BRAKEGLEN LIMITED
  REFRACTORY CONSULTANTS

 

WHAT IS NOT ALWAYS KNOWN BY USERS

OF

CERAMIC FIBRE, INSULATING FIREBRICK &
HIGH EMISSIVITY COATINGS

 

This report endeavours to show that things are not always as they seem in the world of refractories. It is specific to ethylene furnaces but the comments will also have a bearing on other classes of high temperature process plant.

It submits that the move in recent years toward ceramic fibre linings is fundamentally wrong.

It explains why plants with brick linings frequently suffer high maintenance costs, and why casing plates often run significantly hotter than design.

It destroys a major myth which has inhibited technological advancement and clarifies some aspects of the use of high emissivity coatings.

It questions the reliability and accuracy of manufacturer's published data.

 

CERAMIC FIBRE:

Many new ethylene furnaces have been lined with ceramic fibre in recent years. Serious questions can be raised about the wisdom of this decision.

The main advantage of ceramic fibre to industry is it's low thermal mass characteristic.
This allows intermittent and batch type furnaces to operate on a reduced cycle time. Ethylene furnaces are continuously operated under steady state conditions and here the sole advantage of ceramic fibre is cost. Ceramic fibre linings are cheaper, quicker and easier to install (and repair) than brick. All else about use of the material is either questionable, a nonsense, or a danger.

A questionable advantage of ceramic fibre is that it is a better thermal insulator. Undoubtedly it is, but the benefit of reduced heat loss on a furnace which loses only 0.02 of total heat fired through the main fabric is at best marginal. Furthermore, one is asked to believe that heat saved at 90 deg C can be deducted from heat supplied at 1200 deg C.
The First Law of Thermodynamics allows this extravagance in heat balance calculations. The Second Law forbids it. A 10% reduction in radiant wall heat loss equates, at absolute best, to 0.0008 of fuel fired. Heat loss savings from improved insulation pass unnoticed at the gas meter.
 
Also questionable is the claim that less supporting steelwork is required with ceramic fibre. This is true in terms of subsidiary support steel but not necessarily true for the main structure. Wind load is an important, and sometimes dominating, stress factor. A 90% reduction in the weight of the internal lining system can occasion the need for more external bracing.

A nonsense claim is that ceramic fibre is unaffected by water. This is true in terms of chemistry but not true in terms of structural stability. Ceramic fibre will absorb water as a sponge. The density increase can, and has, torn complete fibre systems from their fixings. One must guard against significant amounts of water entering a furnace during overhauls.

Improved temperature uniformity is also a nonsense claim. It is only ever true when a new fibre system has replaced an old and battle weary brick lining. On a new for new comparison there is little difference. If anything, a brick's higher thermal mass and higher surface emissivity should give it the edge.

Low thermal mass brings us into the danger area. This characteristic of ceramic fibre is a potential hazard on ethylene furnaces. Rapid cool down following a trip can lead to thermal shock of the coils. The claim is that ceramic fibre is resistant to thermal shock. Rarely advertised is the fact that it can cause thermal shock elsewhere. Some ethylene plant operators have abandoned the use of ceramic fibre for this reason alone.

Another danger is increased fuel use and/or a fall-off in production. Ceramic fibre has the lowest emissivity of all the commercially available furnace lining materials. It causes a significant reduction in wall to coil radiation which in turn reduces overall firebox efficiency. The material should only ever be used as back-up insulation, for expansion joints, or for coil seals. Its use as the primary hotface lining material on ethylene furnaces is fundamentally wrong.

A word of caution to those plants already using ceramic fibre. Trying to increase wall to coil radiation by coating the ceramic fibre with a high emissivity coating is not without risk. Coated fibre will cool down about 10% faster than uncoated fibre in the event of a trip.

 

INSULATING FIREBRICK:

 
The vast majority of existing ethylene furnaces are lined with insulating firebrick. Insulating firebricks were first developed in the 1940's. Fifty years on there remain several important aspects of the brick which are not generally appreciated by users.
 
Insulating firebricks are manufactured by an extrusion process which gives a preferential bias to both the internal grain structure and the thermal conductivity. Thermal resistance varies with the construction orientation of a brick. Manufacturer's published data inevitably quotes k-values in the most favourable orientation ie, the brick built "stretcher" fashion (laid sideways on). Built "header" fashion (laid endways on), the construction orientation used on many ethylene furnaces, the thermal conductivity is about 8% higher than published data.

While the thermal conductivity of an insulating brick is more or less linear with temperature, the thermal gradient through the brick is not. The common practise is to only take the k-value at mean temperature into consideration. Simplifying the temperature gradient to a straight line then results in the tip temperatures of shelf plates and tie-back rods being understated.

Thermal conductivity is also affected by furnace atmosphere. Insulating firebricks are extremely porous and typically have an apparent porosity (connected open pore structure) of 70%. Reducing conditions are frequently experienced around burners and in the lower reaches of a radiant firebox. With the thermal conductivities of air, methane and hydrogen being 0.09, 0.29, and 0.61 W/mK respectively at 1200 deg C, the effect of a reducing atmosphere on thermal resistance is dramatic and self-evident. Note: Brick porosity has been quoted to illustrate the point but it is the permeability of the brick (not necessarily related to porosity and rarely published) that is the true measure of it's vulnerability in this situation.

The shrinkage resistance and hot strength characteristics of insulating firebrick also diminish rapidly in a reducing atmosphere.

The expansion of brickwork is often assumed to be uniform in all directions. This does not happen in practise. Bricks do not expand upward against gravity as much as they do sideways. Upward expansion is frequently only half that of sideways expansion. Also, published data on expansion is inevitably overstated as it is for the brick in a fully soaked temperature environment. The end result is usually excessive expansion allowance. While this may be seen as erring on the safe side, it is not conducive to a gas tight lining.
 
A misunderstanding often arises over brick selection due to the Classification Temperature system used for insulating firebrick. Published data typically states 2300 Grade, 2600 Grade (23 Grade and 26 Grade to ASTM C155), and so on. It is often assumed that these figures refer to the maximum or safe operating temperature in Fahrenheit. This is not the case. Historically the figures related to the temperature at which a brick would shrink by 1.5% under it's own weight. This criteria being a long assumed acceptable level for all industrial applications. Improvements in the manufacture of insulating firebrick over the years mean that the shrinkage figures are now considerably less but the Classification Temperatures remain and have no bearing on the safe working temperature.

A reduction occurs to the properties of refractories with time at temperature. Engineers are familiar with the creep phenomena of metals at temperature but far less so with the decline of refractory properties with time in service.

Disappointments with refractory life, high maintenance costs, and excessively hot casing plates can usually be traced to a lack of appreciation of some of the above mentioned points.

 

HIGH EMISSIVITY COATINGS:

 
The introduction mentioned destroying a major myth which has inhibited technological advancement and it relates to the use of high emissivity coatings.

Refractory linings have long been considered to be docile static structures with their primary function being to inhibit the escape of heat to atmosphere. This is a myth. The refractory walls in a radiant firebox are a dynamic entity. In reality a working component. They are akin to a large heat exchanger capturing heat before it escapes to the bridgewall area and radiating the heat so captured to the coils. Wall to coil radiation is the predominant mode of heat transfer in an ethylene furnace firebox.

This fact, and the scope it offers for improvements in radiant firebox efficiency, has passed largely unrecognised for decades. Text books are partly to blame and have no doubt misled the industry. Who would look for plant improvement from refractory emissivity enhancement when advised that, "Refractory bricks have an emissivity of 0.9", and "Furnace enclosures act as a black body"?

The end result is that the vast majority of ethylene furnaces, regardless of their assumed high overall thermal efficiency, are firing somewhere between 6% and 10% of fuel unnecessarily.

With the interest in high emissivity coatings now gathering pace some misunderstandings and misconceptions are already apparent.

The first concerns the colour of high emissivity coatings. Some vendors make a major selling point of having a black, or near black, coating and misuse the term "black body" coating. Visible colour is not the dominant factor in the infrared region of the spectrum. Strange things happen in the quantum world of electromagnetic radiation; some white radiator paints have a higher emissivity than black paint at room temperature and human skin has an emissivity of 0.9 in the infrared! The preoccupation with a visibly black coating has often led to the use of metallic oxide pigments in the formulation with their attendant health, safety, and final disposal risks.

It is also common practise for vendors to quote a blanket emissivity figure, such as 0.9, for a particular coating. Most refractory materials have an emissivity of about 0.9 at room temperature. At elevated temperature the emissivity becomes strongly wavelength dependent; varying accordingly and sometimes dramatically. On ethylene furnaces it is only the refractory emissivity in the 1.5 to 6 micron wavelength region of the infrared spectrum, and to a lesser extent in the 6 to 14 micron region, that has any real bearing on net heat transfer. Refractory emissivities quoted without reference to wavelength are not only misleading but meaningless.

Having said this, a serious problem arises in the measurement of emissivity at discrete wavelengths. No International Standards exist. There is no approved test apparatus and no approved test method. No guidance notes exist as to the correct interpretation of results. Test houses and authorities on the subject are often critical of each other's approach to measurement. As things stand today it is a minefield through which coating vendors are free to stroll without fear of explosion.

Another problem arises when trying to predict a change in heat balance from an increase in refractory emissivity. Most plant operators have access to a mathematical model of their furnaces. Aside from a handful of universities and research establishments, no models are programmed with the spectrally selective emission characteristics of hot gas and the dramatic change in refractory emissivity with wavelength. Consequently, the majority of mathematical models in present use cannot accept the phenomena at work let alone predict the outcome. This presents a problem for those who do not like to go where the computer cannot go.

A final word of caution. The technology may not be suitable for all plants. An increase in radiant firebox efficiency inevitably results in a reduced mass flow of cooler gases to the convection section. The use of a high emissivity coating may not be appropriate on plants which run lean on steam.

 

THERMOPHYSICAL PROPERTIES:

"The published data is typical and presented in good faith. It does not form a specification and no warranty is implied". These, or similar words, appear without exception on published data throughout the refractories and high temperature insulation industry. Why?

Refractory products, castables, bricks, cements, mortars, fibres, etc are manufactured for the most part from naturally occurring clays and minerals which are subject to considerable variation from country to country and quarry to quarry. Small variations, particularly with the unwanted inclusions, can have a marked effect on the final properties. The crushing, grinding, blending, mixing, pressing, drying, firing, and so on, all have a bearing on the final outcome. A not unreasonable comparison lay with baking a cake when the ingredients are subject to variation. The skill of the chef comes into play. Refractory manufacture is not all science. Some art is present. So is compromise. Rarely, if ever, can a given property be improved except at the direct expense of other properties.

So, with a variable product and unwarranted published data what tolerances should be applied to the figures which do appear in print?

Before trying to apply sensible percentages, consideration also has to be given to the accuracy and consistency of existing test methods. Surveys often show surprisingly large variations. A recent example is not unusual. Seven accredited test houses were sent a sample of 135kg/cu metre density mineral wool cut from the same "control" piece of board. The measurements for thermal conductivity gave a spread of +15% -15% about the average in the temperature range 100 to 500 deg C! Bear in mind that this is a relatively low temperature survey. The higher the temperature the more difficult the accurate measurement of conductivity becomes.

The problem is not limited to the measurement of thermal conductivity. It exists to some degree with all the thermophysical properties at high temperature - thermal diffusivity, permeability, refractoriness under load, crushing strength, modulus of rupture, reversible thermal expansion, permanent linear change, and so on.

Competitive pressures frequently force designers close to the line on safety margins. When the line is unwarranted and ill-defined then real dangers exist. For those who wish to sail in safer water and uphold high engineering standards, it is recommended that all published data on refractory materials, regardless of the particular property concerned, be subject to at least a 20% downward adjustment.

 

CONCLUDING COMMENT:

 
It is perhaps not by mere chance that the word "refractory" has a shared meaning with that which is perverse and unruly. Refractory technology certainly differs from other engineering disciplines in that it is not an exact science.

Engineers can design with confidence in steel. The application of reliable and consistent physical property data to established formula readily gives accurate values for stress, strain, sheer, deflection, creep, yield point, and so on. The refractory designer not only uses different language for the same phenomena but only has unwarranted property data to go on. Furthermore, the published data is rarely suitable for use in standard formula.

The shortfall in "science" with refractory technology can only be made up by experience and a sympathetic understanding of the materials concerned.

 

Copyright © John G Clements 1999

THE AUTHOR: John G Clements is Managing Director of Brakeglen Ltd (Refractory Consultants), Helston, Cornwall, England. His 40 years experience in the refractories industry includes 25 years with M H Detrick Company in the UK where he also served as Managing Director. Mr Clements is a Chartered Mechanical Enginneer, a member of the Institute of Energy, and a founder member of the Thermophysical Properties Awareness Club at the National Physical Laboratory.

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