Transient Nucleate Boiling and Its Use for Thermomechanical
Technologies Development
NIKOLAI I. KOBASKO
Intensive Technologies Ltd. Kyiv,
UKRAINE
Abstract: - In the paper high temperature and low temperature intensive thermomechanical treatment is
discussed. It is based on recently discovered new three physical principles that belong to the transient nucleate
boiling process taking place in cold fluids. Such processes are considered in conditions when any film boiling
during quenching in cold fluids is completely absent. That makes nucleate boiling very intensive, i.e.
Bi
V
.
The discoveries are used for direct quenching articles after forgings. The first is intensive high-temperature
thermo-mechanical treatment (HTTMT). It is used for low and middle-carbon alloy steels. Forged steel parts
are intensively quenched with a cooling interruption at the proper time to form surface compression residual
stresses and fine bainitic microstructure at the core that increases radically surface life of forgings. The second
method includes high-temperature and low temperature intensive thermo - mechanical treatment (LTTMT) of
high carbon alloy steels with delaying martensitic transformation to make low-temperature thermo - mechanical
treatment (LTTMT) possible. Then, after high temperature and low-temperature thermomechanical treatment,
the steel goes to immediate tempering to create highly strengthened fine bainitic microstructure throughout the
section of the steel part. A modified method of cooling time calculation, suitable for any size and form of steel
part, is widely discussed in this paper.
Key-Words: - Thermo- mechanical treatment, Forging, New intense technology, Surface compression stresses,
Fine bainitic microstructure, Service life, Environment improvement.
Received: May 13, 2023. Revised: February 11, 2024. Accepted: May 6, 2024. Published: June 4, 2024.
1 Introduction
High and low temperature thermomechanical
treatment is known from literature and its practical
use in forging shops [1], [2] and [3]. As a rule,
thermomechanical treatment was performed in
slowly cooling oils to prevent crack formation.
Authors [4], used intensive cooling for direct
quenching of forging designated by them as DFIQ
process. As reported, [4], the intensive quenching of
forging immediately after hot forging operations
(DFIQ) improves the mechanical properties of parts,
allowing in many cases, a substitution of lower
alloy and less expensive steel for higher alloy steel.
Also, the use of the DFIQ process allows the
manufacturer to eliminate post-forging heat
treatment resulting in a significant reduction in the
heat treatment costs. In addition, the DFIQ forgings
have very little surface scale, since the parts are not
reheated two times. It was noticed by the author, [2],
that the mechanical properties of AISI 1040 steel
after high-temperature accelerated
thermomechanical treatment are significantly
improved as compared with the conventional
hardening process (Table 1). The quenching after
forging was performed in cold water. One can
expect that forging combined with intensive
quenching to obtain fine bainite at the core of forged
steel parts will provide more benefits. After
intensive high-temperature thermomechanical
treatment at the surface of forgings the compression
stresses are formed while at the core intermediate
phases are present. In contrast to existing
technology, this paper considers situations when at
the surface of forgings high compression stresses
are formed simultaneously with forming fine or
nano-bainitic microstructure at the core of forgings.
It can be achieved by interrupting the quenching
process at the proper time and delivering forging to
tempering at the temperature that provides fine or
nano–bainitic microstructures. The second possible
approach consists of delaying martensite
transformation during intensive quenching that
allows performing effective high and low thermo-
mechanical treatment while obtaining fine bainitic
microstructure throughout the forged articles. The
fine bainitic microstructure possesses high
mechanical properties of steel, [5], [6]. As known,
alloy and high alloy steels were quenched in slowly
cooled liquid media (oils, water solutions of
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polymers of high concentration) to prevent crack
formation during forging and quenching.
Table 1. Mechanical properties of AISI 1040 steel for heavy rolling with 19 mm diameter in the case of high–
temperature thermo-mechanical treatment and conventional heat treatment, [2]
Tempering
R MPa
m
( )
R MPa
p0 2.
( )
A(%)
Z(%)
R
m
(J/cm2)
200oC
1972
1422
,
,
1570
1240
,
,
7 0
2 0
.
.
40 0
16 0
.
.
35
30
300oC
1766
1628
,
,
1472
1511
,
,
7 5
7 0
.
.
39
35
30
40
400oC
1373
1177
,
,
1226
1099
,
,
8 5
8 5
.
,
53
50
80
85
Low-temperature thermomechanical treatment is
performed in hot oils to delay the transformation of
austenite into martensite to to perform forging at
400oC 500oC. Since oil cools slowly, the low-
temperature thermomechanical treatment is possible
when alloy or high alloy steels are used. The current
paper discusses high and low temperature
thermomechanical treatment in conditions when
cooling is intensive and is always suitable for plain
carbon steels and alloy steels of any chemical
composition. The technology is based on new
physical principles published in [7], [8] which sound
as:
During quenching from high temperature in cold
fluid any film boiling can be absent completely if
initial heat flux density
q q
in cr
1
.
If any film boiling during quenching is
completely absent, the cooling process is
intensive and uniform.
The time of full transient nucleate boiling
establishment is the same for different sizes and
forms of steel parts due to the very fast cooling
process.
Duration of transient nucleate boiling is directly
proportional to the squared size of the steel part
and inversely proportional thermal diffusivity of
the material and is evaluated by a fundamental
generalized equation, [6].
Transition from nucleate boiling to
convection is evaluated by equalizing heat
fluxes at the end of nucleate boiling and the
beginning of convection.
Based on these formulated principles, [6], the
new intensive thermomechanical technologies were
developed and used for direct quenching. From the
point of view of thermal science these processes are
discussed below. Such technology was not tested yet
because it was a big problem to delay the
transformation austenite to martensite to perform
successfully low-temperature thermomechanical
treatment.
2 Absence of Film Boiling during
Quenching Steel in Cold Fluids
The most significant achievement in developing
intensive quenching technologies is the theoretical
explanation why during quenching in cold fluids the
film boiling can be completely absent and cooling in
this case is intensive. Since the fluid is cold during
steel part immersion. first starts incredibly short
convection (Figure 1). After overheating of a
boundary layer shock boiling begins which continues
in two possible ways, [7].
Fig. 1: Two possible ways of the quenching process
taking place when steel part heated to high-
temperature immersions into the cold fluid
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If the initial heat flux density
q
in
is below the
first critical heat flux density
q
cr1
(
q
in
<
q
cr1
). no film
boiling will occur.
Due to the huge overheat of the boundary layer,
small bubbles appear known as the shock boiling
process (Figure 2a).
Fig. 2: Shock (a) and nucleate boiling (b) processes
during quenching in liquid media
These small bubbles became larger passing to the
developed nucleate boiling process if
q
in
<
q
cr1
(Table 2, film boiling is absent). The process of
cooling in cold fluid is uniform since any film
boiling is completely absent which decreases
distortion of hardened steel parts, [7], [8]. Note,
shock boiling is present also at the beginning and at
the end of film boiling oscillating with high
frequency 13.6 kHz (Figure 3).
Fig. 3: Temperature–time, broadband, and
narrowband quenching data [7]: a) is cooling rate vs
time; b) are frequencies of film and nucleate boiling
modes; c) is the frequency of shock boiling.
Table 2. Time required for the surface of steel spheres of different sizes to cool to different temperatures when
quenched from 875 oC in 5 % water solution of NaOH at 20 oC agitated with 0.9 m/s, [9]
Size in
Mm and
Time,
sec
Temperature
700oC
600oC
500oC
400oC
300oC
250oC
200oC
150oC
6.35
0.027
0.037
0.043
0.051
0.09
0.15
0.29
0.69
12.7
0.028
0.042
0.058
0.071
0.11
0.15
0.26
0.60
120.6
0.043
0.066
0.09
0.12
0.17
0.21
0.29
0.95
180
0.043
0.070
0.10
0.14
0.24
0.31
0.42
1.15
286
0.043
0.12
0.19
0.33
0.57
0.96
1.28
2.18
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If
q
in
>
q
cr1
film boiling starts which decreases
the cooling process during quenching of steel parts
[6].
3 Fundamentals of the Transient
Nucleate Boiling Process
To be sure that the absence of film boiling process is
intensive and can compete with powerful propellers
and pumps, let’s see a decrease of Kondra’ev
numbers Kn versus time. Such data can be received
by solving inverse problems, [10], [11] using
accurate experimental data of author, [9], presented
in Table 2. The initial temperature of the transient
nucleate boiling process and the initial temperature
of convection are evaluated using equations (1) and
(2).
Io I
R
12
0 3.
(1)
II conv II uh
1
0 3.
(2)
75
0 5 0 5
0 5 0 7 0 2
' ' "
" " Pr
..
...
g
r W
;
10293
.
;
a
v
Pr
.
Duration of transient nucleate boiling process is
evaluated as:
nb F
kD
a
2
(3)
where
Pr is Prandtl number;
cr
P
P
W
Wlg5.03.2
1.0
"
1.0
;
"
1.0
W
is bubble growth rate at normal pressure P;
P
cr
is critical pressure in Pa;
is heat transfer
coefficient at nucleate boiling (
Km
W2
);
is
thermal conductivity of fluid (
mK
W
);
is surface
tension (
m
N
);
g
is gravity acceleration factor
(
2
s
m
);
'
is liquid density (
3
m
kg
);
is vapor
density (
3
m
kg
);
q
is heat flux density (W/m2);
*
r
is heat of vapor formation (J/kg);
W
is steam
bubble growth rate (m/s);
T
o
is initial temperature;
v
is kinematic viscosity (m2/s);
a
is thermal
diffusivity of liquid (m2/s).
Tabe 3 presents values of
when initial
temperature of heated steel part is fixed at 850oC
and the temperature of quenchant is fixed at 20oC.
Table 3. Parameter
as a function of convective
Biot number when initial temperatures Tm and To
are fixed at 200C and 850oC
Bi
Bi
0.1
5.40
2
2.41
0.2
4.72
3
1.98
0.3
4.32
4
1.69
0.4
4.02
5
1.46
0.5
3.79
6
1.27
0.6
3.63
7
1.12
0.7
3.47
8
0.98
0.8
3.33
9
0.86
0.9
3.21
10
0.75
1.0
3.11
12
0.56
Table 4 provides coefficients
k
F
depending
on the forms of different steel parts.
Table 4. Coefficients
k
F
depemnding on forms of
steel parts.
Shape of a body
k
F
Plate
0.1013
Cylinder
0.0432
Sphere
0.0253
Round plate D = nZ:
n = 1
0.0303
n = 2
0.0639
n = 5
0.0926
Using experimental data of author, [9] (see
Table 1) and equations (1), (2), and (3), it was
possible to restore surface temperature for different
sizes of probes during the transient nucleate boiling
process to solve the inverse problem discussed in [7],
[10]. Simultaneously. a system with hyperbolic heat
conductivity equations (4) and (5) (8) was solved
by authors [12], [13] to investigate properly
quenching processes when during cooling any film
boiling is completely absent.


a
T T div gradT q
r
2
2
(4)
T
rT T
m
s
m
r R
0
(5)
T r T,0
0
(6)
q q
cn nb
(7)
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T
rT T
conv r R
0
(8)
m
10 3/
The problem is rather complicated and requires
additional investigations to simplify methods of
calculations.
4 Self-regulated Thermal Process to
be used for HTTMT and LTTMT
Its essence is as follows. The surface temperature of
the steel part during immersion into liquid
quenchant drops immediately almost to the
saturation temperature of a liquid and maintains at
this level relatively a long time until transient
nucleate boiling is finished. The real heat transfer
coefficient (HTC) at the beginning of boiling is very
large and can reach 200,000 W/m2K. Convective
HTC is rather small and for still water and water salt
solutions reaches 400 - 1200 W/m2K. Convective
HTC on average is 200 times smaller as compared
with the nucleate boiling process. It means that
nbconv

or
nb
V
conv
VBiBi 
(9)
Here
conv
V
Bi
is the generalized Biot number
during convection;
nb
V
Bi
is the generalized Biot
number during the transient nucleate boiling process.
To prove the theoretical existence of SRTP let’s
consider a well-known universal correlation (10),
[14], [15], [16]:
1437.1
1
2
VV
mV
msf
BiBi
TT
TT
(10)
Here
sf
T
is average surface temperature;
V
T
is
average volume temperature,
m
T
is bath temperature,
V
Bi
is generalized Biot number.
Note that during transient nucleate boiling
process Tm = Ts.
Assume that the surface temperature of steel
part at the beginning of cooling is below the
saturation temperature TS and is in the convection
area. Taking into account Eq. (10), one can assume
that
0
V
Bi
. In this case, according to Eq. (10),
Vsf TT
. It means that surface temperature must
increase immediately if it drops below Ts and occurs
in the convection area. Assume now that the
overheat of the boundary layer is rather large. In this
case generalized Biot number
V
Bi
is very large
also which tends to infinity, i.e.
V
Bi
.
According to Eq. (10),
ssf TT
and it means that
overheating is zero and transient nucleate boiling
process must stop. Only one way is left. The surface
temperature must be very close to the boiling point
of a liquid from the very beginning of cooling. The
cooling system controls overheating
by itself
which depends on the size and form of a steel part.
The overheating
is small as compared with the
initial temperature T0. For practical use, one can
consider this behavior of the surface temperature as:
constTT Ssf
(11)
4.1 Main Characteristics of SRTP
Below (Figure 4 and Figure 5) are surface and core
cooling curves for cylindrical probes quenched from
850oC in water salt solution and water under
pressure 0.7 MPa.
Fig. 4: Cooling curves vs time during quenching of
cylindrical sample 25 mm dia 120 mm height in
cold water salt solution of optimal concentration
Fig. 5: Surface and core cooling curves vs time
during quenching of cylindrical sample 50 mm dia
75 mm height in cold water under pressure 0.7 MPa
As seen from Figure 4 and Figure 5 the surface
temperature of cylindrical probes is maintained at
the level of boiling point of a liquid. The surface
temperature during nucleate boiling can be replaced
by average temperature when calculating the
temperature field in the probe (Figure 6).
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Fig. 6: Cooling curves vs time during quenching
cylindrical sample 50 mm dia 200 mm long in cold
water solution (14%) of NaCl at room temperature.
Lines are numerical calculations; dots are
experiments
To see how intense is cooling process is during
quenching in water and water solution of low
agitation, the real and effective Kondrat’ev numbers
were evaluated using the IQLab program, [8]
(Figure 7). Real Knnb and effective Knconv
Kondrat’ev numbers versus time. when cooling the
cylindrical sample 25 mm dia 120 mm height in
cold water salt solution of optimal concentration.
are within 0.2 1 for effective data and 0.8 - 1 for
real Kondrat’ev numbers, [8]. Their average values
are:
Kn
eff
0 6.
and
Kn
real
0 9.
.
Quenching in water under pressure 0.7 MPa
increases dimensionless numbers Kn and they are:
Kn
eff
065.
and
Kn
real
095.
. All calculated data
show that the transient nucleate boiling process
provides intensive quenching because Knreal >
0.8.
Fig. 7: Real Knnb and effective Knconv Kondrat’ev
numbers versus time when cooling cylindrical
sample 50 mm dia 75 mm height in cold water
under pressure 0.7 MPa
Based on the above investigations, it is possible
to propose different types of thermomechanical
treatment:
HTTMT with the delay of martensite
transformation to achieve bainitic fine or
nano microstructures.
LTTMT with the delay of martensite
transformation to perform plastic
deformation mediate temperatures.
To combine HTTMT and LTTMT to
improve significantly mechanical properties
of materials.
To combine HTTMT and LTTMT to delay
martensite transformation and achieve fine
bainitic microstructure.
The listed above technologies are possible if
film boiling is completely absent and SRTP lasts
relatively a long time. The film boiling is absent if
the initial heat flux density qin is below the first
critical heat flux density qcr1, i.e., qin < qcr1. Initial
heat flux densities are evaluated by solving inverse
problems, [10], 12]. The critical heat flux densities
were considered by authors, [17], [18], [19]. It was
possible to evaluate initial heat flux densities for ,
different sizes of cylindrical probes (Figure 9a,b).
For both sizes, 25 mm and 50 mm initial heat flux
densities were almost the same and were equal
approximately to 20 MW/m2. Such behavior is due
to very fast cooling where heat transfer can be
considered in the semi - infinity domain. For this
situation both initial heat flux densities are below
the first critical heat flux generated by the shock
boiling process (Figure 8) which is why the film
boiling was completely absent (Figure 4 and Figure
5).
a)
b)
Fig. 8: Heat flux density versus time taking place
during quenching cylindrical probes in water salt
solutions of optimal concentration: a) 25 mm
diameter; b) 50 mm diameter
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To explore the transient nucleate boiling process
for new technologies development, convective HTC
should be reduced as much as possible, it increases
the duration of transient nucleate boiling.
Cooling time
and cooling rate
at the core
of steel parts during quenching are approximately
evaluated using equations (12) and (13), [7], [8]:
kBi
Bi
T T
T T
K
aKn
V
V
o m
m
2095 3867. . ln
(12)
vaKn
KT T
m
(13)
Equations (12) and (13) are widely used for
recipes development when hardening steel parts of
different configurations.
5 Chemical Composition of Steel
Optimization
The chemical composition of steel optimization was
developed to provide optimal hardened layer (see
Figure 9) that results in high surface compression
residual stresses and a fine bainitic microstructure at
the core of steel parts. Both of these factors increase
the service life of quenched steel parts, [16].
Fig. 9: Optimal depth of hardened layer
corresponding to the maximum surface compressive
residual stresses, [20], [21]: LH, low hardenability
steel; OH, optimal hardenability; ThH, through
hardening
The heat-treating industry can generate great
benefits performing HTTMT and LTTMT using low
hardenability steels (Figure 9). In this case, along
with the increased mechanical properties of the
material, hardened components will attain high
compressive residual stresses and viscose core
resulting in a higher degree of super- strengthening
effect.
The generalized correlation for optimizing the
chemical composition of steel, depending on the
size and form of the steel part, is evaluated by
equation (14), [20], [21]:
DI
DKn
a
opt
0 5
035 0095
.
. .
(14)
The critical thickness of a small model DIa ,
which is equal to the form of a real steel part,
D
opt
is
the thickness of steel part to be quenched. Here Kn
is Kondrat’ev number. For cylindrical forms like
semi-axle, that is quenched in condition
Bi
,
the correlation (14) became more simple and is
written as, [20]:
DI
D
opt
035 0095. .
(15)
According to author, [22], critical diameter DI for a
cylinder depends on the chemical composition of
steel and is evaluated as:
.....4.25 NiCrSiMnFe fffffDI
(16)
where
f
x
is the multiplicative factor for the
particular alloying element. The available set of
alloy factors is presented in the book by author,
[23]. These multiplicative factors are used for
optimizing the chemical composition of steel
depending on the size and form of the steel part.
More information on an optimal hardenability steels
and chemical composition optimization can be
found in the book, [21].
It was shown by authors that intensive
quenching (IQ) provides compressive residual
stresses, [23], [24], [25]. The optimal hardenability
steel provides optimal stress distribution through the
section of hardened steel parts creating very high
compression residual stresses and hardness at the
surface. Core hardness is reduced with the high
viscosity of material that increases the service life of
hardened components.
6 Technique of Film Boiling
Elimination
6.1 Optimal Concentration of Water Salt
Solutions
The HTTMT and LTTMT, as a rule, in many cases
are performed in water solutions under pressure to
eliminate the developed film boiling process.
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Quenching is performed in water solutions of neutral
salts. The optimization of aqueous salt solutions is
achieved by controlling the ionic charge that is
present at the interface of the quenchant and the
metal surface. A phenomenon was described by
author, [26], [27] and further developed by authors,
[28]. It should be noted here that quenching
processes, [29], [30], are investigated by scientists
thoroughly while intensive HTTMT and LTTMT
are not investigated enough. The current paper asks
scientists put together their efforts to investigate
properly the intensive HTTMT and LTTMT
technologies.
As known, for all electrolytes there are optimal
concentrations where the first critical heatflux
densities are maximum (Figure 10).
Fig. 10: Maximal critical heat flux densities qcr1
versus concentration for NaCl and LiCl [7]: 1 is
NaCl; 2 is LiCl
Some water salt solutions are used in the heat
treating industry as quenchants to eliminate film
boiling processes that provide uniform cooling and
decrease distortion of steel parts after quenching.
Any water salt solution provides the maximum
value of the first critical heat flux density if the
concentration is optimal (Figure 10).
6.2 Intensive Quenching in Pressurized Fluid
Flow
Figure 11 shows the schematic installation to
provide intensive and uniform cooling by exploring
pressurized fluid flow. Critical heat flux density in
this case can be increased by short-lasting external
negative electrical force directed to semi – the axle.
Fig. 11: Detailed scheme of quench chamber with
automatic control, [7], [31], [32]: 1 semi-axle; 2
quench chamber; 3 pressurized water flow; 4
mechanical drive for semi-axles; 5 sensor for
analyzing the process. of nucleate and film boiling;
6 sensor for analyzing the portion of transformed
structures by the changing ferromagnetic state; 7
electronic device (amplifier and microprocessor); 8
– amplifier
Currently, the technology is used for intensive
quenching of trucks [7], [30], [31]. The technology
provides high surface compression residual stresses
and viscose core of semi-axles if low hardenability
steel is used for their manufacturing. It can be
incorporated easily in line with HTTMT and
LTTMT technologies.
6.3 Surface Insulating Polymeric Layer that
Reduces Initial Heat Flux Density
Low concentration (1%) of inverse solubility
polymers is used as a quenchant for intensive
quenching of steel parts. The technology explores
thin surface polymeric insulating layer to reduce
initial heat flux density according to equation (17):
qq
R
in o
coat
1 2
(17)
It can be used also for performing HTTMT and
LTTMT processes. Figure 12 shows a thin surface
polymeric layer that covers metal to reduce initial
heat flux density during quenching, [8]. The
proposed technology saves polymers and increases
the mechanical properties of steel due to the reduced
concentration of polymers and intensive quenching
(IQ) process. It decreases also distortion due to
uniform and intensive cooling.
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Fig. 12: Section of a coated cylindrical probe and
typical temperature distribution during quenching in
polymer water solution of inverse solubility
6.4 Resonance Effect to Eliminate Local and
Developed Film Boiling Processes
To eliminate film boiling processes one can use
special emitters that produce waves with frequencies
equal to the frequencies of film boiling processes.
The arrangement of emitters in the quench tank are
shown in Figure 13, [8].
Fig. 13: Emitters arrangement in quench tank: a is
emitter, where 1 is liquid flow, 2 is tube, 3 is
circulated liquid stream, 4 is generator waves in
liquid, 5 is regulator of wave frequency, 6 is liquid
flow combined with generated waves; b is quench
tank with located in it emitters, where 1 is quench
tank; 2 is water salt solution of optimal
concentration; 3 is fixture; 4 is steel part; 5 is local
film boiling; 6 is emitter
6.5 Effect of Intensive Quenching for
Providing High Surface Compression
Stresses
The effect of intensive quenching on surface
compression residual stress formation was for the
first time discussed by authors, [7]. Further accurate
numerical investigations in this field were fulfilled
in the USA, Germany, and Japan [33], [34] and [35].
An overview, of concerning results of experiments
and calculations, is provided in the handbook [30].
Now is clear that compression residual stresses can
be formed by interrupting intense cooling at the
proper time, [8], or reducing alloying of steel to
provide an optimal hardened layer in quenched
component, [21]. Cooling time interruption is
discussed below.
7 Universal Correlation for Cooling
Time Calculation
The universal correlation was proposed for
calculating the heating and cooling times of any
steel part during its hardening, [7], [8]. The same
technique can be used when performing HTTMT
and LTTMT processes. The equation contains
Kondratjev form factor K, Kondratjev number Kn,
the average thermal diffusivity of a material, and a
function depending on how N times the core
temperature of a steel part differs from its initial
temperature. It is shown that these parameters are
enough to calculate recipes when heating and
cooling the steel parts of any configuration. A
tendency of thermal equilibrium establishment is
considered, which depends on the size and
configuration of objects, thermal diffusivity of
material, and the condition of cooling (heating)
characterized by Kondratjev number Kn. The
proposed generalized equation provides engineers
with extremely simple and understandable
parameters for calculating the heating (cooling) soak
time of any object. According to the proposed
equation, the time of thermal equilibrium
establishment is directly proportional to Kondrat’ev
form factor K, inversely proportional to the thermal
diffusivity of material and Kondratjev number Kn,
and depends on the accuracy of the thermal
equilibrium measurement, see Eq. (17) and Table 5:
eq eq
EK
aKn
(17)
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Table 5. Coefficients
E
eq
, depending on dimensionless value
N T T T T
S S
( ) / ( )
0
which was
decreased from 1.5 to 1,000 times
Bi
V
2
E
eq
N
1.5
2
2.5
3
3.5
4
4.5
5
10
100
1000
Plate
0.61
0.90
1.12
1.30
1.46
1.59
1.71
1.81
2.51
4.81
7.11
Cylinder
0.81
1.10
1.32
1.50
1.66
1.79
1.91
2.02
2.71
5.01
7.33
Sphere
1.01
1.30
1.52
1.71
1.86
1.99
2.11
2.22
2.91
5.21
7.51
Bi
V
3
E
eq
N
1.5
2
2.5
3
3.5
4
4.5
5
10
100
1000
Plate
0.625
0.912
1.135
1.318
1.472
1.605
1.723
1.828
2.522
4.824
7.127
Cylinder
0.843
1.131
1.354
1.537
1.691
1.824
1.942
2.047
2.741
5.043
7.346
Sphere
1.062
1.350
1.573
1.757
1.910
2.043
2.161
2.266
2.960
5.262
7.565
Bi
V
5
E
eq
N
1.5
2
2.5
3
3.5
4
4.5
5
10
100
1000
Plate
0.63
0.92
1.14
1.32
1.48
1.61
1.74
1.83
2.54
4.83
7.13
Cylinder
0.86
1.15
1.37
1.50
1.71
1.84
1.97
2.07
2.77
5.06
7.36
Sphere
1.10
1.38
1.61
1.80
1.94
2.08
2.20
2.30
3.00
5.29
7.58
Bi
V
E
eq
N
1.5
2
2.5
3
3.5
4
4.5
5
10
100
1000
Plate
0.64
0.93
1.15
1.33
1.49
1.62
1.73
1.84
2.53
4.84
7.15
Cylinder
0.87
1.16
1.38
1.51
1.72
1.85
1.96
2.08
2.76
5.07
7.38
Sphere
1.11
1.39
1.62
1.80
1.95
2.09
2.20
2.31
3.00
5.30
7.60
Approximately thermal equilibrium is established
when
E
eq
7136.
for plate;
E
eq
7362.
for cylinder
and
E
eq
7582.
for sphere.
8 High and Low-Temperature Thermo-
Mechanical Treatment
The HTTMT of forgings, made of optimal
hardenability steels, requires complete intensive
cooling to room temperature. Figure 14 shows
combined high and low thermomechanical treatment
with the possibility of obtaining the fine or nano-
bainitic microstructure at the core of forgings
.
Fig. 14: HTTMT and LTTMT to obtain fine bainitic
microstructure
In this case, after forging, the component is
intensively cooled to low thermomechanical
treatment temperature, forged again, and cooled
a second time and tempers at the specific
temperature that provides nano bainitic
microstructure. Such technology can provide
super-strengthened material and increase
significantly the service life of forged machine
components, [6], [7], [8]
9 Discussion
It has been shown by the author of well-known
investigations, [5], [6] that fine bainitic
microstructure has better mechanical properties
(strength and viscosity) as compared with the
martensitic microstructure. After a short
discussion of some problems with the author,
[5], it was clear that there is a big problem in
delaying martensite transformation when steels
are quenched intensively. As a rule, for
obtaining bainitic microstructure steel
components are quenched slowly in hot oils or
melted salts to delay the start of martensitic
transformation. After reducing of steel core
temperature in melted salts, steel components go
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to tempering to obtain fine bainitic microstructure.
Since the cooling rate in melted salts is rather low,
engineers use high alloy steels to delay any
transformation during slow cooling, and then
undercooled steel goes for long tempering to obtain
bainitic microstructure. It is impossible to obtain fine
bainitic microstructure for low alloy steels using slow
cooling. Our investigations allow delaying martensite
transformation during the IQ process quenching steel
in fluid under pressure (Figure 5 and Figure 10). It
means that fine bainitic transformation can easily be
obtained using plain carbon steels and any alloy steels.
The problem is very important for the practice which
is why it makes sense to further discuss the problem at
the conferences. There are highly developed tools and
devices for infestation cooling processes in fluids to
predict hardness distribution during the hardening of
materials, [35], [36]. There are computer codes for the
fluid dynamics investigations, [37] and highly
developed codes for temperature fields and stress
distribution investigations, [38] and fracture
phenomena when the material is brittle [39]. If these
opportunities together, it will be possible to properly
investigate HTTMT and LTTMT processes.
10 Conclusions
1. A new high-temperature thermo - mechanical
strengthening of low-carbon or middle carbon
alloy steel is proposed. After forging steel part is
intensively quenched with an interruption cooling
process at a moment when the optimal surface
hardened layer is formed to create surface
compression residual stresses. After the
interruption of the cooling process, steel goes to
immediate tempering to create fine bainitic
microstructure at the core and a martensite surface
strengthened layer at its surface.
2. A new high-temperature and low temperature
thermo-mechanical strengthening of high-carbon
alloy steel is proposed. After forging the steel part
is intensively quenched delaying martensitic
transformation and interrupting the cooling
process at the moment when low-temperature
thermo-mechanical treatment is possible. Then
high temperature and low temperature thermo-
mechanical treatment is performed followed by
immediate tempering to create highly strengthened
material (fine bainitic microstructure throughout
all sections of forged steel part).
3. A modified method of cooling time calculation
suitable for any size and form of steel part
quenched intensively in cold water or special
water solution is proposed to perform correctly
high temperature and low-temperature
thermo-mechanical treatment.
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Contribution of Individual Authors to the Creation
of a Scientific Article (Ghostwriting Policy)
N.I. Kobasko developed intensive quenching of
alloy steels and simplified methods for their
recipes design, which currently are used for
strengthening of forgings.
Sources of Funding for Research Presented
in a Scientific Article or Scientific Article
Itself
No funding was received for conducting this
study.
Conflict of Interest
The author has no conflicts of interest to
declare.
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(Attribution 4.0 International, CC BY 4.0)
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Creative Commons Attribution License 4.0
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