A completely enclosed stirred-tank heating process is used | StudySoup

Textbook Solutions for Process Dynamics and Control

Chapter 2 Problem 2.2

Question

A completely enclosed stirred-tank heating process is used to heat an incoming stream whose flow rate varies.

The heating rate from this coil and the volume are both constant.

(a) Develop a mathematical model (differential and algebraic equations) that describes the exit temperature if heat losses to the ambient occur and if the ambient temperature (\(T_a\)) and the incoming stream's temperature (\(T_i\)) both can vary.

(b) Discuss qualitatively what you expect to happen as \(T_i\) and w increase (or decrease). Justify by reference to your model.

Notes:

\(\rho\) and \(C_p\) are constants.

\(U\), the overall heat transfer coefficient, is constant.

\(A_s\) is the surface area for heat losses to ambient.

\(T_i > T_a\) (inlet temperature is higher than ambient temperature).

Solution

Step 1 of 2

(a)

The energy balance can be written as,

\(\frac{d U_{\text {int }}}{d t}=-\Delta(w \widehat{H})+Q \cdots \ldots \ldots(1)\)

where \(U_{i n t}\) is the internal energy of the system, \(\widehat{H}\) is the enthalpy per unit mass, w is the mass flow rate, and Q is the rate of heat transfer to the system.

The \(\Delta\) operator denotes the difference between outlet conditions and inlet conditions of the flowing streams.

Consequently, the \(-\Delta(w \widehat{H})\) term represents the enthalpy of the inlet stream(s) minus the enthalpy of the outlet stream(s).

The liquid inlet stream consists of a single component with a mass flow rate \(w_{i}\) and an inlet temperature \(T_{i}\).

The tank contents are agitated and heated using an electrical heater that provides a heating rate,

Q.

A dynamic model will be developed based on the following assumptions:

  1. Perfect mixing; thus, the exit temperature T is also the temperature of the tank contents.
  2. The inlet and outlet flow rates are equal; thus, \(w_{i}=w\) and the liquid holdup V is constant.
  3. The density \(\rho\) and heat capacity C of the liquid are assumed to be constant. Thus, their temperature dependence is neglected.
  4. Heat losses are negligible.

After simplifying the general energy balance in equation (1), we can write the following expression which gives the desired dynamic model of the stirred-tank heating system.

\(C_{p} \frac{d\left[\rho V\left(T-T_{r e f}\right)\right]}{d t}=w C_{p}\left(T_{i}-T_{r e f}\right)-w C_{p}\left(T-T_{r e f}\right)-U A_{s}\left(T-T_{a}\right)+Q\)

On simplifying,

\(\begin{array}{l}
\rho V C_{p} \frac{d T}{d t}=w C_{p}\left(T_{i}\right)-w C_{p}(T)-U A_{s}\left(T-T_{a}\right)+Q \\
\rho V C_{p} \frac{d T}{d t}=w C_{p}\left(T_{i}-T\right)-U A_{s}\left(T-T_{a}\right)+Q
\end{array}\)

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full solution

Title Process Dynamics and Control 3 
Author Dale E. Seborg
ISBN 9780470128671

A completely enclosed stirred-tank heating process is used

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