Surface transformation hardening of carbon steel with high power fiber laser
Qiu, Feng (2013-01-09)
Väitöskirja
Qiu, Feng
09.01.2013
Lappeenranta University of Technology
Acta Universitatis Lappeenrantaensis
Julkaisun pysyvä osoite on
https://urn.fi/URN:ISBN:978-952-265-361-1
https://urn.fi/URN:ISBN:978-952-265-361-1
Tiivistelmä
This study investigated the surface hardening of steels via experimental tests using a
multi-kilowatt fiber laser as the laser source. The influence of laser power and laser
power density on the hardening effect was investigated. The microhardness analysis
of various laser hardened steels was done. A thermodynamic model was developed to
evaluate the thermal process of the surface treatment of a wide thin steel plate with a
Gaussian laser beam. The effect of laser linear oscillation hardening (LLOS) of steel
was examined.
An as-rolled ferritic-pearlitic steel and a tempered martensitic steel with 0.37 wt% C
content were hardened under various laser power levels and laser power densities. The
optimum power density that produced the maximum hardness was found to be
dependent on the laser power. The effect of laser power density on the produced
hardness was revealed. The surface hardness, hardened depth and required laser
power density were compared between the samples. Fiber laser was briefly compared
with high power diode laser in hardening medium-carbon steel.
Microhardness (HV0.01) test was done on seven different laser hardened steels,
including rolled steel, quenched and tempered steel, soft annealed alloyed steel and
conventionally through-hardened steel consisting of different carbon and alloy
contents. The surface hardness and hardened depth were compared among the
samples. The effect of grain size on surface hardness of ferritic-pearlitic steel and
pearlitic-cementite steel was evaluated. In-grain indentation was done to measure the
hardness of pearlitic and cementite structures. The macrohardness of the base material
was found to be related to the microhardness of the softer phase structure. The
measured microhardness values were compared with the conventional macrohardness
(HV5) results.
A thermodynamic model was developed to calculate the temperature cycle, Ac1 and
Ac3 boundaries, homogenization time and cooling rate. The equations were
numerically solved with an error of less than 10-8. The temperature distributions for
various thicknesses were compared under different laser traverse speed. The lag of the was verified by experiments done on six different steels. The calculated thermal cycle
and hardened depth were compared with measured data. Correction coefficients were
applied to the model for AISI 4340 steel.
AISI 4340 steel was hardened by laser linear oscillation hardening (LLOS). Equations
were derived to calculate the overlapped width of adjacent tracks and the number of
overlapped scans in the center of the scanned track. The effect of oscillation
frequency on the hardened depth was investigated by microscopic evaluation and
hardness measurement. The homogeneity of hardness and hardened depth with
different processing parameters were investigated. The hardness profiles were
compared with the results obtained with conventional single-track hardening. LLOS
was proved to be well suitable for surface hardening in a relatively large rectangular
area with considerable depth of hardening. Compared with conventional single-track
scanning, LLOS produced notably smaller hardened depths while at 40 and 100 Hz
LLOS resulted in higher hardness within a depth of about 0.6 mm.
multi-kilowatt fiber laser as the laser source. The influence of laser power and laser
power density on the hardening effect was investigated. The microhardness analysis
of various laser hardened steels was done. A thermodynamic model was developed to
evaluate the thermal process of the surface treatment of a wide thin steel plate with a
Gaussian laser beam. The effect of laser linear oscillation hardening (LLOS) of steel
was examined.
An as-rolled ferritic-pearlitic steel and a tempered martensitic steel with 0.37 wt% C
content were hardened under various laser power levels and laser power densities. The
optimum power density that produced the maximum hardness was found to be
dependent on the laser power. The effect of laser power density on the produced
hardness was revealed. The surface hardness, hardened depth and required laser
power density were compared between the samples. Fiber laser was briefly compared
with high power diode laser in hardening medium-carbon steel.
Microhardness (HV0.01) test was done on seven different laser hardened steels,
including rolled steel, quenched and tempered steel, soft annealed alloyed steel and
conventionally through-hardened steel consisting of different carbon and alloy
contents. The surface hardness and hardened depth were compared among the
samples. The effect of grain size on surface hardness of ferritic-pearlitic steel and
pearlitic-cementite steel was evaluated. In-grain indentation was done to measure the
hardness of pearlitic and cementite structures. The macrohardness of the base material
was found to be related to the microhardness of the softer phase structure. The
measured microhardness values were compared with the conventional macrohardness
(HV5) results.
A thermodynamic model was developed to calculate the temperature cycle, Ac1 and
Ac3 boundaries, homogenization time and cooling rate. The equations were
numerically solved with an error of less than 10-8. The temperature distributions for
various thicknesses were compared under different laser traverse speed. The lag of the was verified by experiments done on six different steels. The calculated thermal cycle
and hardened depth were compared with measured data. Correction coefficients were
applied to the model for AISI 4340 steel.
AISI 4340 steel was hardened by laser linear oscillation hardening (LLOS). Equations
were derived to calculate the overlapped width of adjacent tracks and the number of
overlapped scans in the center of the scanned track. The effect of oscillation
frequency on the hardened depth was investigated by microscopic evaluation and
hardness measurement. The homogeneity of hardness and hardened depth with
different processing parameters were investigated. The hardness profiles were
compared with the results obtained with conventional single-track hardening. LLOS
was proved to be well suitable for surface hardening in a relatively large rectangular
area with considerable depth of hardening. Compared with conventional single-track
scanning, LLOS produced notably smaller hardened depths while at 40 and 100 Hz
LLOS resulted in higher hardness within a depth of about 0.6 mm.
Kokoelmat
- Väitöskirjat [986]