Minimisation of Heating Time for Full Hardening in Hot Stamping Using Direct Resistance Heating

To obtain enough hardness of the die-quenched products after hot stamping using direct resistance heating, the effects of the electrifying condition and initial microstructure of the quenchable steel sheet on hardness were examined in a hot bending experiment. The steel sheet was heated up to 900 °C in 3 to 10 s. The required heating time was shortened by normalising heat treatment due to the fine grain size of the sheet. The standard deviation of the hardness of the sheet heated to 900 °C in 3.2 s without temperature holding at the austenitising temperature was 12 HV, whereas the deviation reduced to 5 HV for temperature holding at the austenitising temperature of 3 s.


Introduction
To reduce the weight and improve the crash safety of automobiles, hot stamping of quenchable steel sheets is useful. By heating the steel sheets, the forming load is remarkably reduced, springback is prevented, and formability is improved [1]. The stamped parts are hardened by quenching with dies, and thus ultra-high strength steel parts with a tensile strength of approximately 1.5 GPa are obtained under a low forming load. In hot stamping, the quenchable steel sheets are heated to approximately 900 • C to transform the sheets to the austenite phase during heating [2]. The sheets are generally heated by a furnace in the conventional warm and hot stamping. So, the temperature decreases due to the takeout procedure of the specimen from the furnace. In addition, the oxidation of the heated sheets occurs due to the forming setup and procedure. Therefore, rapid heating of the sheet is vital to reduce the oxidation scale. By changing the layout of the electrodes, the resistance heating is applicable to heat the sheets. Utilising resistance heating is a rapid way to synchronise with a press, and has higher energy efficiency than the other heating methods such as induction heating.
Mori et al. [3] developed a hot stamping process using rapid resistance heating to improve the productivity and investment cost. The sheets are heated for only 2 s to 900 • C required for quenching. The oxide scale of the products is hardly generated by rapid heating [4]. The efficiency of resistance heating is higher than that of induction heating employed by Kolleck et al. [5] due to the direct passage of current through the sheets. Maki et al. [6] studied the feasibility of hot stamping and press quenching of ultra-high strength steel sheet of SPFC980Y using resistance heating. Ozturk et al. [7] used resistance heating in the hot stamping process of titanium alloy sheets. of the water. Nakagawa et al. [26] reduced the holding time at bottom dead centre in hot stamping by water and die quenching using submerged tools.
In the present study, the hardening behaviour of an uncoated quenchable steel sheet for hot stamping using rapid resistance heating was examined in a hot bending experiment to obtain full hardening of the products. To achieve full hardening, the heating rate was decreased, and the holding at the austenitising temperature was performed in hot stamping using resistance heating.

Hot Stamping Having Simultaneous Heating of Next Blank with the Die Quenching
Resistance heating is attractive for downsizing the hot stamping processes. In resistance heating, steel sheets are Joule-heated by passing current between both the edge electrodes. A hot stamping process having simultaneous heating of the next blank with the die quenching and its time table are shown in Figures 1 and 2, respectively. For furnace heating, the blanks are in a furnace where the temperature is kept constant. So, it is easy to match the timing of taking out the heated blank from the furnace with the finishing of the stamping of the preceded products. On the other hand, for direct resistance heating, heating must be complete just before the die quenching. The heating starts after the die quench of the preceded products, and the die lies idle until the end of heating. The synchronising of direct resistance heating and die-quenching improve the productivity of hot stamping. In addition, having the heating time shorter than the die quenching time is desirable to avoid the bottleneck. speed of the water. Nakagawa et al. [26] reduced the holding time at bottom dead centre in hot stamping by water and die quenching using submerged tools.
In the present study, the hardening behaviour of an uncoated quenchable steel sheet for hot stamping using rapid resistance heating was examined in a hot bending experiment to obtain full hardening of the products. To achieve full hardening, the heating rate was decreased, and the holding at the austenitising temperature was performed in hot stamping using resistance heating.

Hot Stamping Having Simultaneous Heating of Next Blank with the Die Quenching
Resistance heating is attractive for downsizing the hot stamping processes. In resistance heating, steel sheets are Joule-heated by passing current between both the edge electrodes. A hot stamping process having simultaneous heating of the next blank with the die quenching and its time table are shown in Figures 1 and 2, respectively. For furnace heating, the blanks are in a furnace where the temperature is kept constant. So, it is easy to match the timing of taking out the heated blank from the furnace with the finishing of the stamping of the preceded products. On the other hand, for direct resistance heating, heating must be complete just before the die quenching. The heating starts after the die quench of the preceded products, and the die lies idle until the end of heating. The synchronising of direct resistance heating and die-quenching improve the productivity of hot stamping. In addition, having the heating time shorter than the die quenching time is desirable to avoid the bottleneck.

Experimental Procedure of Hat-Shaped Bending Using Direct Resistance Heating
Non-coated 22MnB5 steel sheets are bent into hat-shapes in hot stamping using direct resistance heating to investigate the effects of the resistance heating conditions on hardening behaviour in hot stamping. The details of the used electrodes and dies in the experiment are shown in Figures 3 and  4, respectively. The equipment for resistance heating and the bending dies were installed in a 1500 kN CNC servo press. A typical uncoated quenchable steel sheet non-coated 22MnB5 having 1.6 mm speed of the water. Nakagawa et al. [26] reduced the holding time at bottom dead centre in hot stamping by water and die quenching using submerged tools.
In the present study, the hardening behaviour of an uncoated quenchable steel sheet for hot stamping using rapid resistance heating was examined in a hot bending experiment to obtain full hardening of the products. To achieve full hardening, the heating rate was decreased, and the holding at the austenitising temperature was performed in hot stamping using resistance heating.

Hot Stamping Having Simultaneous Heating of Next Blank with the Die Quenching
Resistance heating is attractive for downsizing the hot stamping processes. In resistance heating, steel sheets are Joule-heated by passing current between both the edge electrodes. A hot stamping process having simultaneous heating of the next blank with the die quenching and its time table are shown in Figures 1 and 2, respectively. For furnace heating, the blanks are in a furnace where the temperature is kept constant. So, it is easy to match the timing of taking out the heated blank from the furnace with the finishing of the stamping of the preceded products. On the other hand, for direct resistance heating, heating must be complete just before the die quenching. The heating starts after the die quench of the preceded products, and the die lies idle until the end of heating. The synchronising of direct resistance heating and die-quenching improve the productivity of hot stamping. In addition, having the heating time shorter than the die quenching time is desirable to avoid the bottleneck.

Experimental Procedure of Hat-Shaped Bending Using Direct Resistance Heating
Non-coated 22MnB5 steel sheets are bent into hat-shapes in hot stamping using direct resistance heating to investigate the effects of the resistance heating conditions on hardening behaviour in hot stamping. The details of the used electrodes and dies in the experiment are shown in Figures 3 and  4, respectively. The equipment for resistance heating and the bending dies were installed in a 1500 kN CNC servo press. A typical uncoated quenchable steel sheet non-coated 22MnB5 having 1.6 mm

Experimental Procedure of Hat-Shaped Bending Using Direct Resistance Heating
Non-coated 22MnB5 steel sheets are bent into hat-shapes in hot stamping using direct resistance heating to investigate the effects of the resistance heating conditions on hardening behaviour in hot stamping. The details of the used electrodes and dies in the experiment are shown in Figures 3 and 4, respectively. The equipment for resistance heating and the bending dies were installed in a 1500 kN CNC servo press. A typical uncoated quenchable steel sheet non-coated 22MnB5 having 1.6 mm in thickness was used for the experiment. The length, width and thickness of the 22MnB5 sheet were 155, 90 and 1.6 mm, respectively, and the heating temperature was 900 • C. Figure 3. The centre portion of the lower surface of the blank was painted by a black body paint, the temperature was measured from the bottom, and feedforward-controlled current was utilised for the experiments. However, black body paint cannot be used in mass production, and it is not suitable for feedforward control. Therefore, it is desirable to measure temperature without contact even at changing emissivity. The two-colour thermometry system without emissivity calibration is suitable for hot stamping production with resistance heating [27].   In this study, the temperature was measured with a spot type infrared thermometer as shown in Figure 3. The centre portion of the lower surface of the blank was painted by a black body paint, the temperature was measured from the bottom, and feedforward-controlled current was utilised for the experiments. However, black body paint cannot be used in mass production, and it is not suitable for feedforward control. Therefore, it is desirable to measure temperature without contact even at changing emissivity. The two-colour thermometry system without emissivity calibration is suitable for hot stamping production with resistance heating [27].   Both ends of the steel sheet in the longitudinal direction were sandwiched between the chromium copper electrode and the stainless-steel holder under a pressure of 1.4 MPa. The blank was heated by the passage of direct current for several seconds. To heat the sheet uniformly, flat copper braids were inserted at the interface between the electrode and the steel sheet to obtain the uniform distribution in electrical contact resistance as shown in Figure 3. The heated blank was released from the holder immediately after heating and was transferred to the hat-shaped bending dies with a pneumatic cylinder. The heated sheet was bent and die-quenched under the conditions of stamping shown in Table 1. Each experiment was performed three times to verify the repeatability of the experiments. It is important to precisely measure the temperature of the blank in hot stamping. However, it is not easy to measure temperature in resistance hating because the electrical noise is significant for thermocouple, and emissivity changes with the growth of the oxide layer for infrared thermometers. In this study, the temperature was measured with a spot type infrared thermometer as shown in Figure 3. The centre portion of the lower surface of the blank was painted by a black body paint, the temperature was measured from the bottom, and feedforward-controlled current was utilised for the experiments. However, black body paint cannot be used in mass production, and it is not suitable for feedforward control. Therefore, it is desirable to measure temperature without contact even at changing emissivity. The two-colour thermometry system without emissivity calibration is suitable for hot stamping production with resistance heating [27].
The heating path and conditions of resistance heating used for the experiment are shown in Figure 5 and Table 2, respectively. The temperature of the blank increases almost linearly with the heating time. The heating rate v during the rise in temperature was adjusted with the current density. The target temperature of 900 • C was held between 0 and 5 s by the passage of low current.  The heating path and conditions of resistance heating used for the experiment are shown in Figure 5 and Table 2, respectively. The temperature of the blank increases almost linearly with the heating time. The heating rate v during the rise in temperature was adjusted with the current density. The target temperature of 900 °C was held between 0 and 5 s by the passage of low current.   An example of a hat-shaped bent part using direct resistance heating is shown in Figure 6. The heating condition is v = 275 °C/s and t = 0 s. A result using furnace heating at 900 °C for 240 s is also shown for comparison. The oxidation of resistance-heated one is remarkably small compared with that of furnace-heated one.   An example of a hat-shaped bent part using direct resistance heating is shown in Figure 6. The heating condition is v = 275 • C/s and t = 0 s. A result using furnace heating at 900 • C for 240 s is also shown for comparison. The oxidation of resistance-heated one is remarkably small compared with that of furnace-heated one.  The heating path and conditions of resistance heating used for the experiment are shown in Figure 5 and Table 2, respectively. The temperature of the blank increases almost linearly with the heating time. The heating rate v during the rise in temperature was adjusted with the current density. The target temperature of 900 °C was held between 0 and 5 s by the passage of low current.  An example of a hat-shaped bent part using direct resistance heating is shown in Figure 6. The heating condition is v = 275 °C/s and t = 0 s. A result using furnace heating at 900 °C for 240 s is also shown for comparison. The oxidation of resistance-heated one is remarkably small compared with that of furnace-heated one.

Effect of Heat Microstructure of Blank Sheet on Quenchability in Die Quenching
To investigate the effect of the microstructure of the blank sheet on the die-quenchability for v = 275 • C/s and t = 0 s as comparatively short heating time, normalise and anneal heat treatment were performed before hot stamping. Then, the heat-treated sheets were resistance-heated, stamped, and quenched for the experiments. The heating path used for the heat treatment and the microstructures of the as-received, normalised and annealed sheets before hot stamping are shown in Figures 7 and 8, respectively. At first, the cut section was polished with emery paper to get a smooth mirror-like surface, and then it was lapped with alumina powder. The polished surface was etched with Nital solution. The optical microscope was utilised for observation. As illustrated in Figure 8, the dark areas show perlite and the light-grey areas show ferrite. All of the sheets in these experiments contain ferrite and perlite structures. The as-received sheet reveals the band structure due to cold rolling; however, the granular perlite with the precipitated ferrite is obtained from normalised sheet. The annealed sheet shows the band structure, because the manganese forms the band structure by rolling and carbon is also segregated according to the segregation of manganese. The grain size of the normalised sheet is considerably small, whereas that for the annealed sheet is large.

Effect of Heat Microstructure of Blank Sheet on Quenchability in Die Quenching
To investigate the effect of the microstructure of the blank sheet on the die-quenchability for v = 275 °C/s and t = 0 s as comparatively short heating time, normalise and anneal heat treatment were performed before hot stamping. Then, the heat-treated sheets were resistance-heated, stamped, and quenched for the experiments. The heating path used for the heat treatment and the microstructures of the as-received, normalised and annealed sheets before hot stamping are shown in Figures 7 and  8, respectively. At first, the cut section was polished with emery paper to get a smooth mirror-like surface, and then it was lapped with alumina powder. The polished surface was etched with Nital solution. The optical microscope was utilised for observation. As illustrated in Figure 8, the dark areas show perlite and the light-grey areas show ferrite. All of the sheets in these experiments contain ferrite and perlite structures. The as-received sheet reveals the band structure due to cold rolling; however, the granular perlite with the precipitated ferrite is obtained from normalised sheet. The annealed sheet shows the band structure, because the manganese forms the band structure by rolling and carbon is also segregated according to the segregation of manganese. The grain size of the normalised sheet is considerably small, whereas that for the annealed sheet is large.  An effect of the heat treatment of the blank before hot stamping on Vickers hardness after dieand water-quenching using direct resistance heating for v = 275 °C/s and t = 0 s is shown in Figure 9. The die-quenched hardness of the as-received sheet using furnace heating of 240 s reaches 450 HV, whereas the die-quenched hardness of the as-received and annealed sheets using direct resistance heating reduce. Figure 10 illustrates the effect of heat treatment of blank on the distributions of Vickers hardness in thickness direction after die-quenching using direct resistance heating for v = 275 An effect of the heat treatment of the blank before hot stamping on Vickers hardness after dieand water-quenching using direct resistance heating for v = 275 • C/s and t = 0 s is shown in Figure 9. The die-quenched hardness of the as-received sheet using furnace heating of 240 s reaches 450 HV, whereas the die-quenched hardness of the as-received and annealed sheets using direct resistance heating reduce. Figure 10 illustrates the effect of heat treatment of blank on the distributions of Vickers hardness in thickness direction after die-quenching using direct resistance heating for v = 275 • C/s and t = 0 s. The hardness scatter of the normalised sheet becomes approximately steady in thickness direction, whereas it increases for the annealed sheet and decreases for the as-received one. The result of Figure 9 was arranged based on the grain size of the microstructure of the blank and is shown in Figure 11.
All heat-treated sheets have enough hardness in case of water quenching. Therefore, the quenchability of the sheet is a reason for insufficient hardness. The manganese and boron have a large effect on the quenchability. However, since the band structure was formed for as-received and annealed sheets as shown in Figure 8, it expects the segregation of manganese and boron near perlite and grain boundary. So, it is difficult to diffuse those to ferrite for short heating time, hence the low quenchability portion partially appears.       The microstructures of the die-and water-quenched sheets from as-received, normalised and annealed sheets for v = 275 °C/s and t = 0 s are shown in Figure 12. On the results of die quenching, ferrite is observed for as-received and annealed sheets. In particular, ferrite forms a thick layer in the result of the annealed sheet, corresponding to the microstructure shown in Figure 8c. As a result of Figure 11. Effect of average grain size of blank on Vickers hardness after die-and water-quenching using direct resistance heating for v = 275 • C/s and t = 0 s. The microstructures of the die-and water-quenched sheets from as-received, normalised and annealed sheets for v = 275 • C/s and t = 0 s are shown in Figure 12. On the results of die quenching, ferrite is observed for as-received and annealed sheets. In particular, ferrite forms a thick layer in the result of the annealed sheet, corresponding to the microstructure shown in Figure 8c. As a result of water quenching, a small ferrite layer was observed for both the as-received and the annealed sheets. A full martensitic transformation occurred for the result from the normalised sheet even for the comparatively short heating time of direct resistance heating. water quenching, a small ferrite layer was observed for both the as-received and the annealed sheets. A full martensitic transformation occurred for the result from the normalised sheet even for the comparatively short heating time of direct resistance heating.

Full Hardening of Products by a Decrease in Heating Rate and by Temperature Holding in Hot Stamping Using Direct Resistance Heating
The effect of the heating rate on the Vickers hardness and the standard deviation of the asreceived sheet without pre-heating treatment for t = 0 s is shown in Figure 13. As the heating rate decreases, the standard deviation of the hardness improves and the hardness slightly increases. The heating rate is required below a certain value for full hardening.

Full Hardening of Products by a Decrease in Heating Rate and by Temperature Holding in Hot Stamping Using Direct Resistance Heating
The effect of the heating rate on the Vickers hardness and the standard deviation of the as-received sheet without pre-heating treatment for t = 0 s is shown in Figure 13. As the heating rate decreases, the standard deviation of the hardness improves and the hardness slightly increases. The heating rate is required below a certain value for full hardening. The heating temperature was held at the target temperature for several seconds to obtain full hardening even for a short heating time in direct resistance heating. The variations in temperature in resistance heating with and without holding at 900 °C above the austenitising temperature for v = 275 °C/s are shown in Figure 14. After reaching 900 °C, the temperature was kept almost constant by resistant-heating under low current. The hot hat-shaped bent parts for v = 275 °C/s and t = 0, 5, and 10 s are shown in Figure 15. The appearances about oxidation of the formed products are similar to the parts without temperature holding due to the short temperature holding time. The heating temperature was held at the target temperature for several seconds to obtain full hardening even for a short heating time in direct resistance heating. The variations in temperature in resistance heating with and without holding at 900 °C above the austenitising temperature for v = 275 °C/s are shown in Figure 14. After reaching 900 °C, the temperature was kept almost constant by resistant-heating under low current. The hot hat-shaped bent parts for v = 275 °C/s and t = 0, 5, and 10 s are shown in Figure 15. The appearances about oxidation of the formed products are similar to the parts without temperature holding due to the short temperature holding time. The hot hat-shaped bent parts for v = 275 • C/s and t = 0, 5, and 10 s are shown in Figure 15. The appearances about oxidation of the formed products are similar to the parts without temperature holding due to the short temperature holding time. The effect of temperature holding during austenitising on the Vickers hardness and standard deviation of that for v = 275 °C/s is shown in Figure 16. As the holding time during austenitising increases, the hardness slightly increases up to t = 5 s. The standard deviation of the hardness is remarkably reduced by temperature holding above 1 s and is similar to the result of furnace heating. The microstructures of hot hat-shaped bent parts with and without temperature holding during austenitising for v = 275 °C/s are shown in Figure 17. By temperature holding, formation of the ferrite is prevented, and the fully martensitic structures are obtained for t = 5 and 10 s. The effect of temperature holding during austenitising on the Vickers hardness and standard deviation of that for v = 275 • C/s is shown in Figure 16. As the holding time during austenitising increases, the hardness slightly increases up to t = 5 s. The standard deviation of the hardness is remarkably reduced by temperature holding above 1 s and is similar to the result of furnace heating. The effect of temperature holding during austenitising on the Vickers hardness and standard deviation of that for v = 275 °C/s is shown in Figure 16. As the holding time during austenitising increases, the hardness slightly increases up to t = 5 s. The standard deviation of the hardness is remarkably reduced by temperature holding above 1 s and is similar to the result of furnace heating. The microstructures of hot hat-shaped bent parts with and without temperature holding during austenitising for v = 275 °C/s are shown in Figure 17. By temperature holding, formation of the ferrite is prevented, and the fully martensitic structures are obtained for t = 5 and 10 s. The microstructures of hot hat-shaped bent parts with and without temperature holding during austenitising for v = 275 • C/s are shown in Figure 17. By temperature holding, formation of the ferrite is prevented, and the fully martensitic structures are obtained for t = 5 and 10 s. The decrease in heating rate and temperature holding during austenitising are effective for full hardening of products in hot stamping using direct resistance heating. The total heating times with and without temperature holding during austenitising were compared. The relationships between the Vickers hardness and total heating time with and without temperature holding during austenitising are shown in Figure 18. For resistance heating with temperature holding, the sufficient hardness was obtained above 4 s, whereas 8 s is required without temperature holding. The minimum heating time for full hardening is decided to 4 s based on the hardness in this quenchable steel sheet in hot stamping using direct resistance heating. The rapid heating rate with temperature holding during austenitising is effective to minimise the heating time for full hardening. The effect of the total heating time on the thickness of the oxide layer of hat-shaped bent parts in hot stamping using direct resistance heating is shown in Figure 19. The oxide layer was removed by the soaking into the 3% hydrochloric acid with ultrasonic vibration. Then, the thickness was measured after removing the oxide layer. The thickness of the oxide layer is half of the difference in thickness of between that before and after oxide removing. The thicknesses of the oxide layer of both heating paths increase with the increase of the total heating time. For the result using temperature holding, the thicknesses of the oxide layer are slightly thicker than that without temperature holding owing to the fact that the time at the high temperature was slightly long. The decrease in heating rate and temperature holding during austenitising are effective for full hardening of products in hot stamping using direct resistance heating. The total heating times with and without temperature holding during austenitising were compared. The relationships between the Vickers hardness and total heating time with and without temperature holding during austenitising are shown in Figure 18. For resistance heating with temperature holding, the sufficient hardness was obtained above 4 s, whereas 8 s is required without temperature holding. The minimum heating time for full hardening is decided to 4 s based on the hardness in this quenchable steel sheet in hot stamping using direct resistance heating. The rapid heating rate with temperature holding during austenitising is effective to minimise the heating time for full hardening. The decrease in heating rate and temperature holding during austenitising are effective for full hardening of products in hot stamping using direct resistance heating. The total heating times with and without temperature holding during austenitising were compared. The relationships between the Vickers hardness and total heating time with and without temperature holding during austenitising are shown in Figure 18. For resistance heating with temperature holding, the sufficient hardness was obtained above 4 s, whereas 8 s is required without temperature holding. The minimum heating time for full hardening is decided to 4 s based on the hardness in this quenchable steel sheet in hot stamping using direct resistance heating. The rapid heating rate with temperature holding during austenitising is effective to minimise the heating time for full hardening. The effect of the total heating time on the thickness of the oxide layer of hat-shaped bent parts in hot stamping using direct resistance heating is shown in Figure 19. The oxide layer was removed by the soaking into the 3% hydrochloric acid with ultrasonic vibration. Then, the thickness was measured after removing the oxide layer. The thickness of the oxide layer is half of the difference in thickness of between that before and after oxide removing. The thicknesses of the oxide layer of both heating paths increase with the increase of the total heating time. For the result using temperature holding, the thicknesses of the oxide layer are slightly thicker than that without temperature holding owing to the fact that the time at the high temperature was slightly long. The effect of the total heating time on the thickness of the oxide layer of hat-shaped bent parts in hot stamping using direct resistance heating is shown in Figure 19. The oxide layer was removed by the soaking into the 3% hydrochloric acid with ultrasonic vibration. Then, the thickness was measured after removing the oxide layer. The thickness of the oxide layer is half of the difference in thickness of between that before and after oxide removing. The thicknesses of the oxide layer of both heating paths increase with the increase of the total heating time. For the result using temperature holding, the thicknesses of the oxide layer are slightly thicker than that without temperature holding owing to the fact that the time at the high temperature was slightly long. From the aforementioned results, it was found that the increase in the heating time due to holding at the austenitising temperature and decrease in heating rate is small, and this time is included in the time for transferring the heated sheet to dies. For example, it is conceivable to maintain the temperature by installing an electrode on the transfer manipulator as shown in Figure  20.

Conclusions
Hot stamping using direct resistance heating is attractive due to high and flexible productivity and low investment. Sufficient austenitisation is important even in a short heating time with rapid resistance heating to obtain the full hardening. Since the initial microstructure of the steel sheet affects the quenchability of the sheets, it is important to care for the microstructure of the blank such as band structures by rolling. The development of normalised steel sheets is suitable for rapid resistance heating. Since it is not difficult to normalise a steel sheet at material production, the use of that can be effective to reduce the heating time for austenitisation and to obtain high productivity. Full hardening was obtained, and the standard deviation of the hardness was reduced by holding at the austenitising temperature and the decrease in heating rate.   From the aforementioned results, it was found that the increase in the heating time due to holding at the austenitising temperature and decrease in heating rate is small, and this time is included in the time for transferring the heated sheet to dies. For example, it is conceivable to maintain the temperature by installing an electrode on the transfer manipulator as shown in Figure 20. From the aforementioned results, it was found that the increase in the heating time due to holding at the austenitising temperature and decrease in heating rate is small, and this time is included in the time for transferring the heated sheet to dies. For example, it is conceivable to maintain the temperature by installing an electrode on the transfer manipulator as shown in Figure  20.

Conclusions
Hot stamping using direct resistance heating is attractive due to high and flexible productivity and low investment. Sufficient austenitisation is important even in a short heating time with rapid resistance heating to obtain the full hardening. Since the initial microstructure of the steel sheet affects the quenchability of the sheets, it is important to care for the microstructure of the blank such as band structures by rolling. The development of normalised steel sheets is suitable for rapid resistance heating. Since it is not difficult to normalise a steel sheet at material production, the use of that can be effective to reduce the heating time for austenitisation and to obtain high productivity. Full hardening was obtained, and the standard deviation of the hardness was reduced by holding at the austenitising temperature and the decrease in heating rate.

Conclusions
Hot stamping using direct resistance heating is attractive due to high and flexible productivity and low investment. Sufficient austenitisation is important even in a short heating time with rapid resistance heating to obtain the full hardening. Since the initial microstructure of the steel sheet affects the quenchability of the sheets, it is important to care for the microstructure of the blank such as band structures by rolling. The development of normalised steel sheets is suitable for rapid resistance heating. Since it is not difficult to normalise a steel sheet at material production, the use of that can be effective to reduce the heating time for austenitisation and to obtain high productivity. Full hardening was obtained, and the standard deviation of the hardness was reduced by holding at the austenitising temperature and the decrease in heating rate.

Conflicts of Interest:
The authors declare no conflict of interest.