Package: Loose Leaf For Numerical Methods For Engineers With 1 Semester Connect Access Card
Package: Loose Leaf For Numerical Methods For Engineers With 1 Semester Connect Access Card
7th Edition
ISBN: 9781259289163
Author: Steven C. Chapra Dr., Raymond P. Canale
Publisher: McGraw-Hill Education
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Chapter 28, Problem 16P

Bacteria growing in a batch reactor utilize a soluble food source (substrate) as depictedin Fig.P28.16. The up take of the substrate is represented by a logistic model with Michaelis-Menten limitation. Death of the bacteria produces detritus which is subsequently converted to the substrate by hydrolysis. In addition, the bacteria also excrete some substrate directly. Death, hydrolysis, and excretion are all simulated as first-order reactions. Mass balances can be written as

d X d t = μ max ( 1 X K ) ( S K s + S ) X k d X k e X d C d t = k d X k h C d S d t = k e X + k h C μ max ( 1 X K ) ( S K s + S ) X

where X, C and S = the concentrations ( mg / L ) of bacteria, detritus, and substrate, respectively; μ max = maximum growth rate ( / d ) , K = the logistic carrying capacity ( mg/L ) ; K s = the Michaelis-Menten half-saturation constant ( mg / L ) , k d = death rate  ( / d ) ; k e = excretion rate  ( /d ) and  k h = hydrolysis rate  ( /d ) . Simulate the concentrations from t = 0 to 100 given the initial conditions X ( 0 ) = 1 mg / L,  S ( 0 ) = 100 mg/L,  and  C ( 0 ) = 0  mg/L Employ the following parameters in your calculation: μ max = 10 /d, K = 10  mg/L,  k d = 0  1/d,  k e = 0 ,  1/d, and  k h = 0.  1/d .

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Chapter 28 Solutions

Package: Loose Leaf For Numerical Methods For Engineers With 1 Semester Connect Access Card

Ch. 28 - An on is other malbatchre actor can be described...Ch. 28 - The following system is a classic example of stiff...Ch. 28 - 28.13 A biofilm with a thickness grows on the...Ch. 28 - 28.14 The following differential equation...Ch. 28 - Prob. 15PCh. 28 - 28.16 Bacteria growing in a batch reactor utilize...Ch. 28 - 28.17 Perform the same computation for the...Ch. 28 - Perform the same computation for the Lorenz...Ch. 28 - The following equation can be used to model the...Ch. 28 - Perform the same computation as in Prob. 28.19,...Ch. 28 - 28.21 An environmental engineer is interested in...Ch. 28 - 28.22 Population-growth dynamics are important in...Ch. 28 - 28.23 Although the model in Prob. 28.22 works...Ch. 28 - 28.25 A cable is hanging from two supports at A...Ch. 28 - 28.26 The basic differential equation of the...Ch. 28 - 28.27 The basic differential equation of the...Ch. 28 - A pond drains through a pipe, as shown in Fig....Ch. 28 - 28.29 Engineers and scientists use mass-spring...Ch. 28 - Under a number of simplifying assumptions, the...Ch. 28 - 28.31 In Prob. 28.30, a linearized groundwater...Ch. 28 - The Lotka-Volterra equations described in Sec....Ch. 28 - The growth of floating, unicellular algae below a...Ch. 28 - 28.34 The following ODEs have been proposed as a...Ch. 28 - 28.35 Perform the same computation as in the first...Ch. 28 - Solve the ODE in the first part of Sec. 8.3 from...Ch. 28 - 28.37 For a simple RL circuit, Kirchhoff’s voltage...Ch. 28 - In contrast to Prob. 28.37, real resistors may not...Ch. 28 - 28.39 Develop an eigenvalue problem for an LC...Ch. 28 - 28.40 Just as Fourier’s law and the heat balance...Ch. 28 - 28.41 Perform the same computation as in Sec....Ch. 28 - 28.42 The rate of cooling of a body can be...Ch. 28 - The rate of heat flow (conduction) between two...Ch. 28 - Repeat the falling parachutist problem (Example...Ch. 28 - 28.45 Suppose that, after falling for 13 s, the...Ch. 28 - 28.46 The following ordinary differential equation...Ch. 28 - 28.47 A forced damped spring-mass system (Fig....Ch. 28 - 28.48 The temperature distribution in a tapered...Ch. 28 - 28.49 The dynamics of a forced spring-mass-damper...Ch. 28 - The differential equation for the velocity of a...Ch. 28 - 28.51 Two masses are attached to a wall by linear...
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