Home / Examples / Electric Analysis [Coulomb] / Example 9 Plating (Plating a Device in the Bath)

Example 9 Plating (Plating a Device in the Bath)

General

 

 

 

 

 

Analysis Space

Item

Settings

Analysis Space

3D

Model Unit

mm

 

Analysis Conditions

The material is conductor for the plating analysis.

Select the [Perform the plating analysis] option.

Item

Settings

Solver

Electric Analysis [Coulomb]

Analysis Type

Static Analysis (Resistance)

Material

Conductor

Options

Select Perform the plating analysis
Select Calculate the plating thickness
Plating Time: 300 [s]

Meshing Setup

General Mesh Size: 6.0 [mm]*1

 

Meshing Control
Select Place middle nodes of the 2nd-order elements on curves *2
Minimum Number of Tessellations for Curved Face: 12 *2

Matrix Solver Type

Direct Method*3

 

 

 

Graphical Objects

Box body (green) is the plating solution. As the target object for plating, a disc part (yellow) is placed in the box.

The disc part is a cathode. Anodes (red) are placed on both sides of the disc part.
Assuming that the protruding portion of the cylinder on top of the anodes are connected to the current power source, electric walls V1 and V2 are set on the anodes.
The disc part is supported by a conductive supporting body (blue) that flows current.
Assuming the end of the conductive part is connected to the ground, the electric wall of ground, GND, is set on the end.

Body Attributes and Materials

Create solid bodies for the plating bath, the anodes, the disc part (cathode), and supporter of the disc part (conductor). Body attributes are plating solution and metal.

Body Number/Type

Body Attribute Name

Material Name

3/Solid

Cathode

Metal

9/Solid

Anode

Metal

10/Solid

Anode

Metal

11/Solid

Cathode

Metal

12/Solid

Plating Solution

Solution

 

The body attribute is set as follows.

Body Attribute Name

Plating Tab

Anode

 

Type of Plating Body: Anode

 

Overvoltage Type: Linear

a1 [V]

0.0

A2 [Vm2/A]

5.0x10-5

 

Cathode

 

Type of Plating Body: Cathode

Extracted Metal Setting

Conductivity

50×106 [S/m]

Electrochemical Equivalent

100×10-9 [kg/(As)]

Density

10×103 [kg/m3]

Extraction Efficiency

1.0x100

 

Overvoltage Type: Tafel's Law

a1 [V]

5.0x10-2

a2 [Vm2/A]

1.0x10-1

 

Plating Solution

 

Type of Plating Body: Plating Solution

 

 

The material properties are set as follows.

Material Name

Conductivity Tab

Metal

 

Conductivity Type: Conductor

Conductivity: 10 x106 [S/m]

 

Solution

 

Conductivity Type: Conductor

Conductivity: 10 [S/m]

 

Boundary Condition

The boundary conditions are set as follows.

Boundary Condition Name/Topology

Tab

Boundary Condition Type

Settings

Ground/Face

Electric

Electric Wall

Ground

V1/Face

Electric

Electric Wall

Current 1 A

V2/Face

Electric

Electric Wall

Current 1 A

Results

Current density of the plating solution is shown in Fig. 1.
Bodies except the plating solution are hidden
because current density of the plating solution cannot be seen due to the current density of electrodes if the electrode bodies are shown.

The current from the anodes is observed to flow to the cathode which consists of the disc part and the supporting body.


Fig. 1 Distribution of current density in plating solution

 

 

 

Fig. 2 shows the current density (normal component) on the disc part's surface and
Fig. 3 shows the plating thickness extracted on the disc part, each in the form of contours. Only the disc part body is shown in both figures.
Both parts are placed such that the supporting body is on your side.
The supporting body is directed upward from the disc's center.
In Fig. 2, you can see the current density at the upper area of the part is small due to the absence of current by obstruction from the supporting body.
Fig. 3 shows that the plating thickness is distributed according to the current density distribution.

Fig. 2 Current density (normal component) on the surface of part

Fig. 3 Plating thickness extracted on the part

 

Fig.4 shows the contour of the electric potential on one of the anodes.
You can see that there is electric potential distribution in the anode and the distribution is taken into account in the analysis.

Fig. 4 Electric potential distribution of the anode

Model with plating wall

In this example, the bodies are created for the anode and cathode.
This method has the advantage that electric potential distribution in the electrodes can be taken into account.
It has, however, a disadvantage that the number of meshes increases according to the number of electrodes, and a longer time is required for calculation.
If the plating wall boundary condition is used instead of the electrode body,
it can reduce meshes and shorten calculation time while the electric potential distribution in the electrode cannot be taken into account.

 

Fig. 5 shows the model with the plating wall replacing the electric wall.
The plating solution body is cut out and hollow where the disc part is supposed to be.