BACKGROUND OF THE INVENTION
The present invention is directed to metal hardening processes and, more particularly, to a
method of hardening a beta titanium member.
In recent years, products made of titanium or of titanium alloy, both of which are lightweight
and hard, have become widely used. However, titanium and titanium alloy are active
metals and have low wear resistance. Also, surface processing of either material is extremely
difficult.
To overcome such problems, methods have been employed to increase the surface hardness
of members formed from such metals. Such methods include forming an outer hardened
layer via surface plating or hardening the product surface itself via nitriding or carburizing.
However, plating processes encounter the problems of poor adhesion between the plating layer
and the titanium surface and damage to the appearance of the titanium, and surface hardening via
nitriding or carburizing encounter the problems of coarsening of the product surface and extended
processing times.
Japanese published patent application nos. 2003-73796, 2002-97914 and 2001-81544 disclose
further surface hardening methods that employ oxygen diffusion to increase the wear resistance
of titanium products. For example, JP 2003-73796 discloses a surface hardening method
wherein a titanium member is heated while buried in a highly oxygen-absorbent powder. The
powder reduces the oxygen concentration of the atmosphere surrounding the titanium member by
physically preventing the titanium surface from coming into contact with oxygen. As a result, a
TiO oxygen diffusion layer is formed in the surface of the titanium member while minimizing
the formation of an oxidized outer surface layer.
Although the surface hardness can be increased using such methods, because the titanium
member must be buried in oxygen-absorbing powder each time processing is carried out, the
process is relatively inefficient and costly. Furthermore, because the titanium member is buried
in the oxygen-absorbing powder, the desired cooling rate cannot be obtained following the heat
processing, so an appropriate aging treatment cannot be performed.
SUMMARY OF THE INVENTION
The present invention is directed to various features of a method of hardening a beta titanium
member. In one embodiment, a method of hardening the surface of a beta titanium member
comprises the step of heating the beta titanium member in a gas mixture consisting essentially of
an inert gas and oxygen. Additional inventive features will become apparent from the description
below, and such features alone or in combination with the above features may form the basis of
further inventions as recited in the claims and their equivalents.
BRIEF DESCRIPTION OF THE DRAWINGS
Fig. 1 shows the basic construction of a particular embodiment of an apparatus for surface
hardening a beta titanium member;
Figs. 2A and 2B are graphs of surface hardness for various heat treating methods;
Fig. 3 is a bar graph of the results of friction testing beta titanium members when subjected
to the methods shown in figs. 2A and 2B; and
Fig. 4 is a cross sectional diagram of a surface hardened beta titanium member formed
according to the methods taught herein.
DETAILED DESCRIPTION OF THE EMBODIMENTS
Fig. 1 shows the basic construction of a particular embodiment of a beta titanium surface
hardening apparatus 10 in the form of a titanium melting furnace for surface hardening a beta
titanium member 11. In general, beta titanium member 11 is placed in a processing chamber S of
beta titanium surface hardening apparatus 10, and then beta titanium member 11 is heated in an
atmosphere comprising a gas mixture comprising oxygen and an inert gas such as argon gas. As
a result, heat processing can be carried out in an atmosphere having a lower oxygen concentration
than ordinary atmospheric air. In this embodiment, the oxygen concentration ranges from
approximately 0.05 vol% to approximately 20 vol% (preferably approximately 1.0 vol% to approximately
10 vol%), the heating temperature ranges from approximately 700°C to approximately
1000°C (preferably approximately 850°C to approximately 950°C), and the heat processing
time ranges from approximately 10 minutes to approximately 30 minutes (preferably approximately
15 minutes to approximately 25 minutes).
After this processing, titanium member 11 undergoes an aging treatment at an ambient
temperature of from approximately 400°C to approximately 550°C (preferably approximately
850°C to approximately 950°C) for a time of from approximately 6 hours to approximately 16
hours (preferably approximately 10 hours to approximately 14 hours).
Figs. 2A and 2B are graphs of surface hardness for various heat treating methods. In Fig.
2A, one line represents an unprocessed beta titanium member, another line represents a beta titanium
member subjected to an Argon-Oxygen atmosphere of 5 vol% oxygen at 850°C for 10
minutes, and another line represents a beta titanium member subjected to an Argon-Oxygen atmosphere
of 10 vol% oxygen at 850°C for 10 minutes. In Fig. 2B, one line represents an unprocessed
beta titanium member, another line represents a beta titanium member subjected to an Argon-Oxygen
atmosphere of 1.7 vol% oxygen at 900°C for 10 minutes, another line represents a
beta titanium member subjected to an Argon-Oxygen atmosphere of 5 vol% oxygen at 900°C for
10 minutes, and another line represents a beta titanium member subjected to an Argon-Oxygen
atmosphere of 10 vol% oxygen at 900°C for 10 minutes.
As shown in Fig. 2A, a beta titanium member that was processed at a temperature of
850°C for 10 minutes in an atmosphere having an oxygen concentration of 5 vol% exhibited an
HV hardness of 570-400 down to a depth of 0.10 mm (100 µm) below the surface, as compared
to the more or less fixed HV hardness of 400 for an unprocessed beta titanium member. In particular,
the HV hardness increased to 570-400 from the surface down to a depth of 0.05 mm (50
µm) below the surface. A beta titanium member that was processed at a temperature of 850°C for
10 minutes in an atmosphere having an oxygen concentration of 10 vol% also exhibited an HV
hardness of 570-400 down to a depth of 0.10 mm (100 µm) below the surface. In particular, the
HV hardness increased to 570-450 from the surface down to a depth of 0.05 mm (50 µm) below
the surface.
As shown in Fig. 2B, a beta titanium member that was processed at a temperature of
900°C for 10 minutes in an atmosphere having an oxygen concentration of 1.7 vol% exhibited an
HV hardness of 590-420 from the surface down to a depth of 0.10 mm (100 µm) below the surface,
as compared to the more or less fixed HV hardness of 450 for an unprocessed beta titanium
member. In particular, the HV hardness increased to 590-495 from the surface down to a depth
of 0.05 mm (50 µm) below the surface. A beta titanium member that was processed at a temperature
of 900°C for 10 minutes in an atmosphere having an oxygen concentration of 5 vol%
exhibited an HV hardness of 580-470 from the surface down to a depth of 0.10 mm (100 µm)
below the surface. In particular, the HV hardness increased to 585-515 from the surface down to
a depth of 0.05 mm (50 µm) from the surface. A beta titanium member that was processed at a
temperature of 900°C for 10 minutes in an atmosphere having an oxygen concentration of 10
vol% exhibited an HV hardness of 545-395 down to a depth of 0.10 mm (100 µm) from the surface.
In particular, the HV hardness increased to 545-490 from the surface down to a depth of
0.05 mm (50 µm) below the surface.
It should be readily apparent from the graphs in Figs. 2A and 2B that, with respect to the
temperature parameter, a temperature of 900°C resulted in a greater increase in hardness over a
greater range than a temperature of 850°C. More specifically, when the beta titanium member
was subjected to a processing temperature of 900°C, the HV hardness declined more gradually
beyond a depth of 0.02 mm (20 m) below the surface than it did when the beta titanium member
was subjected to a processing temperature of 800°C. Therefore, taking into consideration the
melting temperature of beta titanium, it is preferable that processing be carried out at a temperature
in the range of from approximately 850°C to approximately 950°C.
With respect to the oxygen concentration parameter, Fig. 2B shows that HV hardness increases
to a greater degree when the oxygen concentration is 1.7 vol% than when it is 5 vol%.
The same is true when the oxygen concentration is 5 vol% than when it is 10 vol%. Therefore, in
order to minimize the formation of an oxidized layer while increasing HV hardness, it is preferable
that processing be carried out within an oxygen concentration in a range of from approximately
1 vol% to approximately 10 vol%.
Fig. 3 is a bar graph of the results of friction testing beta titanium members when subjected
to the methods shown in Figs. 2A and 2B. The beta titanium member that was heated at
850°C for 10 minutes in an oxygen concentration of 5 vol% is referred to as a first sample, the
beta titanium member that was heated at 900°C for 10 minutes in an oxygen concentration of 10
vol% is referred to as a second sample, a beta titanium member that was heated at 900°C for 10
minutes in an oxygen concentration of 5 vol% is referred to as a third sample, and a beta titanium
member that was heated at 900°C for 10 minutes in an oxygen concentration of 1.7 vol% is referred
to as a fourth sample.
As shown in Fig. 3, the average amount of wear was 0.15 mm for the unprocessed beta
titanium member, 0.138 mm for the first sample, 0.132 mm for the second sample, 0.110 mm for
the third sample, and 0.104 mm for the fourth sample. Clearly, the average wear amount was
lower for the processed beta titanium members than for the unprocessed beta titanium member.
The average wear amount for the third and fourth samples in particular, which were processed at
900°C for 10 minutes, was approximately 30% lower than the wear amount for the unprocessed
beta titanium member. Thus, processing at a temperature in a range of from approximately
850°C to approximately 900°C results in wear resistance and surface hardness values that are
higher than the equivalent values for an unprocessed beta titanium member.
From a comparison between the first sample and the third sample, it may be seen that the
average amount of wear can be reduced when heating is carried out at 850°C than at 900°C. Accordingly,
heating at a temperature of 850°C may be preferred in some applications. Moreover,
from a comparison of the second through fourth samples, it may be seen that the average amount
of wear can be reduced by reducing the oxygen concentration from 10 vol% to 1.7 vol%, so such
oxygen concentration reduction also may be prefererable in some applications.
Fig. 4 is a cross sectional diagram of a surface hardened beta titanium member 11 formed
according to the methods taught herein. In this condition, beta titanium member 11 comprises a
topmost oxidized layer 11a, a hardened oxygen diffusion layer 11b having a thickness of approximately
100 µm below oxidized layer 11a, and an unprocessed layer 11c below hardened
layer 11b. Oxidized layer 11a has a thickness of from approximately 0 µm to approximately 5
µm. Such a layer is significantly thinner than the oxidized layers formed in the prior art processes
that heat the titanium member in atmospheric air. Thus, removal of oxidized layer 11a created
by the teachings herein is very easy.
In other words, because hardened layer 11b can be formed to a thickness of at least 70
µm (preferably 100 µm) while minimizing the thickness of oxidized layer 11a, a beta titanium
member 11 having increased surface hardness can be efficiently obtained. When the same processes
as described above are performed in atmospheric air, a hardened layer may be formed to a
thickness of 300 µm with an increased HV hardness of 500, but an oxidized layer having a
thickness of 100 µm is formed on top of the hardened layer. An oxidized layer on the surface of
the product is undesirable because it tarnishes the product's appearance. Since the oxidized layer
is hard and brittle, removal of such a thick layer is extremely cumbersome and impairs production
efficiency.
The processes described above have particular benefit when applied to beta titanium
members. When the process was applied to pure titanium and alpha-beta titanium alloys, a hardened
oxygen diffusion layer did not form. This is thought to be due to the fact that an oxygen
diffusion layer cannot be formed via melting of the surface of pure or alpha-beta titanium,
whereas such a layer can be formed in beta titanium by surface melting.
While the above is a description of various embodiments of inventive features, further
modifications may be employed without departing from the spirit and scope of the present invention.
For example, while argon gas was used solely as the inert gas, other inert gases could be
used alone or in combination argon in addition to the oxygen. The size, shape, location or orientation
of the various components may be changed as desired. Components that are shown directly
connected or contacting each other may have intermediate structures disposed between
them. The functions of one element may be performed by two, and vice versa. The structures and
functions of one embodiment may be adopted in another embodiment. It is not necessary for all
advantages to be present in a particular embodiment at the same time. Every feature which is
unique from the prior art, alone or in combination with other features, also should be considered
a separate description of further inventions by the applicant, including the structural and/or functional
concepts embodied by such feature(s). Thus, the scope of the invention should not be limited
by the specific structures disclosed or the apparent initial focus or emphasis on a particular
structure or feature.