Not applicable.
Not applicable.
This invention relates generally to additive layering techniques, particularly those using an emitted energy source such as in additive metal layering.
Additive metal deposition is an industrial technique that builds fully-dense structures by melting powdered or wire metal, via a laser or other energy source, into solidifying beads, which are deposited side by side and layer upon layer upon a workpiece substrate. It is known to utilize the process to repair and rebuild a worn or damaged component using a laser to build up structure on the component. The process is particularly useful to add features such as bosses or flanges on subcomponents of fabricated structures. The basic process involves adding layers to the component to create a surface feature on the component via the introduction of depositing material (delivered in the form of injected powder or a wire) into a laser beam. The additive process is known by several names including “laser cladding,” “laser metal deposition,” “direct metal deposition” or “additive metal layering.”
Additive metal layering is typically performed by using a computer aided design (“CAD”) to map the geometry of a part (known as a “build”) and then depositing metal, layer-by-layer, on the part. The CAD mapped geometry is input into a computer controlled (robotic) part handler that can manipulate the part in multiple axes of movement during the deposition process. In all of these techniques a heat source (typically an industrial laser beam) is used to create a melt pool into which a wire or powdered feedstock is fed in order to create beads upon solidification. In practice, the heat source is under computer numerical control and is focused onto a workpiece, producing the melt pool. A small amount of powder or wire metal is introduced into the melt pool, building up the part in a thin layer. The beam follows a previously determined toolpath. The toolpath is generated based on the CAD data that computes the needed build layer by layer. The beads are created by means of relative motion of the melt pool and the substrate, e.g. using an industrial robot arm or an XY-table. A part is then built by depositing the beads side by side and layer upon layer. The most popular approach combines a high-power laser heat source with metal powder as the additive material.
Careful tuning of the deposition tool and parameters, such as the powder or wire feed rate, the energy input, and the traverse speed are therefore important in order to obtain layers, which are free from defects such as shape irregularities, lack-of-fusion or cracks. Droplet forming, i.e. globular transfer of the molten metal, is also a common disturbance that affects the geometrical profile of the deposited beads and stability of the additive layers.
Creating an accurate geometric description of, and tool path for, the build to be fabricated is critical to system operation and achieving a high-quality layered end product. The currently known laser additive processes attempt to generate a geometric description using a homogeneous, full geometry representation of the part to program the in-process tool path. This current method is depicted in
Using the current processes for generating a geometric description, the build process runs into a problem. This is shown in
The present invention addresses the deficits of the prior art by providing for a method of generating a geometric description of a part along with a build sequence for use in an additive layer process that creates the part. The method involves decomposing the overall geometry of the part into substructures that can be sequentially additively manufactured.
The present invention thus enhances the additive manufacturing process by incorporating the ability to pre-process overall part geometry into manufacturable pieces by a purely topological approach, and unlike the prior art does not strictly rely on drawing standards or modeling feature information to dictate the tool path. The decomposition technique is adaptable to individual manufacturing methods as it arises from formalizing via heuristics and mathematics how a process expert would choose to decompose a component for additive manufacturing.
The inventive decomposition method is integrated into an additive layering method and system. It has particular useful application in an additive layering method and system utilizing a power prediction method that calculates optimum beam power for any point P(s) along the additive path, particularly the method disclosed herein that utilizes a calculated idealized geometry for each point P(s) along the additive path and wherein the idealized geometry for each point P(s) comprises a melt pool, hot zone and bulk portion.
In one embodiment of the present invention an additive layering process for building a part having an overall geometry by way of an additive layering process includes creating a build description (refined geometric description and build sequence) for the part according to the decomposition process described below. After the part has been decomposed into substructures that can be sequentially built and the build sequence created, the part is built by additive layering by building each substructure of the part in accordance with the build sequence, which may typically be the same sequence by which the part was virtually decomposed.
The decomposition process can be understood in view of
As shown in
The geometric description and build sequence of the part that forms the build description is created by decomposing the overall geometry of the part by identifying a first substructure 2a of the part. The first substructure has a first starting surface 3a and a first interrogation interval 4a. The first starting surface 3a represents a surface at which additive layering of the first substructure can begin. The first interrogation interval 4a is defined by a first overhang angle θ1 and a first interval height δ1.
The overhang angle θ represents an amount of material overhang for each substructure that is allowed by virtue of the equipment and process employed. For example, some equipment can better articulate a part, which would allow for more overhang. Also, the material involved and temperature environment will affect allowable overhang. In this respect, different materials have different surface tensions which results in different overhang parameters. Also, the gas used in the build chamber will also affect the allowable overhang. These factors are used to select the allowable overhang that can be tolerated during building of a substructure.
With respect to the interrogation interval, the smaller the interval height δ, the better. The interrogation interval height should be selected as close as possible to the layering thickness of the machine environment to better represent the geometry of the subject substructure. In the figures the interrogation interval is oversized for purposes of visual ease.
The first substructure 2a is virtually decomposed by starting from the first starting surface and sequentially subtracting layers of interrogating intervals defined by the first overhang angle θ1 and a first interval height δ1 from first substructure 2a until the first substructure is removed and only a second portion of part 1 remains. From this second portion, a second substructure 2b is identified. Second substructure 2b has a second starting surface 3b and a second interrogation interval 4b. As with the first substructure, the second starting surface 3b represents a surface at which additive layering of the second substructure 2b can begin, the difference being manufacture of the second substructure 2b would commence once the first substructure 2a is additively manufactured. The second interrogation interval 4b is defined by a second overhang angle θ2 and a second interval height δ2. The second substructure 2b is virtually decomposed by starting from the second starting surface 3b (which, as shown in the drawings, is contiguous with a portion of the first substructure) and sequentially subtracting interrogation intervals (i.e., layers) 4b defined by the second overhang angle θ2 and a second interval height δ2 from the second substructure 2b until second substructure 2b is virtually decomposed.
If after decomposing a substructure, no portion of the part remains, the process of creating the refined geometric description and build sequence terminates. Otherwise, this process of creating the build description is repeated and continues for so long as any portion of the part remains. In other words, for each remaining portion of the part a next substructure is identified along with a starting surface and an interrogation interval. Each interrogation interval has a defining overhang angle θ and interval height δ. Hence, in the process depicted in
The decomposition process can be described mathematically via the following equations.
Gisect=Gremainder\Gint (a)
G
model
=G
remainder∪(Gisect) (b)
where
S
continuation=Γ(Gremainder; Gremoved) (c)
where
One embodiment method for building a part having an overall geometry by way of an additive layering process comprises creating a refined geometric description of the part by decomposing the overall geometry of the part. This is done by identifying a first substructure of the part. The first substructure has a first starting surface and a first interrogation interval. The first starting surface represents a surface at which additive layering of the first substructure can begin. The first interrogation interval is defined by a first overhang angle θ1 and a first interval height δ1. The first substructure is virtually decomposed by starting from the first starting surface and sequentially subtracting layers equal to the first interrogation interval from the first substructure until the first substructure is removed and only a second portion of the part remains. A second substructure from the second portion of the part is identified. The second substructure has a second starting surface and a second interrogation interval. The second starting surface represents a surface contiguous with the first substructure and at which additive layering of the second substructure can begin once the first substructure is additively manufactured. The second interrogation interval is defined by a second overhang angle θ2 and a second interval height δ2. The second substructure is virtually decomposed by starting from the second starting surface and sequentially subtracting layers equal to the second interrogation interval from the second substructure until the second substructure is removed. This process is continued for so long as any portion of the part remains. The starting surface for a later identified substructure represents a surface contiguous with a previously decomposed substructure and at which additive layering of that later identified substructure can begin once the previously decomposed substructure is additively manufactured. Once the part is fully decomposed, a sequence is determined for building by additive layering all of the substructures previously identified. The part is built by additively layering each substructure of the part in the sequence determined.
In another embodiment, the invention is directed to a method of controlling beam power during an additive deposition process employing a beam source at a point P(s) along an additive path that will be traveled to form a part during the additive deposition process. The method comprises creating a build description for the part by the decomposition and build sequence determination process described above. A path description is created based upon the build description that represents the path of the beam source through space during the additive process. The mass of the part is calculated at a point P(s) during the additive process based upon the build description. The power of the beam emitted by the beam source at the point P(s) of the additive path is modulated based upon the mass of the part at the point P(s) during the additive process.
In another embodiment the invention is directed to a system for fabricating a part on a substrate using a deposition beam source that emits a beam that follows an additive path composed of a plurality of points. The system comprises a substrate support for supporting the substrate and manipulating it through space and a metal stock delivery system. The system further includes a controllable beam source capable of emitting a beam onto the substrate and adapted to form a melt pool thereon. The system has a database for storing a build description as described above for the part. In this respect, the build description comprises: a first identified substructure of the part and one or more additional identified substructures of the part, with each additional identified substructure being contiguous with at least one other substructure of the part; and a build sequence for the part that sets forth a sequence of building by additive layering each of the identified substructures. The system includes a controller adapted to control power to the beam source. The controller is programmed to receive as an input the build description and regulate energy of the produced beam for any point on the additive path based upon the build description.
The decomposition process described above has been incorporated into a system and method for calculating a heat source power schedule for additive manufacturing. In this respect the decomposition method described above can be used to create the build description for a part, which build description can then be used in the below-described laser power prediction method. The method utilizes the following items to create an improved thermodynamic model of the work piece to compute needed laser power at intervals during the additive process. The method does so using: a) an additive path describing the path of the laser through space; b) a geometric representation of the geometry that the additive path is intended to create (i.e., the build description method described above); c) a description of the thermodynamic characteristics of the manufacturing environment; and d) computed thermophysical characteristics of the materials involved. This model is used to predict an appropriate input laser power at definable intervals along the laser path. It accomplishes this by using the path and geometric representation of the part being produced to create an idealized geometry that allows for tenable calculations.
As shown in
The laser power input is calculated by performing an energy balance calculation at intervals along the laser's path with the following considerations:
1. Conduction from the melt pool to the hot zone;
2. Conduction from the hot zone to the bulk of the particular workpiece;
3. Conduction from the bulk of the part to the clamping system of the CNC machine;
4. Radiation from the melt pool;
5. Radiation from the hot zone;
6. Convection from the melt pool;
7. Convection from the hot zone;
8. Convection from the bulk structure;
9. Process activity at the current point (i.e. is the laser supposed to be on now or not?);
10. Mass of the hot zone; and
11. Area for conduction between the hot zone and bulk structure.
Relevant to describing and demonstrating the inventive method are the following elements and symbols, which have the meanings indicated.
An exemplary calculation method thus proceeds as follows. First, before beginning the formal calculations representing the in-process thermodynamic environment, initial values are input based upon the starting temperature environment
Initialize the energy content of the part:
Hbuild=CpTambmsub (1)
Initialize the mass of the part:
mbuild=msub (2)
Initialize the temperature of the part:
Tbuild=Tamb (3)
Initialize the hot zone temperature:
Thot=Tbuild (4)
Set the path to begin at the beginning:
s=0 (5)
Useful constants should be then pre-calculated.
Maximum volume of the hot zone:
V
max=2/3r3hotπ (6)
Maximum area of the hot zone:
Amax=2r2hotπ (7)
Approximate surface area of the melt pool:
A
melt=1/4w2π (8)
Mass per unit length of deposition
mul=wdlρ (9)
Time for the laser to traverse one calculation interval:
Δt=ip/f (10)
With the above initial pre-calculation steps undertaken, one can proceed to calculate needed laser power along a given deposition path according to the following method.
A. Calculate the geometry index for the current position.
V
hot
=G∩Z(rhot, P(s), t′(s)) (11)
A
hot
=V
hot
A
max
/V
max (12)
B. Compute the energy balance at the melt pool.
H
rad
=εσA
melt(T4melt−T4env)Δt (13)
H
cond
=kA
hot
/r
hot(Tmelt−Thot)Δt (14)
H
conv
=hA
melt(Thot−Tenv)Δt (15)
C. Compute the laser power.
H
powder
=m
ul
i
p((Tmelt−Tp)Cp+Hf) (16)
H
remelt
=m
ul
i
p
r((Tmelt−Thot)Cp+Hf) (17)
H
total
=H
powder
+H
remelt
+H
rad
+H
cond
+H
conv (18)
Q
laser=min(Qmax, Htotal/αΔt) (19)
D. Update the mass of the build.
m
build
=m
build
+m
ul
i
p (20)
E. Calculate the energy losses at the build.
r
build=3√{square root over (3mbuild/ρ4π)} (21)
Abuild=4r2buildπ (22)
H
hot
=εσA
hot(T4hot−T4amb)Δt (23)
H
mach=(kAmachine/rbuild)(Tbuild−Tmach)Δt (24)
H
env
=hA
build(Tbuild−Tamb)Δt (25)
F. Update enthalpy of the build.
H
build
=H
build
+Q
laser
Δt−H
mach
−H
hot
−H
env (26)
G. Update the build temperature.
T
build
=H
build
/C
p (27)
H. Update the hot zone temperature estimate.
T
hot=(Tbuild+Ttarget)/2 (28)
I. Update the position along the deposition path.
s=s+i
p (29)
J. If the path is not complete, return to step 1.
These calculations are carried out in sequence with each result being an input for the next step in the process. For example, during the calculation of a laser power schedule for a 56.5 mm long×3.3 mm wide×190 mm tall rectangular structure (approximately 500 layers, ˜20 minutes of real machine time), the laser power prediction algorithm calculated the appropriate laser power for 14502 discrete points along the path.
With the foregoing explanation, it will be appreciated that in one embodiment the inventive method is a power schedule calculation method for an additive deposition process using a beam source that using the decomposition process described above to create a geographic description and build sequence for a part calculates optimum beam power for any point P(s) along an additive path that will be traveled to form the part, the part having a geometry and being formed from deposited material added to a structure, the point P(s) along the additive path having associated with it an idealized geometry comprising a melt pool, hot zone and bulk portion.
As shown in
With step 111 completed, the geometry factor computation 104 is completed and the calculation proceeds to compute laser power at step 105.
Having explained the method mathematically, the inventive method can be verbally summarized and described. In summary description, the method comprises using the decomposition process described above to create a geometric description representing the refined (substructure constituency) geometry and build sequence of the part during the additive process and creating a path description that represents the path of the beam source through space during the additive process. The method further includes calculating the idealized geometry for a point P(s) on the additive path based upon the geometric description and path description. In addition, the method includes calculating an energy balance at the melt pool (EBmelt pool) for the point P(s) on the additive path, the energy balance calculation being based upon the following calculations:
a) a calculation of energy radiated from the melt pool (Hrad);
b) a calculation of energy conducted from the melt pool to the hot zone (Hcond), the calculation of Hcond being based upon the calculated idealized geometry; and
c) a calculation of energy lost due to convection at the melt pool (Hconv);
The method further includes calculating total energy (Htotal) needed at the point P(s) on the additive path according to the following equation
H
total
=H
deposited material
+H
remelt
+EB
melt pool
wherein Hdeposited material represents energy required to melt the deposited material and Hremelt represents energy required to remelt existing material; and
The last step of the first embodiment of the inventive method includes calculating optimum beam source power Qsource for the point P(s) according to the following equation
Q
source=min(Qmax, Htotal/αΔt)
wherein Qmax represents maximum laser power, α represents a beam absorption coefficient and Δt represents a calculation interval.
The first embodiment inventive method can be refined further by enhancing the calculation of the idealized geometry by calculating a geometry index hot zone volume (Vhot) for the point P(s) on the additive path according to the formula
V
hot
=G∩Z(rhot, P(s), t′(s))
wherein G represents deposition geometry, Z represents a hemisphere of a certain radius (r) and having a circular surface centered at a point P(s) on the additive path with a normal direction ({hacek over (n)}), rhot represents the radius of the hot zone and t′(s) represents tool axis direction at a distance s along the additive path; and
calculating a geometry index hot zone area (Ahot) for the point P(s) on the additive path based upon the calculated geometry index hot zone volume (Vhot) according to the formula
A
hot
=V
hot
A
max
/V
max
wherein Amax represents the maximum area of the hot zone and Vmax represents the maximum volume of the hot zone
The first embodiment inventive method can be refined further by calculating EBmelt pool according to the formula
EB
melt pool
=H
rad
+H
cond
+H
conv
In another embodiment, the invention is directed to a power schedule calculation method for an additive deposition process using a beam source that calculates optimum beam power for any point P(s) along an additive path that will be traveled to form a part, the part having a geometry and being formed from deposited material added to a structure, the point P(s) along the additive path having associated with it an idealized geometry comprising a melt pool, hot zone and bulk portion. This method comprises creating a part geometry description and build sequence using the decomposition technique described herein that will represent the geometry of the part during the additive process and creating a path description based upon data representing the path of the beam source through space during the additive process. The method also involves calculating the mass of the part at a point P(s) during the additive process that accounts for accretion of the part during the additive process and calculating the idealized geometry at point P(s) during the additive process, the idealized geometry calculation calculates the size of the melt pool, hot zone and bulk portion. Additionally, the method involves calculating the temperature of the part at point P(s) during the additive process, the calculation of the temperature of the part includes a calculation of hot zone temperature based upon the idealized geometry.
The second embodiment method further comprises calculating an energy loss of the part at point P(s) during the additive process, the calculation of energy loss being based upon the calculation of temperature and including a calculation of energy conducted from the melt pool to the hot zone; calculating an enthalpy of the part at point P(s) in time during the additive process; calculating total energy needed at the point P(s) based upon the calculated energy loss and enthalpy of the part at point P(s) on the additive path; and calculating an optimum beam source power based upon the calculation of total energy needed.
Using the calculations above, the laser energy delivered during an additive path deposition process can be controlled for each point along the path by regulating power to the laser at each point in accordance with the required power predicted by the above calculation methods. As such, in another embodiment of the invention the method can be programmed into a computer-controlled laser metal deposition system to improve the fabrication of component of almost any geometry or build description that can be produced from a computer database. This system for fabricating a part on a substrate using a deposition beam source that follows an additive path is depicted in
The process described herein can also be used in connection with other traditional welding techniques, such as tungsten inert gas (“TIG”) welding, gas metal arc welding (“GMAW”), plasma transferred arc (“PTA”) welding and electron beam (“EB”) welding. While the embodiments of the method and system of the present invention have been described herein, numerous modifications, alterations and changes to the described embodiments are possible without departing from the scope of the invention. The embodiments described herein are not intended to be limiting.
This application is a continuation-in-part of U.S. patent application Ser. No. 14/474993 entitled “System and Method for Determining Beam Power Level Along an Additive Deposition Path.” The full contents of that application are herein incorporated by reference.
Number | Date | Country | |
---|---|---|---|
Parent | 14474993 | Sep 2014 | US |
Child | 14643812 | US |