1 Introduction

Steel is the fundamental material of a country’s industrialization. Strength is one of the important performances of steel structures. For over half a century, ferrous-metallurgy and materials scientists from different countries have performed much in-depth research into steel’s strengthening mechanisms. For single-phase alloy, Hall–Petch proposed the grain refinement strengthening theory[1,2] based on the dislocation pileup model. For steel in which second-phase precipitation exists, many authors proposed various kinds of precipitation strengthening mechanisms, based on the interaction between second-phase particles and dislocation motion, the most important of which are the shearing mechanism and bypass (looping) mechanism.[36]

High-strength low-alloy (HSLA) steel containing microalloying elements such as V, Nb, and Ti is a typical steel with a precipitation strengthening mechanism, in which nanoscale V, Nb, and Ti carbides have a significant precipitation strengthening effect. However, because it is hard to determine the volume fractions of different types and sizes of nanoscale particles, by existing theoretical formulas, the contribution of precipitation strengthening to steel strength can only be analyzed in a qualitative way rather than by quantitative calculation, which prevents further research into steel’s precipitation strengthening mechanisms.

Based on chemical phase analysis, X-ray small-angle scattering (XSAS), room temperature organic (RTO) analysis, high-resolution transmission electron microscopy (TEM), and steel tempering rapid-cooling technology, the precipitated nanoscale particles were quantitatively analyzed. The contribution of precipitation strengthening to the yield strength was calculated. Subsequently, the steel’s strengthening mechanisms are discussed based on this calculation, and a comprehensive strengthening mechanism of steel is proposed.

2 Nanoscale iron-carbon precipitates in hslc steel

Thin slab continuous casting and rolling process (referred to hereinafter as TSCR), one of the contemporary steel production processes, has been growing rapidly in the world in recent years. Over 95 pct of TSCR products are low-carbon steels with 0.06 to 0.25 pct carbon content or low-carbon high-strength alloyed steels. Higher strength is one of the significant mechanical properties of TSCR products. In studying the reasons for the high strength of TSCR’s high-strength low-carbon (HSLC) steels, the authors of References 7 and 8 first found that there were a great number of nanoscale oxides and sulfides, whose sizes range from tens to hundreds of nanometers. They also found plenty of precipitation particles sized less than 20 nm, which have spinel-shape structure. The authors of References 9 and 10 found in their experiments that there existed nanoscale AlN particles in steel, whose size ranges from several to tens of nanometers, and they also did kinetic studies on these particles. The authors of References 11 and 12 studied the nanoscale carbides in TSCR’s low-carbon steels and their influence on steel’s mechanical properties and pointed out that there existed a great number of precipitates (Figure 1) sized less than 20 nm in TSCR’s low-carbon slabs, rolled pieces, and final products. They are mainly iron-carbon precipitates and have a significant precipitation strengthening effect in steels.

Fig. 1
figure 1

TEM micrograph of nanoscale precipitates in HSLC: (a) slab, (b) rolled piece, and (c) product[13]

The types, size distribution, and volume fractions of precipitates with size less than 20 nm in TSCR’s low-carbon steels were systematically studied by the authors of Reference 13. The contribution of iron-carbon precipitates to steel’s strength was discussed. They pointed out that the precipitates’ strengthening contribution to the yield strength of HSLC equals that of grain refinement strengthening.

2.1 Tempering Rapid-Cooling Experiment[13]

According to the Fe-C binary phase diagram, at temperature A1, the equilibrium carbon content in ferrite is 0.022 pct; at room temperature, it is less than 0.008 pct. Below temperature A1, with the drop of temperature, part of the supersaturated carbon will precipitate from ferrite. In the course of thin slab continuous casting and rolling, the great intensity of laminar cooling results in rapid cooling of the strips, the precipitates’ size is small, their strengthening effects are great, and therefore, the TSCR steels have higher strengths. In coiling, on the other hand, the cooling rate of coils is slow, the precipitates are coarsened, and therefore, the steel’s strength will be expected to be a bit lower than before the coiling.

Three special experiments were designed to study the precipitating temperature, precipitation, growth, coarsening, and strengthening effects of iron-carbon precipitates with size less than 20 nm. The first set of experiments studied the influence of treating temperature below A1 on the mechanical properties of steels (one more experiment was done to test the reproducibility of the results). The second studied the influence of treating time on steel’s strength, and the experimented material was HSLC steel ZJ330 (coil no. 53921); the results are shown in Table I (the mechanical property of repeated experiments is represented by Tests 1 and 2) and Figure 2. The third is the repeated experiment of the second, in which the experimented material is another coil of ZJ330 (coil no. 53931), and the σ s , σ b , and δ were 351 MPa, 425 MPa, and 42 pct, respectively; the results are shown in Figure 3.

Table I Effect of Tempering Temperature (Holding 20 Minutes) and Cooling Method on the Mechanical Properties of ZJ330 Steel
Fig. 2
figure 2

Influence of tempering time on the mechanical properties of HSLC steel at the same temperature below A1

Fig. 3
figure 3

Relation between tempering time of ZJ330 (coil no. 53931) steel and its performance

From Table I and Figures 2 and 3, we can see that the cooling speed has a great influence on steel strength. When the temperature is above 873 K (600 °C) but lower than A1, tempering and fast cooling could increase steel strength significantly. As cooling speeds of steel during casting, rolling, and after coiling are all relatively fast in the TSCR process, a large amount of nanoscale participants include the size less than 20 nm participants that exist in slab, rolling pieces (steel sheets stuck in rolling processes), and products (finished plates); the experimental results match the expected results mentioned previously, indirectly proving the existence of nanoscale iron carbide precipitates, as shown in Figure 1.

2.2 Analysis Using High-Resolution TEM

Liu et al.[8] found a large number of 50- to 60-nm Fe-O-C participants near ferrite grain boundaries in HSLC steel. It is a bit difficult to observe particles with size less than 20 nm using an analytical electron microscope, particularly those with size only several nanometers, as it is quite hard to determine whether these particles are iron-carbon precipitates because of the matrix effect disturbances. To determine the characters and precipitation mechanism of these particles, further observation of the precipitate particles extracted by the electrolysis method was done with high-resolution TEM.

During the experiments, the hot-rolled strip piece (3-mm thickness) was electrolyzed with organic solution for 24 hours, and then the particles obtained from electrolysis were put into dehydrated alcohol solution. After ultrasonic vibrating, the fine particles floating on the upper layer were sucked with a chemical dropper and dipped onto a copper microgrid; finally, the sample for TEM was obtained when all the dehydrated alcohol was evaporated. The sample was observed with a high-resolution transmission electron microscope JEM2010 (JEOL Limited, Tokyo, Japan), with 500,000 times magnification and 200 kV voltage. The chemical composition of the powder was also analyzed with an X-ray energy spectrum. The results are shown in Figure 4.

Fig. 4
figure 4

(a) High-resolution TEM image of electrolytic nano Fe-O-C precipitate and (b) EDS from ZJ330 steel

From Figure 4, it can be seen that there are a large number of Fe-O-C precipitates with sizes less than 10 nm. Figure 4(b) is the energy spectrum of the center particle (about 10 nm) of Figure 4(a).

2.3 Chemical Phase Analysis and XSAS

It is quite difficult to determine the mass fraction or volume fraction of nanoscale particles in steel with an electron microscope, yet the volume fractions of precipitates with different sizes are indispensable for calculating the strength of steel. Chemical phase analysis and XSAS are effective methods to determine the chemical composition, mass fraction, or volume fraction of nanoscale particles with different sizes.

Chemical phase analysis can be described as the following processes:

  1. (1)

    electrolyzing the steel sample to obtain electrolyzed powders containing iron carbonitride Fe3(C x N y ), alloy carbonitride M (C x N y ), sulfides, and nitrides;

  2. (2)

    getting rid of iron carbide, sulfides, and AlN to obtain M (C x N y ) and oxides; and

  3. (3)

    removing M (C x N y ) phase to get stable oxides.

After the preceding separation procedures, the electrolyzed powders were dissolved, respectively; the contents of Fe, Mn, Ni, N, and carbon were analyzed; and then the mass fraction of cementite based on the molecular formula (Fe a Mn b Ni c )3(C x N y ) was calculated.

According to GB/T 1322191 (ISO/TS 13762 2001), the particle size distribution of precipitate powders was analyzed by SAXS with a Kratky small-angle scattering instrument (Rigaku Corporation, Tokyo, Japan) of X-ray diffraction spectroscopy; the analyzed error is less than 10 pct. The chemical compositions of experimental steel and results are shown in Tables II and III, respectively.

Table II Chemical Composition (Mass Percent) of Testing Steels*
Table III Size Distribution of Cementite Particles with Size Less than 18 nm Precipitated in ZJ330 and ZJ 510 Steels

The thickness of the EAF-CSP ZJ330 slab is 50 mm, and it reduced to 25 mm after the first rolling pass. The start rolling temperature is 1363 K (1090 °C), the exit temperature is 1325 K (1052 °C) for the first pass rolling, the finishing rolling temperature is 1163 K (890 °C), and the coiling temperature is 913 K (640 °C).

3 Nanoscale ironcarbon precipitates in hsla steel

HSLA steel refers to the steel containing microalloying elements such as V, Nb, and Ti. The Ti microalloyed high-strength weathering steel is an HSLA steel.

Chemical phase analysis and XSAS analysis were carried out on the samples of HSLA steels and Ti microalloyed high-strength weathering steel. The mass fractions of M3C and MC particles less than 36 nm in the electrolytic powders were measured. The chemical compositions of experimental steel and results of HSLA steel are shown in Tables IV and V, respectively.

Table IV Chemical Compositions of Experimental Steel* (Mass Percent)
Table V Size Distribution of Carbide Particles with Size Less than 36 nm Precipitated in 70A and B2C Steel (Mass Percent)

From Tables IV and V, it can be seen that the mass fraction of M(C x N y ) in the particles with size less than 36 nm is much less than that of M3(C x N y ) with the same size in steel.

The Ti microalloyed high-strength weathering steel under lab[14] and production conditions[15] was studied, and it was found that Ti microalloying has an obvious influence on the strength of hot-rolled strips. The authors of Reference 15 studied the strengthening mechanism of Ti using chemical phase analysis, XSAS, and electron microscope analysis, and they found that the percentage content of nanoscale TiC increases with the increase of Ti content in steel; as a result, the steel’s yield strength increases. They concluded that Ti strengthening mainly comes from TiC’s precipitation strengthening. The calculated results do not match the actual measured strength, as the influence of Fe3C precipitates was not considered. This article studied the size distribution and mass percentage of Fe3C and TiC in Ti microalloyed steels produced by TSCR process.

Tables VI through X show the precipitates’ structural parameters, mass fraction of elements in M3C and MC in steel, size distribution of M3C and MC precipitates in the no. 2 sample of Table IV, and mechanical properties of experimental steel, respectively.

Table VI Structural Parameters of Precipitate

Table VI shows the structural parameters of precipitates obtained by X-ray diffraction for the extracted particles by electrolysis. Table VII shows the mass fraction of precipitated phases in steel; from Table VII, it can be seen that the biggest mass fraction of the precipitated phase is M3C cementite-based compounds, followed by Ti (C, N); the mass fraction of M (C, N) equals that of steel containing 0.09 pct Ti in Reference 15. The size distributions of Fe3C and MC precipitates in the no. 2 sample of Table IV determined by XSAS are shown in Tables VIII and IX, respectively.

Table VII Mass Fraction of Elements in M3C and MC in Steel, Mass Percent
Table VIII Size Distribution of M3C Precipitates in Number 2 Sample of Table IV
Table IX Size Distribution of MC Precipitates in Number 2 Sample of Table IV
Table X Mechanical Properties of Experimental Steels*

To further study the existence of nanoscale iron carbon precipitates in HSLA steels, the RTO metal embedded sections micron-nanometer characterization method[16] was used to prepare the sample, and it was analyzed with high-resolution TEM.

The RTO metal embedded sections micron-nanometer characterization method (hereinafter referred to as the RTO characterization method) is a method to embed the micron-nanometer section sample with metal in the organic solution at room temperature. This method solves the problem of cutting nanoscale films from bulk materials such as steel to observe micron-nanoscale particles; it has been widely used in the research of micron-nanoscale materials.[16,17] The steps of cutting nanoscale films from micron-nanoscale materials were described in References 16 and 17.

Using the RTO method, the experimental hot-rolled steel strip piece was electrolyzed in an organic solution for 24 hours, and dehydrated alcohol was used to disperse the electrolyte containing nanoscale precipitates onto the copper foil; then, the nanoscale precipitates on copper foil were embedded by electroplating copper with the aforementioned RTO method. Then, the sample thickness was reduced by means of polishing and an ion thinning instrument to the extent where an electron beam can get through the sample; following this, the sample was observed with high-resolution TEM.

Figure 5 is a TEM morphology picture of a RTO sample made from the precipitates extracted by electrolysis from the experimental steel. From this picture, it can be seen that more precipitates are of size less than 20 nm and are of polygonal shape rather than circular and oval.

Fig. 5
figure 5

TEM photograph of RTO sample for precipitates extracted from experimental steel no. 2 in Table IV

Figures 6 and 7 are the typical energy spectra of Fe3C and TiC precipitates, respectively, in RTO samples, from which the element’s atom percentage can be roughly judged. It is hard to accurately identify the phase composition of precipitates according to EDS results, because the sizes of the nano precipitates are very small.

Fig. 6
figure 6

XEDS spectrum of Fe3C precipitate in RTO sample prepared from steel no. 2 in Table IV

Fig. 7
figure 7

XEDS spectrum of TiC precipitate in RTO sample prepared from steel no. 2 in Table IV

Figures 8 through 10 are high-resolution images and the electron diffraction pattern of Fe3C and M(C, N) precipitate, respectively, in RTO samples prepared from steel no. 2 in Table IV.

Fig. 8
figure 8

High-resolution image of Fe3C precipitates in RTO sample of Ti microalloyed high-strength weathering steel (no. 2 in Table IV)

Fig. 9
figure 9

High-resolution image of TiC precipitates in RTO sample of Ti microalloyed high-strength weathering steel (no. 2 in Table IV)

Fig. 10
figure 10

(a) String of particles containing Fe, Ti, O, and C in ZJ510 microgrid sample and (b) its energy spectrum

4 Contribution of nanoscale iron-carbon precipitates to steel’s precipitation strengthening

4.1 Theoretical Formula of Precipitation Strengthening

Precipitation strengthening is a strengthening method in which the interaction between dispersed fine precipitation phases and the dislocations in steel obstructs the movement of dislocations, thus increasing the strength of steel.

Two types of interactions occur when the moving of dislocations is obstructed by the precipitation phase; as a result, two types of strengthening mechanisms occur. One is called the shearing (cutting) mechanism where dislocations cut the particles; the other is called the bypass (looping) or Orowan mechanism where the dislocations do not penetrate the particles, but bypass them, forming a dislocation loop around the particles.

The precipitation strengthening effect of fine precipitates in steel can be calculated through the simplified formula [1] proposed by Gladman et al.[3] based on Ashby–Orowan’s revised model. When the average diameter of particles is greater than 40 nm, the contribution of precipitation strengthening is not that much.

$$ \sigma = \frac{5.9\sqrt f }{{\bar{x}}} \times \ln \left( {\frac{{\bar{x}}}{{2.5 \times 10^{ - 4} }}} \right) $$
(1)

where σ = the precipitation strengthening contribution to the yield strength (increment), MPa; \( \overline{x} \) = the diameter of precipitates plane intercept, μm; and f = the volume fraction of precipitation phase.

When the diameters of precipitates are very small, and the interface tension between them and the matrix is small, the precipitation is coherent or semicoherent, from[4]

$$ \sigma = \overline{M} \tau_{P} = \frac{2 \times 1.1}{{\sqrt {2AG} }} \times \frac{{\gamma^{3/2} }}{{b^{2} }} \times d^{1/2} f^{1/2} $$
(2)

where τ p  = the shear stress caused by the dislocations cutting with particles, MPa; \( A = \frac{1}{2\pi K}\ln \left( \frac{d}{2b} \right) \) = the dislocation line tension function; K = (1 – v) for edge type dislocation, K = 1 for screw dislocation, and \( \frac{1}{K} = \frac{1}{2}\left( {1 + \frac{1}{1 - v}} \right) \) for mixed type dislocation; v = Poisson’s ratio v = 0.291; b = the absolute value of the dislocation’s Burgess vector, b = 0.248 nm; G = the shear elasticity modulus, 80,650 MPa; γ = interface energy between precipitates and the matrix, γ = 0.5 to 1 J/m2; d = the second-phase particle diameter, μm; f =  the volume percentage; and \( \overline{M} \) = the average Schmid orientation factor, \( \overline{M} \)= 2 for bcc iron.

From formulas [1] and [2], it can be seen that, when steel’s second-phase precipitate strengthening is shearing (cutting) type, its strengthening effect is proportional to the half power of second-phase volume fraction and the half power of particle size d. When it is a bypass mechanism, its strengthening effect is proportional to the half power of the volume fraction and roughly inversely proportional to particle size d; that is, the strengthening effect of the shearing (cutting) mechanism increases with the increasing particle size, while the strengthening effect of the bypass mechanism deceases with the increase of particle size. The critical transformation size d c can be calculated by the numerical solution of Eq. [3]:[5,6]

$$ d_{c} = 0.209\frac{{Gb^{2} }}{K\gamma }\ln \left( {\frac{{d_{c} }}{2b}} \right) $$
(3)

The meanings of symbols in formula [3] are the same as mentioned previously. The critical transformation size of the precipitate depends on the properties of dispersed particles; the smaller the sizes and the smaller the interface energy between the precipitates and the matrix, the larger the d c . Different types of precipitates have different d c values.

4.2 Contribution of Nanoscale Iron Carbon Precipitates to Yield Strength in HSLC Steel

Based on the size distribution, average diameters, crystal parameters, and mass fraction of different types of nano precipitants obtained, assuming the nanoscale precipitates have the same density with large size particles, the precipitation strengthening contribution could be quantitatively calculated.

According to formulas [1] through [3], and the data in Table III, the influence of nanoscale Fe3C to the yield strength of HSLC steel’s was calculated; the results are shown in Table XI.

Table XI Contribution of Fe3C Precipitates Smaller than 20 nm to the Yield Strength of HSLC Steel (MPa)

From Table XI, it can be seen that, for ZJ330 with 0.06 pct carbon content, the contribution of precipitation strengthening increases with the increase of cooling speed of steel (the rolled piece is thinner than slab and its cooling is faster; though the final product is much thinner, the cooling of hot-rolled coil is slower after coiling). The precipitation strengthening contribution of ZJ510 containing 0.18 pct carbon is greater than that of ZJ330. The precipitation strengthening contribution of ZJ330 to the yield strength is about 145 MPa.

4.3 Contribution of Nanoscale Precipitates to the Yield Strength in HSLA Steel

For HSLA steel, it is generally believed that the precipitation strengthening phase is nanoscale carbide of microalloying elements. In our research, it is found that not only the HSLC steel but also the microalloyed HSLA steels have the precipitation strengthening effects[12,13] by nanoscale iron carbon precipitates.

In considering the precipitates’ contribution to yield strength, the combined contributions of precipitates with different types and sizes based on the bypass mechanism and shearing mechanism should be taken into account:

$$ \sigma_{sp} = \sum\limits_{i = 1}^{n} {\sigma_{{sp_{1i} }} } + \sum\limits_{i = 1}^{n} {\sigma_{{sp_{2i} }} } $$
(4)

where i = nanoscale precipitate; \( \sigma_{{sp_{1i} }} \) = precipitation strengthening contribution to the yield strength of steel based on bypass mechanism; and \( \sigma_{{sp_{2i} }} \) = precipitation strengthening contribution to steel’s yield strength based on shearing mechanism.

By calculating, the d c of TiC is 1.5 to 6 nm and the d c of Fe3C is 4.7 to 10 nm. The precipitation strengthening effects of TiC precipitates with different sizes were calculated based on the bypass mechanism; for nanoscale iron carbides with less than 10-nm size, the precipitation strengthening effects of precipitates are calculated based on the shearing mechanism, and for nanoscale iron carbides with size larger than 10 nm, the precipitation strengthening effects are calculated based on the bypass mechanism. The calculated results are listed in Table XII and match the actual measured strength well (as discussed in the Section V–C).

Table XII Contribution of Fe3C and Ti(CN) to the Yield Strength of Ti Microalloyed High-Strength Weathering Steel

In recent years, Zhao et al.[18] studied the distribution of nano cementite in 0.15 pct C, 1.50 pct Mn ferrite + pearlite steel, and found less than 100-nm-diameter ball-shaped cementite particles. The distribution of those particles is not homogeneous; the content is high in some regions.

Chakraborty et al.[19,20] studied the effect of bainite and martensite microstructure refinement on strengthening and toughening in HSLA bearing steel. From their study, the ultrafine grain strengthening and precipitation strengthening cannot be added directly.

Seong et al.[21] studied the influence of nano precipitates in BF (without boron) and BA (containing boron) low-carbon steel on mechanical properties. It was found that boron can reduce strength, improve elongation in low-carbon steel, possibly reduces solved nitrogen and carbon content, and has a negative impact on solid solution strengthening.

Three-dimensional atom probe is an appropriate tool to study nano cementite properties. Kobayashi quantitatively studied the influence of nano TiC particles on the yield strength of Fe-0.03C-0.1Ti-3Al (wt pct) steel.[22] It was found that steel strength increased with the diameter increasing of TiC precipitates when the TiC diameter was less than 3 nm, the precipitation strengthening contribution to yield strength was approximately 250 MPa.

5 Comprehensive strengthening mechanism

Yield strength is a stress when a large amount of dislocation starts moving at the same time; the larger resistance to the dislocation moving means a higher yield strength of the steel. It is generally agreed that the strengthening mechanism consists of solid solution strengthening, grain refinement strengthening, precipitation strengthening, and dislocation strengthening. At the present time, there are two kinds of strengthening theories: ultrafine grain strengthening and the additivity principle of different strengthening mechanisms.

5.1 Ultrafine Grain Strengthening

In the 1950s, Hall and Petch carefully tested the fracture strengths of low-carbon steel with the carbon content of 0.036 to 0.155 pct at room temperature and liquid nitrogen temperature, and they set up the relationship between the cleavage strength and ferrite grain size for the F+P type low-carbon steel.[1]The equation is shown as follows:

$$ \sigma_{c} = \sigma_{c0} + k_{y} d^{ - 1/2} $$
(5)

The effect of the grain size on the toughness of the steel was also studied by Petch. He pointed out that for the ductile-brittle transition temperature, the subsequent equation can be set up.[2]

$$ T_{C} = a - bd^{ - 1/2} $$
(6)

where T C is the ductile-brittle transition temperature, d is the average diameter of the grain, and a and b are constants.

From the Hall–Petch formula, the grain refinement strengthening can increase not only the strength of the steel but also its toughness.

In 1997, the national projects on the new generation steel development were conducted in Japan, Korea, and China with the support of their governments; they were named “Super steel” in Japan, “New generation steel” in China, and “High performance structure steel” in Korea. The theoretical basis and guiding thought of these projects is based on the Hall–Petch formula, regarding the ultrafine grain strengthening mechanisms of structure steels. The aim of the project is to obtain super fine grains as 1 micron meter or even submicron meter (the width of bainite or martensite lathing), thus doubling the steel strength, for the tensile strengths of low alloyed steel and alloyed steel reaching 800 and 1500 MPa, respectively. The situation is different in China; carbon steel with 400 MPa yield strength is included in the project “National Key Basic Research Program (973) of New Generation Steels.” The goal of the project is to produce hot rolling coil of carbon steel with yield strength of 400 MPa and Grade III steel rebar. After 6 years of hard work from 1997 to 2003, it was found that it was impossible to obtain grain sizes of 1 micron meter in steel using the existing equipment and technology by the industrial practices in Japan. In the laboratory, the steel structure can be refined to micron meter scale via a special process, but grain refinement strengthening and dislocation strengthening or precipitation strengthening could not be added and the actual yield strength of steel was lower than the sum.[23]

During the same period, it was found that before and after the tempering–fast cooling for HSLC steel, the grain size did not change, as shown in Figure 11, but the yield strength of the steel improved around 100 MPa, obviously because of the nanoscaled precipitation strengthening. The contribution of precipitation strengthening in quantity was similar to that of grain refinement strengthening.[13]

Fig. 11
figure 11

Microstructure of ZJ330 steels (a) before and (b) after 873 K (600 °C) and (c) 973 K (700 °C) tempering–fast cooling

For Ti microalloyed high-strength weathering steel, the yield strength increases with the Ti content, as shown in Figure 12.

Fig. 12
figure 12

Relationship between yield strength and Ti content and strip thickness of the steel[15]

From Figure 12, we can see that the yield strength of the Ti microalloyed high-strength weathering steel increased more than 300 MPa when the Ti content in steel increased from 0.04 to 0.10 pct with the same average grain size.[15]

5.2 Additivity Principle of Strengthening Mechanism

To the steel strengthening mechanism and additivity principle, many different regression additivity formulas have been put forward. Reference 24 involves a steel strengthening additivity formula:

$$ \sigma = \sigma_{\text{Fe}} + \sigma_{\text{C}} + \sum {\sigma_{\text{ss}} } + K_{1} \left( {L_{3} } \right)^{ - 1} + K_{2} \rho_{\text{d}}^{1/2} + K_{3} \Updelta^{ - 1} $$
(7)

where σ Fe is the strength of pure annealed iron; σ C is the contribution of solid solution strengthening due to carbon; Σσ ss is the sum of contributions to solid solution strengthening from all substitutional solutes; L 3 is the ferrite plate thickness; ρ d is the dislocation density; Δ is the average distance between primary carbide particles; and K 1, K 2, and K 3 are material constants. In formula [7], solid solution strengthening mechanism contributes to the first three items. The last three items is grain refinement strengthening, dislocation strengthening, precipitation strengthening, respectively. The size of the alternate thin plates of ferrite formed in processes is used as the grain size of the grain refinement strengthening in References 18 and 19.

During April 2003 to March 2007, the forum on Steel Yield Strength and Microstructure was organized in Japan; the dominant structure factors on yield strength of different steel grades were investigated, and the results are reported in the Nishiyama Memorial Lecture.[23] It was reported, for low-carbon steel, that the size of the grains decreases until 1 micron meter, the yield strength of steel increases with d −1/2 proportionally, and it is accorded with the Hall–Petch formula; the grain refinement strengthening can be calculated by formula [8]:

$$ \sigma_{s} = 100 + 600d^{ - 1/2} $$
(8)

where σ s is the yield strength (MPa) and d is the grain size (μm). The intercept of the Hall–Petch relation is 100 MPa, by Reference 23, in accordance with the yield strength of single-crystal iron, equivalent to solid solution strengthening. Thus, relation [8] represents the sum of solid solution strengthening and grain refinement strengthening. For different steel grades, the coefficient of \( d^{ - 1/2} \) is different, which means that the Hall–Petch relation has a different slope and intersection and the effect of the grain size and solid solution element on yield strength is different for different steel grades. By this equation, when the grain size of low-carbon steel is 10 to 5 μm, the yield strength σ s will be 290 to 368 MPa. However, in fact, when the grain size of HSLC ZJ330 steel is 8 to 10 μm, the yield strength σ s reaches 410 MPa, meanwhile the elongation rate is still 29 pct.[3] For Ti microalloyed high-strength weathering steel, which contains 0.09 pct of Ti with the grain size of 2.9 to 3.8 μm,[15] the value of σ s calculated by formula [8] is around 408 to 452 MPa, but the actual value is 700 MPa. It can be seen obviously that some other strengthening mechanism contributes to the yield strength σ s , the difference of yield strength between the sum value of solid solution strengthening and grain refinement strengthening, and the actual value can be regarded as the result of precipitation strengthening and dislocation strengthening.

A large amount of dislocation is produced during the rolling process of steel; the interaction between the original dislocation and newborn dislocation or the resistance of the original dislocation against newborn dislocation causes dislocation strengthening or process hardening.

The contribution of dislocation strengthening to the yield strength of steel is proportional to the square root of the dislocation density, according to the Bailay Hirsch formula;[23] the sum of solid solution strengthening and dislocation strengthening can be calculated by experiential formula [9] as follows:

$$ \sigma_{s} = 100 + 1.2 \times 10^{ - 5} \sqrt {\rho_{\text{X - ray}} } $$
(9)

where σ s is the yield strength (MPa), and ρ X-ray is the dislocation density measured by X-ray diffraction. The solid solution strengthening is included in the intersection of formula [9]; this value corresponds to the base strength of the steel. Cold rolling can cause the iron with the maximum of dislocation density of 1016/m2, and the contribution of dislocation strengthening can reach 1200 MPa. When the density of dislocation is less than <1014/m2 in hot-rolled steel, the contribution of dislocation will disappear.[23]

During the period of austenite recrystallization or ferrite cooling (such as coiling of hot-rolled steel plate or heat treatment), the density of dislocation will decrease. The finding that the density of dislocation of the hot-rolled coil of steel plate with thickness 1 mm is 2.8 × 1013/m2 was reported.[25] Considering that the original density of dislocation is related to the pinning of the precipitated secondary phase particles, the resistance of original dislocation to the move of newborn dislocation can be ignored after calculating the precipitation strengthening of the secondary phase particles; that is, the dislocation strengthening can be ignored.

The ultrafine grain strengthening and dislocation strengthening or precipitation strengthening could not be added; the yield strength of steel is dependent on ultrafine grain strengthening adding one of both dislocation strengthening or precipitation strengthening.

It is regarded by the author of Reference 23 that ultrafine grain strengthening and dislocation strengthening or precipitation strengthening cannot be added together; this is because when the value of ultrafine grain strengthening is calculated, the width of bainite or martensite lath is adopted as the grain size; yet, accompanied with the bainite or martensite forming, a large amount of secondary phase particles and dislocation pinned by nanoscale particles precipitated in the steel, which means that ultrafine grain strengthening occurs accompanied with dislocation strengthening and precipitation strengthening. If dislocation strengthening or precipitation strengthening is added with ultrafine grain strengthening, it will be added twice. If we regard the ferrite size as grain size (approximately the grain size before martensite transform), and take into account the nanoscale precipitates in bainite or martensite, the grain refinement strengthening will agree with the Hall–Petch relationship; thus, grain refinement strengthening can be added with the precipitation strengthening.

According to the production level in the 1950s and the test method from the literature,[1] the size of the precipitates in the trial steel may be larger, so the strengthening effect could not be found; it is assumed that the carbon content and the pearlite have little effect on the strength of the steel, so only the grain size plays a decisive role in strengthening this steel.

The assumption is tenable so that the results of the theoretical calculation and the actual test are in accord and the relationship between the yield strength of several materials and the grain size of the ferrite is linear. At this time, σ c0 in Eq. [5] is about tens of MPa, which is the lattice friction force that expresses the influence of intragranular solute atoms on the dislocation movement.

Since the 1970s, in order to improve the strength and toughness of steel, the HSLA steel has been developed. It is found that owing to the addition of the microalloying elements such as V, Nb, and Ti, a large amount of nano microalloy carbonitride M(C x N y ) forms in the grain boundary and intragranular, which have a significant role in precipitation strengthening, and the theoretical value of the strength from the Hall–Petch formula is obviously lower than the actual value. However, the regression relationship between the yield strength and the grain size of the ferrite from the actual production data is still in accordance with the Hall–Petch formula form. Then, the formula of \( \sigma_{s} = \sigma_{s0} + k_{y} d^{ - 1/2} \) expected by Petch can be confirmed. However, this time the formula is only an empirical formula, and under different conditions, σ s0 and k y have different values. σ s0 expresses the contribution of other strengthening mechanisms apart from the fine grain strengthening to the strength of the steel, and k y expresses the influencing degree of the grain size on the strength of the steel under certain conditions, which have different physical meanings than the original formula of Eq. [1]. Therefore, we should carefully consider the application scope of the formula.

The strength of either low-carbon steel or microalloyed steel caused by solid solution strengthening is normally dozens of MPa. The higher contents of alloy elements in steel indicate the higher contribution of solid solution strengthening.

5.3 Quantitative Calculation of Yield Strength by Comprehensive Strengthening Mechanism for Steel

The contribution of nanoscale TiC with size less than 36 nm to the yield strength of Ti alloyed steel was calculated by the present author according to formula [1]. The result is shown in Figure 13.

Fig. 13
figure 13

Contribution of nanoscaled TiC with size less than 36 nm to the strength of Ti microalloyed steel

The result shows that the contribution of TiC precipitate to the yield strength increment of the Ti microalloyed high-strength weathering steel with 0.09 pct Ti is 130 MPa, 200 MPa lower than the actual yield strength. Exploring the reason, it was thought that the contribution of nano precipitate Fe3C was ignored in Reference 15.

The effect of the nanoscale Fe3C precipitate on the yield strength of steel is discussed in this article; it is found that, except nanoscale MC, there exists nanoscale M3C; the contribution of M3C precipitate to the Ti microalloyed high-strength weathering steel with 0.09 pct Ti content reaches 194 MPa (refer to Table XII).

The comprehensive strengthening mechanism for steel is “the yield strength equals all the contribution coming from all kinds of strengthening mechanisms,” which is a “modified additivity principle of the steel strengthening mechanism.” For low-carbon steel, it is regarded that the yield strength of steel equals the sum of solid solution strengthening, grain refinement strengthening, and precipitation strengthening.

That is,

$$ \sigma_{s} = 100 + 600 \times d^{ - 1/2} + \sum\limits_{i = 1}^{n} {\frac{5.9\sqrt f }{{d_{1i} }}\ln \left( {\frac{{d_{1i} }}{{2.4 \times 10^{ - 4} }}} \right)} + \sum\limits_{i = 1}^{n} {\frac{2.2}{{\sqrt {2AG} }} \times \frac{{\gamma^{3/2} }}{{b^{2} }} \times d_{2i}^{1/2} f^{1/2} ; \,d_{1i} \ge d_{c} \ge d_{2i} i = \, 1,2, \ldots ,n} $$
(10)

In formula [10],

  • σ s  = yield strength, MPa;

  • i = nanoscale precipitate;

  • d 1i  = the diameter of nanoscale precipitate by which the precipitation strengthening should be calculated by the bypassing mechanism, μm; and

  • d 2i  = the diameter of nanoscale precipitate by which the precipitation strengthening should be calculated by the incision mechanism, μm.

The values of σ s calculated by formula [10] agree with the actual measured values, as shown in Table XIII.

Table XIII Comparison of Calculated Yield Strength Values with Those of Actual Measured

6 Applications of proposed strengthing mechanism

6.1 Development of Low-Cost High-Strength Steel

6.1.1 HSLC steel

According to the Hall–Petch equation, for Q195 and Q235 steel, it is impossible to improve the yield strength from 200 to 400 MPa by the traditional process. On the basis of that, there existed a large amount of nanoscale Fe3C precipitates in hot-rolled coil produced by CSP line. Guangzhou Zhujiang Steel Co., Ltd., in cooperation with the University of Science and Technology Beijing, developed HSLC steel; it is a one-of-a-kind low-carbon Mn series steel without microalloying elements such as V, Nb, and Ti, and its mechanical properties are similar to the HSLA steel with similar content of carbon and manganese, as shown in Table XIV.

Table XIV Comparison of Chemical Composition and Room-Temperature Strength in 400 MPa Steel Grades

HSLC steel has the property of isotropy, the ratio of transverse and longitudinal yield strength, and tensile strength, and the ratio of elongation is around 0.96 to 1.10.[11]

HSLC steel has the performances of high strength, plasticity, and toughness. The mechanical performances and low-temperature impact toughness of automobile plate ZJ510L are shown in Tables XV and XVI.

Table XV Average Mechanical Performance of ZJ510L
Table XVI Charpy Impact Energy Akv of ZJ510L and ZJ550L, Joule

6.1.2 Container plate steel and Ti microalloyed high-strength weathering steel

Zhujiang Steel, in cooperation with the University of Science and Technology Beijing, developed SPA-H container steel with C ≤ 0.07 pct, Mn 0.25 to 0.5 pct, Si 0.25 to 0.50 pct, P 0.07 to 0.12 pct, S ≤ 0.01 pct, N < 0.005 pct, and Al < 0.04 pct. By controlling low C, low N in composition, controlling rolling, and cooling in process, the total amount of alloy is less than 1 pct, with σ s higher than 400 MPa. The annual output of container steel of Zhujiang Steel is more than 25 pct of the total amount output of the world.

In order to develop container steel with σ s higher than 450 MPa, Ti microalloyed high-strength weathering steel was developed under the laboratory scale and industrial production, precipitation strengthening was considered to obtain high strength. The relationship of the yield strength of the steel and Ti content is shown in Figure 12 and referred to Reference 15.

The series grades of Ti microalloyed high-strength weathering steel were developed at Zhujiang Steel;[26] steel with different Ti contents has unique yield strength. The weight of a container that is made of Ti microalloyed 550 MPa high-strength weathering steel is 15 pct lighter than that made of Ti microalloyed 400 MPa steel (Table XVII).

Table XVII Effect of Reducing Weight of New Generation Lightweight Container

6.1.3 Other steel grades under development

Some steel grades are under development, as shown in Table XVIII, by the union of the University of Science and Technology Beijing, Wuhan University of Science and Technology, and Valin Lianyuan Steel.[27,28]

Table XVIII Other Steel Grades Under Development

6.2 Steel Softening

Steel softening was studied by the author of Reference 29; the tensile strength of ZJ33 decreased from 350 to 250 MPa by tempering and then slow cooling nearly above the temperature of A1. The results are shown in Table XIX.

Table XIX Effect of the Tempering-Slow Cooling near Temperature of A1 on the Mechanical Properties of ZJ330 Steel[29]

6.3 UHU Process on the Basis of Nanoscale Fe3C Precipitation Controlling

The academician, Mr. Guodong Wang, invented a process of ultrafast cooling (UFC), according to the viewpoint of controlling the precipitate in the steel during the production process; it was considered that the process of UHU, in other words, the process of UFC-holding-UFC has an important meaning to the production of wide and heavy plate. Similar to the heat history of CSP hot-rolled strip, continuous cooling can make the thick plate have a more uniform volume fraction of nanoscale precipitates in the center and the edge of the whole plate, which means the plate has a uniform high strength; thus, high-strength steel can be produced with lower cost.

6.4 Technical Analysis of Advanced High-Strength Steel with σb Being 1500 MPa

One of the research goals of advanced high-strength steel is to produce the structure steel with σ b being 1500 MPa in both China and Korea. According to the theory of the comprehensive strengthening mechanism of steel and the control of nanoscale precipitates in the steel, it is considered by the author that in the production of the structure steel with σ b being 1500 MPa, technical measures should be taken as follows.

6.4.1 Enhancing the contribution of solid solution strengthening

According to Orowan’s mechanism, when the size of nanoscale precipitates is larger than 40 nm, their strengthening contribution will be small. Fe3C precipitates less than 40 nm and carbides of other elements will consume a few carbon under fast cooling conditions, so increasing carbon content in the steel will increase the content of carbon in solid solution. Carbon as solute makes a remarkable contribution to solid solution strengthening. Furthermore, increasing the contents of other alloying elements will enhance the contribution of solid solution strengthening.

6.4.2 Enhancing the contribution of precipitation strengthening

The nanoscale carbides of V, Nb, Ti, and Mo will enhance the contribution of precipitation strengthening; meanwhile, the contribution of nanoscale Fe3C precipitate should not be neglected. The effect of V, Nb, Ti, and Mo on nanoscale Fe3C should be studied.

6.4.3 Increasing tempering temperature and cooling speed

The treatment of quenching and tempering is normally adopted in the production of high-strength structure steel with σ b being 1500 MPa. According to the result of tempering–fast cooling experiments, the speed of carbon dispersion is quick at the temperature of 873 K (600°C); the adoption of the process of tempering temperature around 873 K (600°C) and water cooling after tempering is recommended.

6.4.4 Contribution of grain refinement strengthening

Normally, there exists bainite, martensite in high-strength structure steel with σ b being 1500 MPa; the grain size of austenite should be refined before transforming by control rolling and control cooling, in order to enhance fine grain strengthening. The refined austenite grain size should be taken as the parameter of the formula of Hall–Petch.

6.4.5 Improving the cleanness of the steel

According to the comprehensive strengthening mechanism of steel, not only the cooling process after rolling should be controlled but also the metallurgical quality of steel should be controlled; improving the cleanness of the steel is the basis of enhancing the contribution of nanoscale precipitates.

7 Conclusions

  1. 1.

    The measurement of volume fraction and size distribution of nanoscale cementite precipitates in steel were carried out by using chemical phase analysis and XSAS. There existed the nanoscale cementite precipitates with size less than 18 nm in HSLC steel, and that with size less than 36 nm in Ti microalloyed high-strength weathering steel. The volume fraction of Fe3C is 4.4 times as that of Ti (C, N) in the same size range in Ti microalloyed high-strength weathering steel.

  2. 2.

    The comprehensive strengthening mechanism of steel is “the yield strength equals the total amount of all kinds of strengthening mechanism contribution,” which is ‘the modifying additivity principle of strengthening mechanism.” For low-carbon steel, the calculation formula is proposed. The calculated yield strength corresponded to the actual measured result.

  3. 3.

    The interaction among precipitation strengthening and dislocation strengthening, phase transformation, and phase structure and the effect mechanism of microalloying elements V, Nb, Ti, and Mo, and the type and precipitation kinetics of nanosized precipitates are waiting for further study.