MA2051 - Ordinary Differential Equations
Test 1 Solutions - A96




1
A
rV l/min
B
H l/min
C
The change in the amount of water in the tank from t to is the amount added over less the amount lost. Change over . Amount added . Amount lost . Conservation requires

Divide by , take the limit as tex2html_wrap_inline66 to obtain dV/dt = -rV + H. (Not required: for a complete model, add the initial condition tex2html_wrap_inline70 .)

D
tex2html_wrap_inline72 constant yields tex2html_wrap_inline74 . Hence, there is a single steady state tex2html_wrap_inline76 .

Since tex2html_wrap_inline78 , this steady state represents a balance between leakage at the rate tex2html_wrap_inline80 l/min and additions at the rate H l/min.

E
One stability argument: study solutions of the form V(t) = H/r + p(t), where p is small initially. Substituting in V' = -rV + H and simplifying yields p' = -rp. Since tex2html_wrap_inline92 , the perturbation p decays and tex2html_wrap_inline76 is stable.

Another argument: Using characteristic equations and undetermined coefficients, the general solution of V' = -rV + H is tex2html_wrap_inline100 . The arbitrary constant C is determined by the initial condition. Hence, regardless of the initial state, every solution of V' = -rV + H decays to tex2html_wrap_inline106 .


2
Since the DE is linear, use tex2html_wrap_inline108 . To find tex2html_wrap_inline110 , solve u' - 2u = 0 via characteristic equations: substituting tex2html_wrap_inline114 yields r = 2 and tex2html_wrap_inline118 .

To find tex2html_wrap_inline120 , use undetermined coefficients to guess tex2html_wrap_inline122 . But tex2html_wrap_inline124 solves the homogeneous equation. So revise guess to tex2html_wrap_inline126 . Substitution yields A = 4.

Hence, tex2html_wrap_inline130 . The initial condition u(0) = 3 forces C = 3. The solution of the IVP is tex2html_wrap_inline136 .


3
At t = 0, tex2html_wrap_inline140 . Hence, curves B-D are excluded; they have zero or negative slope at t = 0. Since y'' = dy'/dt = 4y' - 2y y' = (4 - 2y)y', tex2html_wrap_inline146 ; the solution curve is concave up at t = 0. Hence, curve A is a plausible graph of the solution of this IVP.

  

© 1996 by
Will Brother. All rights Reserved. File last modified on September 18, 1996.