positive relation of shock speed to the rate of ionization of ablated atoms. Establishing a link between intensity ratio of calcium emission lines and concrete strength, they deduced that a material hardness might be indicated by the analysis of laser-induced plasmas.

[0021] More recently, application papers [3-5] reported that a line-to-continuum ratio method was used to determine the plasma excitation temperature, T.sub.e′, and this also resulted in a linear relationship with the Vickers hardness number of the bio-12 ceramic material. The study showed that the neutral Mg(I) 278.30 nm and the ionic Mg(II) 279.55 nm emission lines were rated, and as indicated that changes in the values of the emission line ratio can be interpreted as a difference in the hardness of the target material.

[0022] Detecting another ionic Mg(II), @280.27 nm instead of Mg(II) @279.55 nm, a spectrometer with extended bandwidth, including UV range near 280 nm was employed. Although many elements are effective indicators, the ionic Mg(II) 280.270 nm to neutral Mg(I) 285.215 nm line pair is one of the most widely used [6-8]. This pair serves as an excellent indicator, as the two lines are relatively close to one another and can be acquired in the same spectral window for high-resolution monochromators. Additionally, the lines are very intense, and effective use requires only a small amount of Mg be present in the laser induced plasma. It only requires that Mg be present in the samples, or artificially added as a trace element. It is also important that there are no spectral interferences between the trace element and the other matrix elements.

[0023] As shown in FIGS. 3-4, the Mg(II) @280.27 nm and the Mg(I) @285.2 nm emission lines (instead of Mg(I) @278.30 nm) were rated, and it was observed that the value of the emission line ratio at the 1.sup.st layer is larger than that of 3.sup.rd layer, 2.5 to 2.3. The ratio was decreased to ˜10%. FIG. 5 shows the ratio between Mg(II) @280.27 nm and Mg(I) @285.20 nm on the substrate (AA7075) only, i.e., 2.1. If the changes in the values of the emission line ratio can be interpreted as a difference in the hardness of the target material, this invention recognizes that there is likewise a change in the strength of the material.

[0024] Similar research by a group of researchers reported that the strength in the clad region was decreased due to the loss of Mg and Zn in the application of laser repair of damaged AA7075 components [9-10]. This is not uncommon for Zn, as it has a low vaporization point (906° C.) and has vaporized during laser processing. Mg also has a relatively low vaporization point (1119° C.) and hence a small amount has been lost. The trend implies that high loss of Mg causes low micro-hardness, thereby, higher ratio between Mg(II) @280.27 nm and Mg(I) @285.20 nm as shown in FIG. 6.

[0025] Zn(I) @330.2 nm was also detected, but it is noted that the spectral intensity observed was weaker than Mg(I) and Mg(II) as shown in the above FIGS. 3 and 4. This is attributable that the higher atomic energy level (32501.99 & 62772.0 cm.sup.−1) to release Zn(I) @330.2 nm is needed than that to release Mg(I) @280.27 nm (0 & 35051.26 cm.sup.−1) and Mg(II) @285.2 nm (0 & 35669.31 cm.sup.−1) and laser AM is operated in relatively low laser energy density settings, comparing to other laser material processing.

[0026] Using the Saha-Eggert equation, which relates the ratio (I.sub.ion/I.sub.atom) of the two emission lines to the plasma ionization temperature (T.sub.ion) (assuming local thermodynamic equilibrium, LTE) [11-12],

[00001]$\frac{I_{ion}}{I_{\mathrm{atom}}}=\frac{4.83\times 10^{15}}{N_e}{\left(\frac{gA}{\lambda }\right)}_{ion}{\left(\frac{\lambda }{gA}\right)}_{\mathrm{atom}}\times T_{ion}^{3/2}\exp \left[\frac{-\left(V^{+}+E_{ion}-E_{\mathrm{atom}}-\Delta V^{+}\right)}{k{T}_{ion}}\right]$

where all terms have their usual meanings, a potential way to relate the hardness value to the plasma ionization temperature could be established. For the above ratios, plasma ionization temperature was calculated as 8603° K. for Mg(II)@280.27 nm at the 1.sup.st layer (FIGS. 3) and 8542° K. at the 3.sup.rd layer (FIG. 4).

[0027] Recently [14], temporal electron temperature was reported during laser-induced magnesium plasma of Laser Induced Breakdown Spectroscopy (LIBS) with different laser energies and several time delays and at laser energies of 100, 200 and 300 mJ at a delay time of 100 ns, the electron temperatures of Mg(I) were found to be 8810, 9303 and 9724 K, respectively. It is believed that the plasma ionization temperature (8603° K.) of Mg(II)@280.27 nm was calculated a bit lower than those by LIBS due to the laser processing condition (CW vs. pulsed). Table 1, below, presents emission-line data for Saha-Eggert's electron number density calculations [13-14].

TABLE-US-00001 TABLE 1 Emission-line data for Saha-Eggert's electron number density calculations Species 1 (nm, 10.sup.−7 cm) E (cm.sup.−1) g A (×10.sup.8 s.sup.−1) [00002]${\left(\frac{\mathrm{gA}}{\lambda }\right)}_{\mathrm{atom}}/{\left(\frac{\mathrm{gA}}{\lambda }\right)}_{\mathrm{ion}}$ Mg (I) 285.213 35087 3 5.0 Mg (II) 279.553 35732 4 2.6 1.4137 Mg (II) 280.270 35652 2 2.6 2.8346

[0028] Note that k=Boltzmann's Constant (8.6173303×10.sup.−5 eV K.sup.−1), N.sub.e˜2×10.sup.16 cm.sup.−1, 1=wavelength (cm), g=statistical weight of the emitting and ground level, E=energy level (eV), A=transition probability for spontaneous emission, V.sup.+=ionization potential of the lower ionization stage, ΔV+=a correction to the ionization potential V.sup.+ of the lower ionization stage due to plasma interactions. It is further noted that for Mg(II) @1=280.27 nm, g=2, A=2.6×10.sup.8 s.sup.−1, E.sub.ion=4.4223 eV (35669.31 cm.sup.−1), V.sup.+=15.035 eV (121267.64 cm.sup.−1), for Mg(I) @1=285.2 nm, g=3, A=5.0×10.sup.8 s.sup.−1, E.sub.atom=4.3457 eV (35051.26 cm.sup.−1), V.sup.+=7.6462 eV (61671.05 cm.sup.−1). V.sup.+ represents the ionization potential of the lower ionization stage; all other symbols have their usual meaning. There is a small correction to the final term, −ΔV.sup.+, which is a correction to the ionization potential V.sup.+ of the lower ionization stage due to plasma interactions [12]. ΔV.sup.+ is usually considered to be negligible for z=1, but for higher ionization states should be taken into account, and may be determined from the following references [11-12]:

ΔV.sup.+=+ze.sup.2/4πε.sub.0ρ.sub.D

where z is the ionization charge state, e the electron charge, ε.sub.0 the permittivity of free space and ρ.sub.D the Debye shielding distance. Considering a typical laser-induced plasma of T˜7000 K and N.sub.e˜2×10.sup.18 m.sup.−1, then it yields ρ.sub.D as approximately 2.96×10.sup.−9 m, which is considerably smaller than the dimensions of such a plasma, generally of the order of millimeters.

Relationship Between Micro-Hardness and Yield Stress, Tensile Strength

[0029] As shown in FIG. 7(a), the Vickers hardness-yield stress relationship in AA7010 has been developed from two independent datasets involving AA7010 plate and a rectilinear forging [16]:

σ.sub.Y(MPa)=0.383 H.sub.V−182.3

[0030] Also, an empirical relationship between tensile strength and Vickers hardness was also developed for AA7010 as shown in FIG. 7(b):

S.sub.T(MPa)=0.247 H.sub.V+113.1

[0031] The composition of the AA7010 plate used in above investigation is given in Table 2, below. AA7010 has a bit more Zn (˜6.26 wt %) than that (˜5.11%) of AA7075 and the empirical relation shown above may be utilized to estimate micro-hardness. Monitoring and evaluating the ratio of Mg(II)/Mg(I), micro-hardness can be predicted using the relationship developed using FIG. 7. In addition, thermal residual stress induced during the process may be estimated using aforementioned formula between micro-hardness and yielding stress and tensile strength.

TABLE-US-00002 TABLE 2 Chemical composition (in wt %) of AA7010 Si Fe Cu Mg Zn Zr Al Forging 0.03 0.06 1.69 2.44 6.26 0.14 Balance Plate 0.04 0.05 1.75 2.34 6.30 0.12 Balance

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