 
          
            36
          
        
        
          December
        
        
          2014
        
        
          HYDROCARBON
        
        
          ENGINEERING
        
        
          containing catalytic cracking catalyst, which circulates
        
        
          continuously from one vessel to the other through a set of
        
        
          transfer lines. Those vessels are referred to as the reactor and
        
        
          regenerator. The desired reaction occurs in the reactor, and over
        
        
          time the surface of the catalyst particles is coated with coke, a
        
        
          condensed hydrocarbon. Coke reduces the activity of the
        
        
          catalyst and makes it necessary to continually remove
        
        
          deactivated, or spent, catalyst to the regenerator, where the
        
        
          coke is burned off in what is a very exothermic process. Once
        
        
          the catalyst is cleaned, or regenerated, it is returned to the
        
        
          reactor. This loop constitutes a continuous process that must
        
        
          run every day, year after year, to yield maximum benefit.
        
        
          FCC catalysts are typically microporous aluminosilicate
        
        
          materials, and in a fluidised state, they can be quite abrasive.
        
        
          Add to that high temperature and pressure, the presence of
        
        
          steam, and a host of metallic and nonmetallic impurities, and
        
        
          what one is faced with is an extremely difficult environment.
        
        
          
            The impact of abrasive wear
          
        
        
          The fluidised bed in the regenerator is maintained through the
        
        
          use of compressed air, fed through a large number of nozzles
        
        
          situated in one of a number of proprietary configurations. The
        
        
          key element to performance in the regenerator is consistency,
        
        
          and a uniform fluidisation must be maintained for maximum
        
        
          regenerating efficiency.  The size and shape of the orifices of the
        
        
          air grid nozzles are critical to maintaining this uniformity.  Any
        
        
          abrasion to the nozzle has the potential to significantly impact
        
        
          the geometry of the individual nozzle, and with enough damage,
        
        
          eventually the overall performance of the regenerator.
        
        
          When a grid nozzle wears, the shape of the flow path
        
        
          through the nozzle changes, resulting in an alteration in the air
        
        
          flow rate of the nozzle and, potentially, the flow pattern, as the
        
        
          air flows into the bed. Distribute these changes in varying
        
        
          magnitudes across the complete air grid and the resultant
        
        
          variability in fluidisation and combustion can result in serious
        
        
          performance issues. Catalyst regeneration rates can suffer and
        
        
          reaction chemistry can change driving up catalyst deactivation
        
        
          rates. Temperature distribution within the bed can change
        
        
          from optimum design conditions resulting in unexpected
        
        
          consequences such as HCN generation rates high enough to
        
        
          carry through to flue gas discharge.  The value of abrasive
        
        
          wear resistance in FCCU air grid nozzles as it impacts process
        
        
          consistency is significant.
        
        
          
            Abrasion and metals
          
        
        
          There are a number of different engineering strategies for
        
        
          dealing with abrasive wear, but with regard to material
        
        
          selection the generally accepted rule is the harder, the
        
        
          better.
        
        
          This premise can be a little tricky when it comes to metals
        
        
          where in many cases resistance to abrasion is more heavily
        
        
          influenced by specific constituents in alloyed compositions,
        
        
          exhibiting higher individual hardness compared to the overall
        
        
          average macrohardness of the composition. This characteristic
        
        
          peak microhardness forms a basis for understanding abrasion
        
        
          resistance in metals. Regardless, whether pure metal or alloy,
        
        
          metallic compounds, as a class, are less hard than ceramic, and
        
        
          because they deform under tensile stress (due to the elastic
        
        
          nature of metallic bonds
        
        
          1
        
        
          ) they are considered to be ductile
        
        
          bodies; they deform, rather than fracture. Because they are
        
        
          relatively soft as well as ductile, metallic material can be
        
        
          displaced by erosive particles as they move across the surface.
        
        
          2
        
        
          This scouring effect continues for the length of the contact
        
        
          between the erosive particle and the metal compound. Ergo,
        
        
          the more acute the angle of impact, the longer the contact
        
        
          path, and the greater the abrasive wear. The greater the angle,
        
        
          the less total surface area is exposed to the effect of the
        
        
          erosive particle and the less displacement occurs.
        
        
          Consequently, metals wear faster at acute angles of impact
        
        
          than at angles closer to 90˚. Further, metals begin to soften at
        
        
          temperatures much lower than ceramic, and any excursions
        
        
          can fatally undermine the material properties.
        
        
          
            Abrasion and ceramics
          
        
        
          Ceramics simply are harder, and this helps explain why more
        
        
          often than not ceramic materials exhibit significant
        
        
          advantages in wear applications. Ceramic materials,
        
        
          surprisingly to some, share an important similarity to the
        
        
          metallic compounds described above. They can be made
        
        
          from a single ceramic constituent, or they may be ‘alloyed’ if
        
        
          you will; made of multiple ceramic compounds. These
        
        
          ceramic compounds do differ in one key way from metallic
        
        
          alloys, the bond phase.
        
        
          There are a number of grades of ceramic materials,
        
        
          including structural, technical, refractory, and white ware.
        
        
          Technical ceramics include tiles used in the Space
        
        
          Shuttle program, gas burner nozzles, ballistic protection,
        
        
          biomedical implants, jet engine turbine blades and missile
        
        
          nose cones.  Refractory ceramics include such things as kiln
        
        
          linings, steel and glass making crucibles, and various
        
        
          monolithic, or unformed, compositions used in the
        
        
          petrochemical industry.
        
        
          When one thinks of hard, abrasion resistant ceramic
        
        
          materials, one is generally thinking of a technical ceramic,
        
        
          with a fine grained, fully dense, sintered body. This is
        
        
          analogous to the pure metallic composition described above.
        
        
          The hardness of the single constituent dictates the abrasion
        
        
          
            Figure 1.
          
        
        
          Erosion resistance of ductile versus
        
        
          brittle materials.
        
        
          3
        
        
          off the harder ceramic particles. As the angle of impact approaches 90 degrees, erosive particles can
        
        
          hammer away at the typically softer bond phase, and begin displacing harder ceramic particles that way.
        
        
          It is worth noting that the angle of incidence between erosive particles and the exposed surface of the
        
        
          nozzles is generally acute, as the flow of air and particles swirls across the tips of the nozzles.
        
        
          Figure 1. Erosion Resistance of Ductile vs. Brittle Materials
        
        
          3
        
        
          It wasn’t until the late 1980’s that a few plants started using ceramic for the air grid nozzles. They saw
        
        
          the benefit of the monolithic castable materials used in areas covering the grid and in the cyclone.
        
        
          Requirements for length of campaigns have been increasing, along with temperatures and pressures,
        
        
          and it became imperative to find a material that would be up to the task. Over the last 20+ years a wide
        
        
          variety of alloys, weld overlays, and ceramic materials have been tried in grid nozzles, with varying
        
        
          results. The bulk of the ceramic materials have been fully dense technical ceramics, selected purely for
        
        
          their abrasion resistanc . N t surprisingly, most of these suffered from early failure du to thermal
        
        
          shock.
        
        
          3
        
        
          COMPUTATIONAL MODEL OF DUCTILE EROSION BY SINGLE PARTICLE IMPACT, Chandrakant Rai, West Virginia
        
        
          University, Morgant wn, WV, 2000
        
        
          Erosion in g/g ( x 10 ) [Ductile]
        
        
          Ductile Material
        
        
          Brittle Material
        
        
          Angle of Attack in degrees
        
        
          Erosion in g/g ( x 10 ) [Brittle]