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Also consult the cumnt chemistry literature for the appropriate algebraic form of the rate law for a given reaction. For example, check the Journal of Physical

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Chemistry in addition to the journals listed in Section 4 of the Supplementary Reading section in Chapter 4.

W. A. Benjamin, 1969, Chaps. 4 and 5.

Wiley, 1981, Chaps. 4 and 5.

Hill, 1960.

ics, Prentice Hall, New Jersey: 1989.

h o t hermal Reactor Design

4

Why, a four-year-old child could understand this.

Someone get me a four-year-old child.

Grouch0 Marx

Tying everything together

In this chapter we bring all the material in the preceding three chapters together to arrive at a logical structure for the design of various types of ireac- tors. By using this structure, one should be able to solve reactor engineering problems through reasoning rather than memorization of numerous equarions together with the various restrictions and conditions under which each equa- tion applies (Le., whether there is a change in the total number of moles, etc.).

In perhaps no other area of engineering is mere formula plugging more hazard- ous; the number of physical situations that can arise appears infinite, and the chances of a simple formula being sufficient for the adeqhate design of a real reactor are vanishingly small.

This chapter focuses attention on reactors that are operated isothermally.

We begin by studying a liquid-phase batch reactor to determine the specific reaction rate constant needed for the design of a CSTR. After illustrating the design of a CSTR from batch reaction rate data, we carry out the design of a tubular reactor for a gas-phase pyrolysis reaction. This is followed by a discus- sion of pressure drop in packed-bed reactors, equilibrium conversion, and finally, the principles of unsteady operation and semibatch reactors.

4.1 Design

Structure for Isothermal Reactors

The following procedure is presented as a pathway for one to follow in the design of isothermal (and in some cases nonisothermal) reactors. It is the author’s experience that following this structure, shown in Figure 4-1, will lead to a greater understanding of isothermal reactor design. We begin by applying

125

126 isothermal Reactor Design Chap. 4

0

balance equation :

mA

FAo

- FA +/"rA d v =

-

dt

1

@

Design Equations: -i

Batch:

N

dx=

- rAV and t = N../xz

-

rAv

dt 0

FAO X V =

Evaluate the algebraic (CSTR) or integral

to determine &?e reactor volume or the processing [@Determine the rate law in terns of the

concentration of the reacting species

function of conversion.

Gas Phase:

CA = C A ~

-

(1 +EX)

€IB=

-

YBO

E = Y A 0 8 L yAO

Figure 4-1 Isothermal reaction design algorithm

Sec. 4.1 Design Structure for Isothermal Reactors 127

our general mole balance equation (level 1) to a specific reactor to arrive at the design equation for that reactor (level 2). If the feeld conditions are specified (e.g., NAo or FA0). all that is required to evaluate the (design equation is the rate of reaction as a fuinction of conversion at the same conditions as those at which the reactor is to be operated (e.g., temperature and pressure). When - r A = f ( X ) is given, one can go directly from level 3 to level 7 to determine either the

time or reactor volume necessary to achieve the specified conversion.

If the rate of reaction is not given explibitly as a function of conversion, the rate law must be determined (level 4) by either finding it in books or jour- nals or by deterimining it experimentally in the laboratory. Techniques for obtaining and analyzing rate data to determine the reaction order and rate con- stant are presented in Chapter 5. After the rate law has been established, one has only to use stoichiometry (level 5) together with the conditions of the sys- tem (e.g., constant volume, temperature) to express concentration as a function of conversion. By combining the information in levels 4 and 5 , one can express the rate of reaction as a function of conversion and arrive at level 6. It is now possible to determine either the time or reactor volume necessary to achieve the desired conversion by substituting the relationship relating conversion and rate of reaction into the appropriate design equation. The design equation is then evaluated in the appropriate manner (Le., analytically using a table of integrals, or numerically using an ODE solver). Although this structure empha- sizes the determination of a reaction time or volume For a specified conversion, it can also readily be w e d for other types of reactor calculations, such as deler- mining the conversion for a specified volume. Different manipulations can be performed in level 7 to answer the types of questions mentioned here.

The structure shown in Figure 4-1 allows one to develop a few basic con- cepts and then to arrange the parameters (equations) associated with each con- cept in a variety of ways. Without such a structure, one is faced with the possibiliity of choosing or perhaps memorizing the correct equation from a multitude of equations that can arise for a variety of different reactions, reac- tors, and sets of conditions. The challenge is to put everything together in an orderly and logical fashion so that we can proceed to arrive at the correct equa- tion for a given situation.

Fortunately, by using an algorithm to formulate CRE problems, which happens to be analogous to ordering dinner from a fixed-price menu in a fine French restaurant, we can eliminate virtually all memorization. In both of these algorithms we must make choices in each category. For example, in orderling from a French menu, we begin by choosing one dish from the appetiz,ers listed. Step 1 in the analog in CRE is to begin by choosing the mole balance for one of the three types of reactors shown. In step 2 we choose the rate law (eiztre'e), and in step 3 we specify whether the reaction is gas or liquid phase (cheese or dessen). Finally, in step 4 we combine steps 1, 2, and 3 and obtain an analytical solution or solve the equations using an ordinary differential equation (ODE) solver. (See complete French menu on the CD-ROM)

We now will apply this algorithm to a specific situation. The first step is to derive or apply the mole balance equation for the system at hand. Suppose that we have, as shown in Figure 4-2, mole balances for three reactors, three

Use the algorithm rather than

memorizing

equations

French Menu Analogy

128 Isothermal Reactor Design Chap. 4

~~

1. MOLE BALANCES

2. RATE LAWS

>

...I..._

-

FA=Fp,O(l - X ) NA = NAO (1 - X)

p....*

LIQUID IDEAL GAS IDEAL GAS LIQUID OR GAS

Constant flow rate Variable flow rate Variable volume Constant volume

,....\

v =vo

4. COMBINE (First Order Gas-Phase Reaction in a PFR)

1

From mole balance

I

. From stoichiometry

Integrating for the case of constant temperature and pressure gives

Figure 4-2 Algorithm for isothermal reactors.

Sec. 4.2 Scale-Llp of Liquid-Phase Batch Reactor Data to the Design of a CSTR 129

We can solve the equa- tions in the combine step either

1) Analytically (Ap-

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