A multi-high-energy beam-enhanced in situ method for measuring vapor recoil pressure in additive manufacturing
A technology of additive manufacturing and measurement methods, which is applied in the directions of measuring fluid pressure, processing and manufacturing, and additive manufacturing. It can solve problems such as low measurement efficiency, small quantity, and restrictions on in-depth research on steam recoil behavior, so as to achieve easy capture and improve efficiency. Effect
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Embodiment 1
[0056] In this example, gas-atomized GH4169 alloy spherical powder is used, and the particle size range of which is measured by Mastersizer 3000 is D10=21.7 μm, D50=31.1 μm, D90=45.0 μm. The chemical composition of the GH4169 superalloy powder is shown in Table 1.
[0057] Table 1 Chemical composition of GH4169 superalloy powder used in the experiment
[0058] Al Ti Cr Mn Fe Mo Nb C Ni 0.56 1.01 18.94 0.01 18.23 3.0 4.98 0.04 Bal.
[0059] Taking the typical backward deflected splash particles under dual high-energy beams as the object, the related vapor back ramming behaviors are studied as follows:
[0060] using as figure 2 For the measurement system shown, set the two laser beams at the same laser power (500W) and the same scanning speed (1000mm·s -1 ) and the same spot size (130 μm) run forward and backward on the powder bed. The #1 laser is defined as the front row laser, the #2 laser is the rear row laser, and the #2 laser is...
Embodiment 2
[0070] like Figure 5 Shown is the deflection diagram of the motion trajectory of the upper surface of the splash S2 under the action of photo-induced vapor recoil (high-speed imaging timing diagram). Splash S2 is emitted under the action of #1 laser vapor entrainment, at t =1350μs is captured by the backward #2 laser, causing its temperature to rise sharply, reaching the boiling point T b , the upper part of the splash particles begins to vaporize. like Image 6 As shown, the resulting metal vapor exerts a downward recoil pressure on the particles, resulting in drastic changes in their trajectory. exist t=1350μs~1370μs in a very short time, the exit angle of the sputter S2 changes from 162.2° to -96.5° (the negative sign means vertical downward), the vertical component of the exit velocity u v from 0.9m s -1 Change to -11.4m s -1 . The acceleration of the particle can be calculated by taking the derivation of the velocity-angle-time curve of motion a p . At the t...
Embodiment 3
[0072] like Figure 7 Shown is the deflection diagram of the motion trajectory of the upper surface of the splash S3 under the action of photo-induced vapor recoil (high-speed camera timing diagram). Splash S3 emerges under the action of #1 laser vapor entrainment, at t =1740μs was captured by the backward #2 laser, causing its temperature to rise sharply, reaching the boiling point T b , the upper part of the splash particles begins to vaporize. like Figure 8 As shown, the resulting metal vapor exerts a downward recoil pressure on the particles, resulting in drastic changes in their trajectory. exist t =1740μs~1760μs in a very short time, the exit angle of the sputter S3 changes from 180° to -107.4° (the negative sign means vertical downward), the vertical component of the exit velocity u v From about 0m s -1 Change to -6.2m s -1 . The acceleration of the particle can be calculated by taking the derivation of the velocity-angle-time curve of motion a p . At the ...
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