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Heaters shift

Reducing gas is generated from natural gas in a conventional steam reformer. The natural gas is preheated, desulfurized, mixed with steam, further heated, and reformed in catalyst-filled reformer tubes at 760°C. The reformed gas is cooled to 350°C in a waste heat boiler, passed through a shift converter to increase the content, mixed with clean recycled top gas, heated to 830°C in an indirect-fired heater, then injected into reactor 4. [Pg.431]

But an ideological shift in Congress disrupted this process. In the 104th Congress, industrial opponents of appliance efficiency standards found sympathetic support, and passed a one-year moratorium on appliance efficiency standards in 1995. The moratorium held back DOE efforts on appliance standards for nearly two years. The refrigerator standard that was to be issued early in 1995 was delayed until 1997, and the effectiveness date set hack three years until 2001. Progress toward new standards on ballasts, water heaters, air conditioners, clothes washers, and other products was delayed. [Pg.80]

The thermal inertia of the wall is negligible, i.e., we assumed no phase shift between temperature of the channel wall and the heater. [Pg.282]

The simplest and, despite its several drawbacks, the most widely used type of control is the on/off control system. An example is a contact thermometer, which closes or opens a heater circuit. The designation on/off means that the controller output, or the manipulated variable (electric current) is either fully on or completely off. To avoid oscillations around the setpoint, the real on/off controller has built into it, a small interval on either side of the setpoint, within which the controller does not respond, and which is called the differential gap or deadzone. When the controlled variable moves outside the deadzone, the manipulated variable is set either on or off. This is illustrated in Fig. 2.30. Such shifts from the set point are known as offset. [Pg.96]

Table II shows the nominal alpha dose factors for occupational mining exposure. Table III shows the alpha dose factors for the nominal environmental situation. Table IV shows the bronchial dose factors for the smallest sized particles, that dominated by the kerosene heater or 0.03 pm. particles. The radon daughter equilibrium was shifted to a somewhat higher value in this calculation because this source of particles generally elevates the particle concentration markedly with consequent increase in the daughter equilibrium. Table V shows the alpha dose for a 0.12 pm particle, the same as the nominal indoor aerosol particle, but for a particle which is assumed to be hygroscopic and grows by a factor of 4, to 0.5 pm, once in the bronchial tree. Table II shows the nominal alpha dose factors for occupational mining exposure. Table III shows the alpha dose factors for the nominal environmental situation. Table IV shows the bronchial dose factors for the smallest sized particles, that dominated by the kerosene heater or 0.03 pm. particles. The radon daughter equilibrium was shifted to a somewhat higher value in this calculation because this source of particles generally elevates the particle concentration markedly with consequent increase in the daughter equilibrium. Table V shows the alpha dose for a 0.12 pm particle, the same as the nominal indoor aerosol particle, but for a particle which is assumed to be hygroscopic and grows by a factor of 4, to 0.5 pm, once in the bronchial tree.
Just for start up, there are electric gas heaters before the shift, the desulfurization and the synthesis units during normal operation, these heaters are not used. [Pg.49]

Rule 2. Shift heaters or coolers to approach a practical minimum loss in available energy during heat exchange ... [Pg.165]

BODM No. 1 (Figure 1). This modification illustrates the use of Rule 2a to guide the shift of a heater on a given cold process stream. The evolutionary changes shown in Figure 1 are as follows (a) On S, shift H1 to the high-temperature portion, and (b) shift downward on S to a position... [Pg.166]

Arcs can be considered as gaseous resistance heaters and offer temperatures up to 50,000°K. The sustained temperatures realizable from electric arcs can be divided into three general regions according to the current density of the conducting path. The lower temperatures (up to 4000°K. and a current density of 60 amp./cm.2) make the anode material incandescent, but as the current density is increased beyond a critical level the voltage drop shifts suddenly from a uniform drop between cathode and anode to a drop concentrated at the anode surface (for a dc arc—at both electrodes for an ac arc). The transition from the conventional to a high intensity arc is marked by pronounced increases in brilliance and temperature the arc path becomes distorted, and a jet of plasma, called the tail flame, issues from the rapidly... [Pg.98]


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