The present invention relates to a high pressure above 2 Bar vacuum heat treating furnace, either an integral quench or an external quench design, capable of rapidly cooling the heat treated materials by gas quenching using argon gas at pressures at 10 Bar or higher.
A high pressure vacuum heat treating furnace of the type utilized in the present invention is fully described in U.S. Pat. No. 9,187,799 (Wilson et al.), the disclosure of which is incorporated herein by reference. Although the Wilson et al. design covers only an integral quench vacuum furnace in which the quench system is intimately connected to the furnace hot zone, the present invention is also applicable to external quench systems such as described in U.S. Pat. No. 8,088,328 (Jones), or any external or integral quench design.
Typical quenching gases used in the vacuum furnace industry include nitrogen, hydrogen, helium and argon, or some combinations of these gases. Hydrogen gas presents potential safety issues such as explosive dangers under certain conditions. As more and more specialty alloys contain elements that are reactive to nitrogen, and with restrictions on helium usage due to the worldwide shortage of helium production, argon has become a major quench gas for specialty alloys. Argon gas is the least efficient for cooling due to its much lower thermal conductivity. Typically, argon is blended with some helium up to a 50/50 ratio to provide the higher quenching rates needed for specialty alloys. The cost of helium is approximately ten times the cost of argon, so a significant cost reduction was sought. As the vacuum furnace industry continues to look for faster and more effective quenching capabilities, larger fan motors are required. In order to generate the speed needed to fill the furnace chamber quickly and recycle the gas between the hot zone and the water-cooled heat exchanger, the use of an internal gas blower system is required, as described in Wilson et al.
However, the lower thermal conductivity of argon makes it a less effective quench gas because of its decreased cooling rate, and as a result requires higher pressures and faster recirculation times from the beginning of the quench. As previously stated, argon is generally less effective as a quenching medium due to its much lower thermal conductivity and thus relative cooling capacity compared to nitrogen, helium or hydrogen. The relative cooling rates of the quench gases are as follows: hydrogen—1.50; helium—1.33; nitrogen—1.00; and argon—0.76 (Fabian, Roger; Vacuum Technology. Practical Heat Treating and Brazing; ASM International Materials; Park, Ohio, 1993; page 55). The cooling capacity or cooling coefficient is a measure of the rate of heat removal per unit area per degree of temperature—“Optimizing Gas Quenching” by George C. Carter, Published Advanced Materials and Processes, 1996, reprint available at www.solaratm.com.
The only way to provide the necessary quenching rates with argon at pressures at 10 bar or higher is to increase the fan blower motor horsepower, as explained by Carter as follows:
To compensate for the lower thermal heat transfer effectiveness of argon by convection, the argon gas must be able to move at much faster speeds from its introduction compared to nitrogen or a blend of argon and helium at pressures up to and greater than 10-Bar. For vacuum furnaces as described in Wilson et al. the HP required to cool the workload with all argon gas at 10-Bar is a minimum of 600 HP in order to achieve the quench rates of the argon/helium blend currently used to meet the necessary mechanical and metallurgical properties for certain alloys.
Unfortunately, argon gas has a lower dielectric breakdown voltage than any other quenching gas, and as such requires an alternative blower motor power design to avoid unwanted electrical arcing within the blower motor. When using argon, the fact exists that it can ionize under certain high voltage conditions. This means that if an electrical discharge occurs in the presence of argon, plasma or an arc can occur. As the voltage going into the motor increases above a set voltage, any short circuits to ground between the motor windings will result in a flashover. A glow discharge will be generated that could damage the motor windings and shut down the motor completely, thus terminating the quench cycle. This unacceptable result is a damaged motor and spoiled or damaged workload inside the furnace chamber resulting in incorrect mechanical properties of the parts being heat treated.
These shortcomings led to the design of the present invention vacuum furnace blower motor power system, having an integral quench system capable of providing quench pressures up to or greater than 10 Bar using 100% argon gas. This design is capable of meeting the necessary quench speed to satisfy the required specification for certain mechanical and microstructural properties.
Argon breaks down under applied low voltages, which is referred to as dielectric breakdown. Less than 50 Volts is required to start a glow discharge in argon. This condition would provide a path between the windings of a transformer to ground resulting in a short circuit. An autotransformer (step down) could be used to step the voltage down to 230 Volts. However, the gas velocities with lower voltage would not meet the quench rates required during the initial quench stage. A step-down transformer is not a full isolation transformer. Line to ground will cause short circuits within the blower motor.
Backfilling the furnace chamber with argon using a 460 Volt motor will increase the possibility of argon gas ionization and a short circuit within the blower motor during the quench cycle. As previously discussed, ionization forms plasma and results in an electrical breakdown causing a ground fault condition. To prevent such an occurrence the electrical design for connecting the fan blower motor to the power line had to be redesigned from prior art designs. The present invention provides such a redesigned electrical circuit arrangement to allow for safe practice using 100% argon in a vacuum furnace quenching system utilizing a blower motor rated to run at 460 Volts.
The present design includes a 600 HP-460 Volt blower motor attached to a variable frequency drive (VFD), which is also known as a variable speed drive (VSD), and quenches in 100% argon gas at rates that current conventional designs using 230 Volt motors cannot achieve. The 460 Volt motor is connected to a full isolation transformer to ensure that there is a ground-to-earth safety feature incorporated by virtue of the isolation design. The present design is unique in that the current general teachings indicate that the highest voltage allowed in an argon atmosphere is 230 Volts. The only prior art publication indicating the use of 460 Volts in a high pressure gas quenching vacuum furnace internal system uses nitrogen as the quenching gas. This can be found in U.S. Pat. No. 6,428,742 (Lemken) at column 1, line 15, and column 3, line 56.
Prior art furnace blower motors of greater than 300 HP receiving 460 Volts use an autotransformer to step down 460 Volts to 230 Volts for use in argon as well as nitrogen. All prior art gas quenching furnaces use this method to start the quenching cycle. The use of a 460 Volt blower motor has previously been used only for a nitrogen quench cycle, which starts at 230 Volts up to a maximum pressure then converts to 460 Volts above 750 mBar, as described in Lemken, which specifies nitrogen as the quenching medium. This type of cycle using a step-down transformer with an increase in supply voltage to the blower fan motor at a set higher pressure has not been used with pure argon. A blower motor with voltage greater than 230 Volts has not been used upon initiation of any gas quench cycle, especially argon. Accordingly, the present invention is an improvement over prior art vacuum furnaces. As previously discussed, when 460 Volts supply power is introduced into the windings of a blower motor in an argon atmosphere during a quench cycle, there is a possibility of ionizing the argon gas. If the motor windings become conductive due a short circuit, severe damage to the blower motor and the parts being heat treated will occur.
As will be fully described in the ‘Detailed Description of the Invention,’ power source voltage causes spikes or surges that can wipe out the blower motor even when it is powered down. Use of a variable frequency drive (VFD), (or variable speed drive—VSD), varies the 60 cycle frequency of the current to the motor and changes the speed of the motor. This is described in Wilson et al. at column 5, line 59 to column 6, line 3. The change in frequency can also cause spikes, so a spike preventer must be added to the VFD, which is referred to as a Delta 3-phase metal oxide varistor (MOV) device that filters and clamps transient electrical currents or serves as a voltage spike suppressor to filter and clamp the transients to ground. A varistor is a variable resistor, more commonly referred to as a voltage dependent resistor (VDR), which is a nonlinear voltage dependent device with an electrical behavior closely resembling back-to-back Zener diodes. When exposed to very high voltage transients, the MOV impedance changes dramatically from a nearly open circuit to a highly conductive level, thus dropping the transient voltage to safer levels. The MOV clamps those potential transients, absorbing the energy and thereby protecting the blower motor windings from exposure to higher unexpected voltage that could lead to short circuits and damage the motor. This protective circuitry is very important, especially when the blower motor is located within an ionizing gas such as argon.
The variable frequency drive (VFD) can also cause spikes as the frequency is changed. When the frequency is changed, aborted waveforms can occur that cause a sudden spike in voltage. These spikes can also cause breakdown and damage to the motor. A varistor (motor terminator) is attached to the motor on the opposite side of the isolation transformer from the variable frequency drive (VFD) to protect the motor from any spikes from the VFD aborted waveforms. When a VFD is used, the sinusoidal wave is squared off rather than remaining sinusoidal. The peaks of the squared-off wave can result in transients that could eventually damage the motor winding insulation resulting in a short circuit.
The use of the isolation transformer originates from the ability to isolate or separate the primary motor winding from the secondary winding, thus eliminating ground faults when a 460 Volt motor-to-line design is in use. As an added layer of protection, the present invention isolation transformer includes an additional new feature whereby an electrostatic shield is placed between the primary and secondary windings to prevent transient voltage transfer, as will be shown in the drawings and described in the detailed description of the invention.
The vacuum furnace according to the present invention is designed to quench with argon at 10-Bar pressure while utilizing a 600 HP motor running at 460 Volts from a variable speed drive, and rear head movable gas baffle door, as described in Wilson et al. The goal of the massive quench system is to be able to quench larger batches of power generation castings by increasing the cooling rate and eliminating the supplemental use of helium, while operating in 100% argon. This has proved to be successful in operation, as will be demonstrated in the ‘Time vs Temperature’ graph shown in
The following comparison is to a similar sized furnace that cannot meet the quench rate in 100% argon, as it is limited to a 300 HP motor with a step-down to a 230 Volt transformer. The quench rates for the two identical runs are shown in the graph in
This invention is related to an integral high pressure rapid quenching vacuum furnace utilizing an electrical isolation transformer in the blower motor power control system in order to isolate the motor windings, reduce the possibility of gas ionization and eliminate ground faults, particularly when quenching in argon gas.
In one of its aspects this invention provides a high pressure vacuum furnace for heat treating and rapid gas quenching in argon atmosphere in the same furnace comprising a single chamber having blower means therein, the vacuum furnace comprising power source means, and isolation transformer means operatively connected to the power source means, and wherein the blower means being operatively connected to the isolation transformer means, the isolation transformer means having primary winding means, secondary winding means and electrostatic shield means therebetween, the primary winding means receiving electric power from the power source means, and the blower means receiving electric power from the secondary winding means.
Referring to the drawings wherein like reference numerals refer to the same or similar elements across the multiple views,
The inner wall 102 of gas chamber 105 forms a hot zone 106 of vacuum furnace 100. Hot zone 106 includes a work zone 107 for heat treating a work piece placed in the furnace. It should be understood that the term work piece can refer to a single piece or multiple pieces to be heat treated and rapidly quenched. It should also be understood that the dimensions of the hot zone could be advantageously varied to accommodate larger sized work pieces. Reference is made to Wilson et al., the disclosure of which is fully incorporated herein by reference for a complete description of the arrangement of furnace 100.
Still referring to
As stated previously in the background of the invention, there is a recognition that submerging a motor with greater than 230 Volts into an ionizing gas significantly increases the probability of creating an arc which would damage not only the motor, but also the furnace and any material being heat treated. The National Fire Protection Association standards and other recognized electrical codes for these type of vacuum furnaces include recommendations that a motor cannot exceed 230 Volts in the presence of an ionizing gas such as argon. Since the applicable standards and the established prior art have included the use of an autotransformer, the present invention represents an improvement when using integral high pressure argon gas quench systems. The inclusion of a 460 Volt motor submerged in an ionizing gas such as argon in order to create gas quenching speeds required to meet certain strict cooling rates has not previously been utilized.
In
Although the use of isolation transformers in the electrical technology is not new, for this particular application the use of a 460 Volt rated motor in the presence of specifically argon gas, but also other quench gases such as nitrogen and helium, is new and inventive The present invention goes beyond the current teachings regarding use of a motor in an ionizing gas and provides the opportunity for quenching in argon gas at pressures that have not previously been achieved because of prior art industry electrical limitations.
While there has been described what is believed to be a preferred embodiment of the present invention, those skilled in the art will recognize that other and further modifications may be made thereto without departing from the spirit and scope of the invention. It is therefore intended to claim all such embodiments that fall within the true scope of the invention.
Number | Name | Date | Kind |
---|---|---|---|
4124199 | Jones | Nov 1978 | A |
4141539 | Bornor | Feb 1979 | A |
5127823 | Bonner | Jul 1992 | A |
6428742 | Lemken | Aug 2002 | B1 |
8088328 | Jones | Jan 2012 | B2 |
9187799 | Wilson | Nov 2015 | B2 |
Number | Date | Country | |
---|---|---|---|
20200063225 A1 | Feb 2020 | US |