Transcript Slide 1

LINEAR SECOND ORDER
ORDINARY DIFFERENTIAL
EQUATIONS
The general form of the equation:
d2y
dy
P ( x ) 2  Q( x )  R ( x ) y  G ( x )
dx
dx
where P, Q, R, and G are given functions
Samples of 2nd order ODE:
Legendre’s equation
(1  x 2 ) y' '2 xy' (  1) y  0
Bessel’s equation
x 2 y' ' xy'( x 2  n2 ) y  0
Hypergeometric equation
d2y
dy
x 2  (c  x)  ay  0
dx
dx
When function g(x) is set to zero:
2
d y
dy
 p ( x)  q ( x) y  0
2
dx
dx
This is the homogeneous form of 2nd order ODE
Suppose p and q in eqn above are continuous on a<x<b
then for any twice differentiable function f on a<x<b, the
linear differential operator L is defined as:
L[f] = f” + pf’ +qf
L[y] = y” + p(x)y’ + q(x)y = 0
Solutions of Homogeneous Equation
Theorem
If y = y1(x) and y = y2(x) are solutions of the differential
equation
L[y] = y” + p(x)y’ + q(x)y = 0
then the linear combination of y = c1y1 (x) + c2y2 (x), with
c1 and c2 being arbitrary constants is also a solution.
Application of 2nd Order ODE
Two concentric cylindrical metallic shells are separated
by a solid material. If the two metal surfaces are
maintained at different constant temperatures, what is
the steady state temperature distribution within the
separating material?
r + Dr
r
a
R
Solution
Sample of Transport Model (1)
Consider the axial flow of an incompressible fluid in a
circular tube of radius R. By considering long tube
and assuming q-component and r-component of
velocities are negligible, one can reduce the zcomponent for constant r and m
 1   vz   2vz 
 z
P
rz

 m
r
 2 
z
z
 r r  r  z 
Equation of continuity reduces to:
vz
0
z
Sample of Transport Model (2)
Derive the temperature profile T, in a solid cylinder
with heat generation if the governing differential
equation is
1   T  1   T    T  .
T
 k
   k
 kr
 2
  q  rC p
r r  r  r f  f  z  z 
t
where the coordinate system indicates the
independent variables: r is the mass density and Cp
the specific heat.
Example 1
Consider a long solid tube, insulated at the outer
radius ro and cooled at the inner radius ri with uniform
heat generation q within the solid.
a)
b)
c)
d)
Determine the general solution for the temperature profile in
the tube
Suppose the maximum permissible temperature at the
insulated surface ro is To. Identify appropriate boundary
conditions that could be used to determine the arbitrary
constants appearing in the general solution and find the
temperature distribution.
What is the heat of removal rate per unit length of tube?
If the coolant is available at a temperature T, obtain an
expression for the convection coefficient that would have to be
maintained at the inner surface to allow for operation at the
prescribed values of To and q.
ri
Assumptions:
1. Steady state conditions
2. One dimensional radial conduction
3. Physical properties are constant
4. Volumetric heat generation is constant
5. Outer surface is adiabatic
Example 2
A tubular reactor of length L and cross-sectional area 1.0
m2 is used to carry out a first order chemical reaction of
the type
AB
The rate coefficient is k (sec-1). In a given feed rate of u
m3/sec, the initial feed concentration of species A is Co
and the diffusivity of A is D m2/sec. What is the
concentration of A as a function of the reactor length? It
may be assumed that during the reaction the volume
remains constant and that steady-state conditions are
established. Also there is no concentration variation in
the section following the reactor.
Example 3
Two thin wall metal pieces of 1” outside diameter
are connected by ½” thick and 4” diameter
flanges that are carrying steam at 250oF.
Determine the rate of heat loss from the pipe
and the proportion that leaves the rim of the
flange.
Thermal conductivity of the flange metal is k=220 Btu/h
ft2oF ft-1
The exposed surfaces of the flanges lose heat to the
surroundings at T1 = 60oF according to heat transfer
coefficient h = 2 Btu/h ft2oF
Pipe Flange
r + Dr
r
2 in
½ in