13-42 The Civil Engineering Handbook, Second Edition
Operation of a rotary kiln incinerator involves several concerns. The first concern is the seals at the
front and rear ends. As can be seen in Fig. 13.5, the rotating kiln must slide past the fixed wall at the
front, where the waste feed and burner nozzles are, and at the rear by the ash drop and combustion gas
exhaust. There is no practical way to seal a rotary kiln to withstand positive pressure at the points where
the rotating equipment meets the stationary components. As a result, a rotary kiln is operated under
negative pressure. The system is designed to draw air at a specified maximum rate through the seals and
other openings. If the seals become worn or damaged, the air infiltration can become excessive, and the
incinerator will have trouble maintaining temperature at an acceptable gas flow rate. A properly operating
incinerator must include routine inspections and a regular maintenance program of the seals.
A second potential problem that is of particular concern with rotary kiln incinerators is that of
“puffing.” Normally, the gases leaving the kiln are “pulled” into the secondary combustion chamber by
the pressure differential between the two. If there is a sudden increase in the gas production rate in the
kiln (due to sudden explosion, combustion, or volatilization of a chunk of waste, for example) or a draft
decrease in the secondary combustion chamber (due, for example, to a problem with the fan), the gas
flow rate may exceed the capacity of the downstream equipment, and an over-pressure could result. Flue
gas from the kiln, potentially containing unburned POHCs and PICs, could thus be released as a “puff”
from the rotating juncture between the kiln and the secondary combustion chamber. Normally, the seals
can contain the gas from a specified level of overpressure. When the level is exceeded or the seals are
damaged or worn, however, puffing could occur.
This problem is of special concern in incinerators burning munitions or other explosive wastes. In
these cases, puffing could occur when a shell or piece of explosive detonates suddenly. These incinerators
are designed to withstand explosions, but puffing can frequently occur then. The burning of drummed
wastes can also lead to puffing. In this case, if the contents of a drum burn rapidly, the effect could be
similar (although usually not as severe) to an explosion, as discussed above. The resultant overpressure
could produce puffing. When puffing may occur, incinerators are equipped with an “emergency vent
stack,” water column, or other emergency relief vents.
The length-to-diameter ratios of rotary kilns can range from 2 to 10. Outside shell diameters are
generally limited to less than 15 ft to allow shipping of the cylinder sections. Rotational speeds of the
kiln are usually measured as a linear velocity at the shell. Typical values are on the order of 0.2 to 1 in./sec.
Te mperatures for burning vary between 800 to 1600°C (1500 to 3000°F). Bulk gas residence times in the
kiln are generally maintained at 2 sec or higher.
The solids retention time in a rotary kiln is a function of the length-to-diameter ratio of the kiln, the
slope of the kiln, and its rotational velocity. The functional relationship between these variables is given
by the following rough approximation (Bonner, 1981):
(13.13)
where t
solids
is the retention time (in min), L is the length of the kiln (in ft), D is the diameter of the kiln
(in ft), S is the slope of the kiln (in ft/ft), and N is the revolutions per minute (rpm). Typical ranges of
these parameters are L/D: 2–10, S: 0.03–0.09 ft/ft, and rotational speed 1 to 5 ft/min (which can be
converted to rpm by dividing by the kiln circumference measured in ft). The retention time requirements
for burnout of any particular solid waste should be determined experimentally or extrapolated from
operating experience with similar wastes. In a movable grate furnace, the retention time is given by the
ratio of the length of the grate, L, and its speed, S.
Air/solids mixing in the kiln is primarily a function of the kiln’s rotational velocity, assuming a relatively
constant gas flow rate. As rotational velocity is increased, the solids are carried higher along the kiln wall
and showered down through the air/combustion gas mixture. Because solids retention time is also affected
by rotational velocity, there is a tradeoff between retention time and air/solids mixing. Mixing is improved
to a point by increased rotational velocity, but the solids retention time is also reduced. Mixing is also
improved by increasing the excess air rate, but this reduces the operating temperature. Thus, there is a
tradeoff between gas and solids retention time and mixing.
tLDSN
solids
=
()
019.