EP0212007B1

EP0212007B1 - Process for cracking heavy hydrocarbon to produce olefins and liquid hydrocarbon fuels

Info

Publication number: EP0212007B1
Application number: EP19850201308
Authority: EP
Inventors: Robert J. Gartside; Axel R. Johnson; Joseph L. Ross
Original assignee: Stone and Webster Engineering Corp
Current assignee: Stone and Webster Engineering Corp
Priority date: 1985-08-13
Filing date: 1985-08-13
Publication date: 1989-12-27
Also published as: DE3574987D1; EP0212007A1

Description

This invention relates to the production of olefins and liquid hydrocarbon fuels from heavy hydrocarbons, and, more particularly, to the production of olefins in a thermal cracking environment.
It has long been known that naturally occurring hydrocarbons can be cracked at high temperatures to produce olefins and liquid fuel. Both catalytic and non-catalytic cracking processes exist to produce olefins and hydrocarbon fuel from heavy, naturally occurring, hydrocarbons.
However, as lighter hydrocarbons are consumed, the petroleum- and the petrochemical industry has had to focus on the use of heavier hydrocarbons, such as residual oils. Residual oils are customarily identified as residual, reduced crude oils, atmospheric tower bottoms, vacuum residual oils, topped crudes and most hydrocarbons heavier than gas oils. The problem with the residual oils is that they contain contaminants, such as sulphur and metals. Heavy metals are particularly troublesome in catalytic cracking operations. The heavy hydrocarbons also contain a greater abundance of coke precursors (asphaltenes, polynuclear aromatics, and the like). Coke precursors to convert to coke during the cracking operation and tend to foul the equipment and catalyst or inert particles used in the cracking process.
Many methods have been developed to deal with the problem of cracking residual oils, generally by pretreating the residual oil before cracking. Solvent deasphalting, fluid or delayed coking or hydrotreating are residual feed pretreating processes: they are essentially carbon-rejecting processes which result in a substantial loss of feedstock. Hydrotreating typically takes a heavy toll on the economics of the processing due to the poisonous effect of the contaminants on the catalyst and on the consumption of hydrogen.
FR-A 2 247 527 discloses a process in which petroleum is split into fractions by subjecting the fractions which pass above a temperature of from 350_°C to 500_°C to a thermal transformation by contacting with a fluidized bed of a heat-carrier held at a temperature between 500_°C and 670°C, for a time from 10 to 15 s, in the presence of from 25% to 100% of steam, on a weight basis, and subsequently subjecting the fractions passing above temperatures of from 360_°C to 500_°C to a co-current transformation with a heat-carrier at a temperature of from 560_°C to 800_°C, for a time of from 0,3 s to 3,0 s, the fractions passing below a temperature of from 350_°C to 500_°C being so transformed as to have the transformation products reaching the fluidized bed environment.
The comparatively low temperatures ranges selected in FR-A 2 247 527 require long residence times and the use of a fluidized bed and of added steam contribute towards rendering the process cumbersome.
EP-A 0 026 674 discloses a thermal regenerative cracking (TRC) process using coke particles as heat-carriers, which are then centrifugally separated from the diluted mixed-phase stream of gas and solids.
Also this process is cumbersome and economically unsatisfactory.
The objects of the present invention thus are to crack heavy hydrocarbon to produce olefins and liquid fuels, and, additionally, to crack atmospheric tower bottoms by first processing the atmospheric tower bottoms through a vacuum tower and separately cracking the vacuum oil and the vacuum resid.
To achieve these objects, the present invention, therefore, provides: A process for the production of olefins or light hydrocarbon fuels comprising the steps of: (a) separating a heavy hydrocarbon into a light hydrocarbon fraction and a heavy hydrocarbon fraction; (b) thermally cracking the light hydrocarbon fraction with heat supplied by hot particulate solids; (c) separating the cracked product from the hot particulate solids; (d) delivering the separate particulate solids to a stripper-coker; (e) introducing the heavy hydrocarbon in the stripper-coker to produce vaporized hydrocarbon and coke; (f) combusting the coke produced in the reactor and stripper-coker to heat the particulate solids, and (g) returning the heated particulate solids to the thermal cracking reactor.
According to a preferred embodiment of the present invention, the thermal cracking temperature is about 816°C (1500_°F), the ratio of solids to light hydrocarbon by weight is between 5 and 60, and the reaction residence time is from 0,05 to 0,50 s.
The process of the present invention is exemplarily illustrated in the accompanying drawings, wherein:

FIGURE 1 is a schematic view of the instant process.
FIGURE 2 is a cross-sectional elevational view of the reactor feeder in the thermal regenerative (TRC) cracking system.
FIGURE 3 is a cross-sectional elevational view of the separator of the thermal regenerative (TRC) cracking process, and
FIGURE 4 is a sectional view through line 4-4 of FIGURE 3.

The process of the present invention is directed to producing olefins and liquid fuels from a heavy hydrocarbon feed. Atmospheric tower bottoms (ATB) are well suited for processing by the process of the present invention. However, any heavy feed, such as residual oil, that can be separated into a light and a heavy stream can be processed by the present invention.
As best seen in FIGURE 1, the system is comprised essentially of a vacuum tower 2 and a thermal regenerative cracking assembly. The thermal regenerative cracking assembly is comprised of a thermal regenerative cracking reactor 6, a reactor feeder 4, a separator 8 and a coke stripper vessel 10. The system also includes means for regenerating solids particles separated from the cracked product after the reaction. The system shows illustratively an entrained bed heater 16, a transport line 12 and a fluid bed vessel 14 in which the solids can be regenerated.
In the process of the present invention, atmospheric tower bottoms are delivered through line 3 to a conventional vacuum tower 2 (operated at about 26,66 millibar) wherein the atmospheric tower bottoms (ATB) are separated into a light overhead vacuum oil stream and a heavier bottoms vacuum resid. The vacuum gas oil is condensed and then passed through line 20 to the thermal regenerative cracking reactor 6.
The vacuum gas oil is delivered to the reactor 6 with hot solids particles that are passed through the reactor feeder 4 (best seen in FIGURE 2). Immediate intimate mixing of the hot solids and the vacuum gas oil occurs in the reactor and cracking proceeds immediately. The temperature of the solids entering the reactor is in the range of 954_°C (1750_°F). The vacuum gas oil is delivered to the reactor at approximately 371 _°C (700_°F). The solids to feed weight ratio is 5 to 60, and the reaction proceeds at 816_°C (1500_°F) for a residence time of about 0.05 to 0.50 seconds, preferably from 0.20 to 0.30. The product gases are separated from the solids in separator 8 (best seen in FIGURE 3) and the product gases pass overhead through a line 22 and are immediately quenched with typical quench oil that is delivered to line 22 through line 36. The quenched product is passed through a cyclone 24 where entrained solids are removed and delivered through line 45 to the coker stripper 10.
The separated solids leave the separator 8 through line 26 and pass to the stripper coker 10. At the same time, vacuum resid from line 32 is delivered to the stripper coker 10 and is cracked by the solids which are now at a temperature of approximately 704_°C (1300_°F) to 871 _°C (1600_°F). The weight ratio of solids to vacuum resid in the stripper coker ranges from 5 to 1 to 60 to 1. Thus, the vacuum resid is elevated to a temperature of 510_°C-677_°C (950_°F-1250_°F). The vaporized product from the vacuum resid is taken ouverhead through line 30 and either delivered for processing in line 34 or taken directly out of the system through line 42.
The solids which have accumulated coke in both the tubular reactor 6 and the stripper coker 10 are passed to the entrained bed heater 16 and combusted with air delivered to the system through line 44 to provide the heat necessary for thermal regenerative cracking in the reactor 6.
The reactor feeder 4 of the TRC processing system is particularly well suited for use in the system due to the capacity to rapidly admix hydrocarbon feed and particulate solids. As seen in FIGURE 2, the reactor feeder 4 delivers particulate solids from a solids receptacle 70 through vertically disposed conduits 72 to the reactor 6 and simultaneously delivers hydrocarbon feed to the reactor 6 at an angle into the path of the particulate solids discharging form the conduits 72. An annular chamber 74 to which hydrocarbon is fed by a toroidal feed line 76 terminates in angled openings 78. A mixing baffle or plug 80 also assists in effecting rapid and intimate mixing of the hydrocarbon feed and the particulate solids. The edges 79 of the angled openings 78 are preferably convergently beveled, as are the edges 79 at the reactor end of the conduits 72. In this way, the gaseous stream from the chamber 74 is angularly injected into the mixing zone and intercepts the solids phase flowing from conduits 78. A projection of the gas flow would form a cone shown by dotted lines 77, the vortex of which is beneath the flow path of the solids. By introduing the gas phase angularly, the two phases are mixed rapidly and uniformly, and form a homogeneous reaction phase. The mixing of a solid phase with a gaseous phase is a function of the shear surface between the solids and gas phases, and the flow area. As ratio of shear surface to flow area (S/A) of infinity defines perfect mixing; poorest mixing occurs when the solids are introduced at the wall of the reaction zone. In the system of the present invention, the gas stream is introduced annularly to the solids which ensures high shear surface. By also adding the gas phase transversely through an annular feed means, as in the preferred embodiment, penetration of the phases is obtained and even faster mixing results. By using a plurality of annular gas feed points and a plurality of solid feed conduits, even greater mixing is more rapidly promoted, since the surface to area ratio for a constant solids flow area is increased. Mixing is also a known function of the L/D of the mixing zone. A plug creates an effectively reduced diameter D in a constant L, thus increasing mixing.
The plug 80 reduces the flow area and forms discrete mixing zones. The combination of annular gas addition around each solids feed point and a confined discrete mixing zone greatly enhances the conditions for mixing. Using this preferred embodiment, the time required to obtain an essentially homogenous reaction phase in the reaction zone is quite low. Thus, this preferred method of gas and solids addition can be used in reaction systems having a residence time below 1 second, and even below 100 milliseconds. Because of the environment of the reactor 6 and reactor feeder 4, the walls are lined with an inner core 81 of ceramic material. The detail of the reactor feeder is more fully described in United States Letters Patent No. 4,388,187, which is incorporated herein by reference.
The separator 8 of the TRC system seen in FIGURE 3, can also be relied on for rapid and discrete separation of cracked product and particulate solids discharging from the reactor 6. The inlet to the separator 8 is directly above a right angle corner 90 at which a mass of particulate solids 92 collect. A weir 94 downstream from the corner 90 facilitates accumulation of the mass of solids 92. The gas outlet 22 of the separator 8 is oriented 180_° from the separator gas-solids inlet 96 and the solids outlet 26 is directly opposed in orientation to the gas outlet 22 and downstream of both the gas outlet 22 and the weir 94. In operation, centrifugal force propels the solid particles to the wall opposite inlet 96 of the chamber 93 while the gas portion having less momentum, flows through the vapor space of the chamber 93. Initially, solids impinge on the wall opposite the inlet 96 but subsequently accumulate to form a static bed of solids 92 which ultimately form in a surface configuration having a curvilinear arc of approximately 90_° of a circle. Solids impinging upon the bed 92 are moved along the curvilinear arc to the solids outlet 95, which is preferably oriented for downflow of solids by gravity. The exact shape of the arc is determined by the geometry of the particular separator and the inlet stream parameters such as velocity, mass flowrate, bulk density, and particle size. Because the force imparted to the incoming solids is directed against the static bed 92 rather than the separator 8 itself, erosion is minimal. Separator efficiency, defined as the removal of solids from the gas phase leaving through outlet 97 is, therefore, not affected adversely by high inlet velocities, up to 45,75 m/s (150 ft./sec), and the separator 8 is operable over a wide range of dilute phase densities, preferably between 1,6033 kg/m³ and 160,33 kg/m³ (0,1 lbs./ft3 and 10,0 lbs./ft³). The separator 8 of the present invention achieves efficiences of about 80%, although the preferred embodiment can obtain over 90% removal of solids.
It has been found (see EP-A 0 026 674, page 37, line 2 to page 38, line 24) that separator efficiency is dependent upon separator geometry, and, more particularly, the flow path must be essentially rectangular, and there is an optimum relationship between the height H and the sharpness of the U-bend in the gas flow.
It has been found that, for a given height H of the chamber 93, efficiency increases as the 3,14 rad (1800) U-bend between inlet 96 and outlet 97 is brought progressively closer to inlet 96. Thus, for a given H, the efficiency of the separator increases as the flow path decreases and, hence, residence time decreases. Assuming an inside diameter D; of inlet 96, the preferred distance CL between the centerlines of inlet 96 and outlet 97 is not greater than 4,0 Di, while the most preferred distance between said centerlines is between 1,5 and 2,5 Di.
Below 1,5 Di, better separation is obtained, but difficulty in fabrication makes this embodiment less attractive in most instances. Should this latter embodiment be desired, the separator 8 would probably require a unitary casting design because inlet 96 and outlet 97 would be too close to one another to allow welded fabrication.
It has been found that the height of the flow path H should be at least equal to the value of Di, or 101,6 mm (4 inches) in height, whichever is the greater. Practice teaches that, if H is less than D; or 101,6 mm (4 inches), the incoming stream is apt to disturb the bed solids 92, thereby re-entraining solids in the gas product leaving through outlet 97. Preferably, H is on the order of twice D;, to obtain even greater efficiency. While not otherwise limited, it is apparent that too large an H eventually merely increases residence time without substantive increases in efficiency. The width W of the flow path is preferably between 0.75 and 1.25 times Di most preferably between 0.9 and 1.10 Di.
Outlet 97 may be of any inside diameter. However, velocities greater than 22,875 m/s (75 ft./sec) can cause erosion because of residual solids entrained in the gas. The inside diameter of outlet 97 should be sized so that a pressure differential between the stripping vessel 10 shown in FIG. 1 and the separator 8 exist such that a static height of solids is formed in solids outlet line 26. The static height of solids in line 26 forms a positive seal which prevents gases from entering the stripping vessel 10. The magnitude of the pressure differential between the stripping vessel 10 and the separator 8 is determined by the force required to move the solids in bulk flow to the solids outlet 95 as well as the height of solids in line 26. As the differential increases the net flow of gas to the stripping vessel 10 decreases. Solids, having gravitational momentum, overcome the differential, while gas preferentially leaves through the gas outlet.
FIG. 4 shows a cutaway view of a the separator along section 4-4 of FIG. 3. It is essential that longitudinal side walls 101 and 102 should be rectilinear, or slightly arcuate as indicated by the dotted lines 101a and 102a. Thus, the flow path through the separator 8 is essentially rectangular in cross section having a height H and width W as shown in Fig. 4. The embodiment shown in FIG. 4 defines the geometry of the flow path by adjustment of the lining width for walls 101 and 102. Alternatively, baffles, inserts, weirs or other means may be used. In like fashion the configuration of walls 103 and 104 transverse to the flow path may be similarly shaped, although this is not essential.
The separator shell and manways are preferably lined with erosion resistent linings 105, which may be required if solids at high velocities are encountered. Typical commercially available materials for erosion resistent lining include Carborundum Precast Carbofrax D, Carborundum Precast Alfrax 201 or their equivalent. A thermal insulation lining 106 may be placed between the shell land the lining 105 and between the manways and their respective erosion resistent linings when the separator is to be used in high temperatures service. Thus, process temperatures above 1500_°F (816_°C) can be used.
The detail of the separator 8 is more fully described in United States Letters Patent No. 4 288 235.
The following example illustrates the process of the present invention. An atmospheric tower bottoms (ATB) having essentially 44% vacuum resid and 56% vacuum gas oil has the following composition:
28 465,8 kg (62,700 pounds) of atmospheric tower bottoms are delivered through line 3 to the vacuum tower 2. 15935,4kg (35,100 pounds) of vacuum gas oil is taken from the vacuum tower 2 to line 20 and 12 530,4 kg (27,600 pounds) per hour of vacuum resid is taken through line 32. The vacuum gas oil is delivered to the reactor 6 and cracked with particulate solids which have been elevated in temperature to 954_°C (1750_°F). The solids to hydrocarbon feed ratio by weight is 22.
Cracking proceeds at 816_°C (1500_°F) for 0.20 seconds. Approximately 462,172 kg (1018 pounds) per hour for coke is produced on the particles in the reactor 6.
The 12 530,4 kg (27,600 pounds) per hour of vacuum resid is delivered to the coker 10 at approximately 343_°C (650_°F).
Therein 1253,04 kg (2760 pounds) per hour of coke is produced. The total coke produced in the system is 1715,212 kg (3778 pounds). The over all combined yield from the process is:

Claims

1. A process for the production of olefins or light hydrocarbon fuels comprising the steps of:

(a) separating a heavy hydrocarbon into a light hydrocarbon fraction and a heavy hydrocarbon fraction;

(b) thermally cracking the light hydrocarbon fraction with heat supplied by hot particulate solids;

(c) separating the cracked produce from the hot particulate solids;

(d) delivering the separate particulate solids to a stripper-coker;

(e) introducing the heavy hydrocarbon fraction in the stripper-coker to produce vaporized hydrocarbon and coke;

(f) combusting the coke produced in the reactor and stripper-coker to heat the particulate solids, and

(g) returning the heated particulate solids to the thermal cracking reactor.

2. A process according to claim 1, wherein the thermal cracking temperature is 816°C (1500_°F), the ratio of solids to light hydrocarbon by weight is between 5 and 60, and the reaction residence time is from 0,05 to 0,50 s.

3. A process according to claim 2, wherein the temperature of the solids delivered to the stripper-coker is between 704_°C (1300_°F) and 871 _°C (1600_°F), and the coking temperature is comprised between 510_°C (950_°F) and 677_°C (1250_°F).

4. A process according to claim 3, wherein the ratio of solids to heavy hydrocarbon feed by weight in the coker is comprised between 5:1 and 60:1.

5. A process according to claim 2, wherein the heavy hydrocarbon is residual oil.

6. A process according to claim 2, wherein the heavy hydrocarbon is atmospheric-tower bottoms.

7. A process according to claim 2, wherein the light hydrocarbon feed and hot particulate solids are delivered to a tubular thermal regenerative cracking reaction through a reactor feeder having vertical passages communicating with the tubular regenerative cracking reactor and the solids in a hot solids vessel, means for providing localized fluidization to the solids above the vertical passages and means for delivering the light hydrocarbon fraction to the tubular thermal regenerative reactor at an angle to the path of the particulate solids entering the thermal regenerative reactor.

8. A process according to claim 1, wherein the hot particulate solids and the thermally cracked product gases are separated in a separator in which the particulate solids and the thermally cracked product gases enter the separator through a separator inlet and reverse their direction by 90_°, the cracked product gases reverse their direction by additional 90_° to effect a 180_°-reversal relative to the entry direction, the particulate solids continue in the path oriented 90_° relative to the particulate solids-cracked product gas separator inlet, whereafter the path of the particulate solids is directed downwards.

9. A process according to claim 1, wherein the particulate solids and cracked product gases are separated in a separator comprising a chamber for rapidly disengaging at least 80% of the particulate solids from the incoming mixed phase stream, said chamber having approximately rectilinear longitudinal side walls to form a flow path of rectangular cross-section having a height H and a width W, said chamber also having a mixed phase inlet of interior width Di, a gas outlet, and a solids outlet, said inlet being at one end of the chamber and arranged perpendicularly to the flow path, the height H of which is equal to at least Di, or 10,16 cm (4 inches), whichever is greater, and the width of which is no less than 0,75 D; but no more than than 1,25 Di, said solids outlet being at the opposite end of the chamber and being arranged for downflow of discharged solids by gravity, and said gas outlet being positioned therebetween at a distance no greater than 4Di from the inlet, as measured between respective centrelines, and oriented to effect a 180_° change in direction of the gas, whereby resultant centrifugal forces direct the solid particles into the incoming stream toward a wall of the chamber opposite to the inlet, forming thereat, and maintaining there, an essentially static bed of solids, the surface of the bed defining a curvilinear path of and arc of 90_° of a circle for the outflow of solids to the solids outlet.

10. A process according to claim 1, wherein the heavy hydrocarbon is separated into a light hydrocarbon fraction and a heavy hydrocarbon fraction by means of a vacuum fractionation column.