技術レポート

An Analysis of the Porosity Producing Mechanism

H.Fukanuma
Plasma Giken Co.,Ltd.
Saitam Prefecture
Toda City,Japan

Abstract

It is well-known that thermal spray coatings have porosity,but the reason why the porosity is produced in thermal spray coating processes is not known.Although many qualitative discussions have been done about porosity in thermal spray coatings.This paper proposes a physical and mathematical model of the porosity producing mechanism,and flattening process of the molten particle on the surface of the substrate or the coating after the molten particle impinges onto the substrate or the coating in thermal spray processes.This paper theoretically describes that atmospheric gas contributes to producing porosity in the thermal spray process and that there is a distribution of pores between the splat and the substrate or between splats.

IT IS KNOWN that the boundary structure between splats or between the substrate and splats greatly affects the physical characteristics of thermal spray coatings.In particular,porosity in the coating is an important factor in understanding characteristics of coatings.At present,the structures of splat interfaces are being clarified by various studies(1-4);but there is no established theory on the formation mechanism of pores between splats or between the substrate and splats.In this paper,the porosity formation mechanism of coatings is mathematically analyzed under several assumptions.

Theory

Definition of porosity.The structure of coatings is considered to be lamellar shown in Fig.1.An enlarged interface between splats or between the substrate and splat is shown in Fig.2.The porosity ƒp of coatings is defined as follows,

null

null

where

null

The total volume of pores Vg in coatings is defined as follows,

null

where

null

According to Eq.2,the integration is carried out for the surface area of every splat,so integration is performed twice for every splat interface.Therefore,the resultant value divided by 2 represents the total volume of pores.

A mathematical model of porosity formation.The cross section profile of the surface of a substrate or thermal spray coating is assumed to be as shown Fig.3;namely,there are many holes on both surfaces.The total volume of holes on a unit surface area is assumed to be V0.

null

A molten disk particle impinges onto the surface at velocity ν0 as shown in Fig.4.It is assumed that molten particle flows only perpendicularly to the surface,but not parallel to the surface.The molten particle compresses the gas in the holes on the surface.Then,the gas volume changes from V0 to V.Also,it is assumed that the gas is an ideal gas and the pressure and volume of the gas change in a polytropic action.The gas pressure P in the holes is;

null

where

V= the volume of gas in the holes on a unit surface area,

k1= a constant,

n >1

It is assumed that no gas is released from the molten particle and the substrate,the compressed gas is completely released through the interface between splats or between the substrate and splat after the solidification of the molten particle.Also,it is assumed that the work to compress the gas from V0 to V in the holes on a unit surface area is proportional to the kinetic energy of molten particles whose volume equals the compressed volume (V0-V) of the gas.Then,the next equation can be derived as

null

where

ν0= the impinging velocity of molten particle,

ρ= density of molten particle,

k2= a constant.

On substitution of Eq.3 into Eq.4 the next equation is;

null

where

P0= the initial pressure of the gas in the holes.

null

If V/V0,then Eq.5 can be written as;

null

Eq.5 and 6 describe that the volume of pores depends on the impinging velocity of a molten particle,the initial pressure of gas in the holes and the density of molten particles.

The flattening process of molten particle.In the preceding paragraph,the gas compression process in holes was described without consideration of the parallel flow of a molten particle to the surface of the substrate or the coating after impingement.The flattening process of a molten particle must be considered in the porosity producing model.It is assumed that the molten particle is flattened after impingement on the substrate or the coating as shown in Fig.5.Further assumptions are;

1)The impinging particle is completely molten.
2)The particles impinge perpendicularly on the substrate or the coating.
3)The density and viscosity of the molten particles are constant during flow and deformation processes.
4)Flattening is completed before solidification.
5)The thichness h of a flattening particle is constant in the region of r ≥ R0 during the flattening process.

null

6)The energy dissipation of a molten particle by viscous work is negligible in the region of r ≥ R0.
7)Gravity can be neglected.

A cylindrical coordinate is used,and the flow velocity field ν(ν1,νθ,νz) in the region of r ≥ R0assumed to be as follows.Since the flow of a molten particle is symmetrical around the zaxis,then νθ = 0,and there is no flow in the z direction,i.e.νz=0.νr,is assumed to be represented by the next equation,as C(t) is a function of time.

null

C(t) is assumed to be;

null

where

t= time,

ν0= |ν0|

Velocity ν fulfills the continuous equation as follows;

null

The volume of fluid in the range of R0 ≤ r ≤R is equal to the volume flowing out of the region of r < R0 in time from t = 0 to t = t. Therefore,the next equation follows.

null

Eq.10 is calculated as follows;

null

with the assumption that R = Rm when t = ∞,

null

If the velocity field in the region of r ≥ R0 is νr,then the viscosity coefficient of the fluid is μ,and the volume of the fluid in the region r ≥ R0 is Ν.This dissipated energy Φ of the fluid per unit time due to viscous work is written as follows;

null

When the surface tension of the molten particle against atmospheric gas,interfacial tension between the molten particle and substrate or coating,and kinetic energy of the molten particle at the time of impingement are γ,γSL and Ek respectively,Eq.14 holds.

null

Where

S0= the surface area of the molten particle before impingement,

S1= the contact area of the splat on the substrate or the coating after the flattening process is completed.

If the contribution of surface tension and interfacial tension can be negligible,Eq.14 can be written as Eq.15,

null

where d is the diameter of the molten particle before impingement.Since h = d3/6Rm2,the solution of Eq.15 leads to

null

When R0/Rm is small,Eq.16 can be written as

null

null

where

D=2R

d=2R0/ε

When ε=1,then approximation of the formula within the second parenthesis of Eq.17 by a line proportional to D/d in the range from about 3 to 10 of D/d results in;

null

Fig.6 shows the relations between impinging velocity ν0 and D/d in Eq.16,Eq.18 and Madejski’s theory(5).Calculation of the expansion rate νR of the splat radius from Eq.11 and 12 leads to;

null

And calculation of R/R0 from Eq.11 and 12 leads to;

null

On substitution of Eq.18 into Eq.20,R/R0 can be calculated.Fig.7 shows the time dependence of R/R0 during about 10-5sec required for the molten particle to spread.

Compression of gas in the flattening process.The mechanism of porosity formation during impingement and the deformation flow of molten particle is described in this subsection.The porosity formation model described in the preceding paragraph is applied to the flow process in which the splat is formed.The figure of the particle after a very short time at impingement is shown in Fig.5(b)where t = 0.When the contact area between the particle and substrate is small like this case; the theory described in the preceding paragraph can be directly applied to the process by which the gas in holes on the surface of the substrate is compressed.Then,it is assumed that νz = ν0 in the region of r < R0.On the other hand,in the region r ≥ R0,it is assumed that the compression energy of the gas in holes corresponds to the kinetic energy of the expansion of the splat radius.The volume of pores between the splats or between the splat and the substrate Vs is written as Eq.21 using Eq.6. WhenVR→0,Eq.5 instead of Eq.6 must be used,i.e.,in the neighborhood of R = Rm,so the parameter ζ is used. This is a positive number close to 1. null

Substituting Eq.19 into Eq.21 results in;

null

Calculating Eq.22 to substitute n=1.5,n=2,
when n=1.5,Eq.22 results in;

null

when n=2,Eq.22 results in;

null

Since the values of k2 and k3 are less than 10 at most,the first and third terms within the parentheses in Eq.23 and Eq.24 can be negligible as compared to the second terms.Eq.23 and Eq.24 can be written as follows, respectively;

null

where;

null

Since the volume of solid splat is approximately equal to the volume of the molten particle,then the volume of splat VS is πd3/6.Vg/VS can be written as Eq.29 and Eq.30,respectively.

null

null

null

If ƒp and ƒp0 denote the porosity of coatings at the impingement velocity ν and ν0,then the porosity ratio ƒp / ƒp0 is;

null

where

Vg= the volume of pores after solidification when the impinging velocity is ν,

Vg0= the volume of pores after solidification when the impinging velocity is ν0.

Fig.8 shows the relation between impingement velocity &nul and porosity ratio ƒp/ƒp0 which is normalized under the condition of ƒp0 = 0.1 at an impingement velocity of 100m/sec,i.e.by expressing 10% porosity as 1.Fig.9 shows the porosity dependence of the atmospheric pressure in the thermal spray process.When the total volume of pores from the splat center to its radius R is defined as Vgr,Vgr can be written as;

null

When n=2,calculation of the ratio Vgr/Vg results in Eq.33.

null

The results are given in Fig.10,indicating that most of pores exist in the area from 0.6 to 1Rmof the splat.

Discussions

The relations shown in Fig.8 and Fig.9 seem to be very close to empirical facts.The polytropic exponent n is probably between 1.5 and 2.

null

According to this theory,most of the pores between the splats or between the splat and the substrate exist in the periphery of the splat.Figure 10 indicates that most of the pores are distributed outside 0.6-0.8Rm of the splat.Accordingly,the volume of pores is very little in the central 36 to 64% area of splat,existing mostly in the peripheral 36 to 64% area.However,this does not mean that no pores exist in the central areas;but refers only to the relative amounts of pores existing in the interface between the splats or between the splat and the subatrate.The above fact suggests that the real contact area which is effective for bonding between the splat and the coating or between the splat and the substrate becomes larger in the central part of the splat.The splat central area equivalent to the diameter of the molten particle before impingement onto the substrate contributes to bonding between the splat and the substrate or between the splat and the coating.Then the bonding force becomes smaller in the peripheral part of the splat.

It must be considered that the action of wetting between the splat and the substrate contributes to the bonding force.If wetting action between the molten particle and the substrate is not taken into account,in the assumption for compressing the gas in the hole,then the end of the molten particle in the hole will solidify into the shape shown in Fig.11-b.On the other hand,if the splat and the substrate are easy to wet,then the particle will solidify into the shape shown Fig.11-a.The contacting area between the splat and the substrate in Fig.11-a is larger than that in Fig.11-b.Because the time required from impingement to flattening is probably about 10-5sec,then the degree of progress of wetting is an important problem associated with the bonding strength of thermal spray coatings.The analysis of dynamic phenomena on the wetting process is therefore necessary.

References

1. McPherson,R.and Shafer,B.V.,Thin Solid Films 97,201-204(1982)
2. McPherson,R.,Thin Solid Films 83,297-310(1981)
3. Safai,S.and Herman,H.,Thin Solid Films 97,201-204,(1982)
4. Arata,Y.Ohmori,A.and Li,C.,Proceedings of ATAC’88,Osaka,Japan.(May,1988)
5. Madejski,J.,Int.J.Heat Mass Transfer,19,1009-1013(1976)