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at 31815 K (45 C) The feedwater pump, which operates under exactly the conditions of the pump in Ex 710, causes a temperature rise of about 1 K (lnC),making the temperature of the feedwater entering the series of heaters equal to 31915 K (46 C) The saturation temperature of steam at the boiler pressure of 8600 kPa is 57321 K (30006"C), and the temperature to which the feedwater can be raised in the heaters is certainly less This temperature is a design variable, which is ultimately fixed by economic considerations However, a value must be chosen before any thermodynamic calculations can be made We have therefore arbitrarily specified a temperature of 49915 K (226 C) for the feedwater stream entering the boiler We have also specified that all four feedwater heaters accomplish the same temperature rise Thus, the total temperature rise of 49915 - 31915 = 180 K is divided into four 45 K (45 C) increments This establishes all intermediate feedwater temperatures at the values shown on Fig 85 The steam supplied to a given feedwater heater must be at a pressure high enough that its saturation temperature is above that of the feedwater stream leaving the heater We have here presumed a minimum temperature difference for heat transfer of no less than 5 K (5"C), and have chosen extraction steam pressures such that the TSat values shown in the feedwater heaters are at least 5 K (5 C) greater than the exit temperatures of the feedwater streams The condensate from each feedwater heater is flashed through a throttle valve to the heater at the next lower pressure, and the collected condensate in the final heater of the series is flashed into the condenser Thus, all condensate returns from the condenser to the boiler by way of the feedwater heaters.

For an almost-guaranteed kill of process number 593999, issue this command:

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of internal vibration The addition of heat to a substance increases this molecular activity, and thus causes an increase in its internal energy Work done on the substance can have the same effect, as was shown by Joule The internal energy of a substance also includes the potential energy resulting from intermolecular forces (Sec 161) On a submolecular scale energy is associated with the electrons and nuclei of atoms, and with bond energy resulting from the forces holding atoms together as molecules This form of energy is named internal to distinguish it from the kinetic and potential energy associated with a substance because of its macroscopic position or motion, which can be thought of as external forms of energy Internal energy, has no concise thermodynamic definition It is a thermodynamic primitive It cannot be directly measured; there are no internal-energy meters As a result, absolute values are unknown However, this is not a disadvantage in thermodynamic analysis, because only changes in internal energy are required

[root@fedora-serverA ~]# kill -9 593999

The recognition of heat and internal energy as forms of energy makes possible a generalization of the law of conservation of mechanical energy (Sec 18) to include heat and internal energy in addition to work and external potential and kinetic energy Indeed, the generalization can be extended to still other forms, such as surface energy, electrical energy, and magnetic energy This generalization was at first a postulate However, the overwhelming evidence accumulated over time has elevated it to the stature of a law of nature, known as the first law of thermodynamics One formal statement is:

Type the following to send the HUP signal to the init program (which is always PID 1):

Although energy assumes many forms, the total quantity of energy is constant, and when energy disappears in one form it appears simultaneously in other forms

[root@fedora-serverA ~]# kill - 1 1

In application of the first law to a given process, the sphere of influence of the process is divided into two parts, the system and its surroundings The region in which the process occurs is set apart as the system; everything with which the system interacts is the surroundings The system may be of any size depending on the application, and its boundaries may be real or imaginary, rigid or flexible Frequently a system consists of a single substance; in other cases it may be complex In any event, the equations of thermodynamics are written with reference to some well-defined system This focuses attention on the particular process of interest and on the equipment and material directly involved in the process However, the first law applies to the system and surroundings, and not to the system alone In its most basic form, the first law requires: A(Energy of the system)

TIP To get a listing of all the possible signals available, along with their numeric equivalents, issue the kill -l command!

+ A(Energy of surroundings) = 0

(21)

The following tools don t fall into any specific category we ve covered in this chapter, but they all make important contributions to daily system administration chores

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