Calculus Lecture - Ch 9
9.1 First-Order Differential Equations and Applications
State the order of a DE: first page of lesson
Confirm a given solution to a given DE: by substitution:
Def: Solution to a DE is a function (not a numerical value) that makes the DE true
To test a proposed solution, calculate the required derivatives and plug into the DE
Ex: verify that y = 4cos(3t) - 5sin(3t) is a solution of the 2nd order DE y'' = -9y
Ex: for what values of r does the function y = ert satisfy the same DE y'' = -9y ?
[solve r2ert = -9ert to get r = ±3i]
Confirm that the functions in a given family are solutions to a given DE #3-4
Ex from above: verify that y = C1cos(3t) + C2sin(3t) is a solution of the 2nd order DE y'' = -9y
Use implicit diff to confirm a given solution to a given DE: #5-6
Solve DE using integrating factors, apply initial conditions
Solve 1st order linear DE by method of integrating factors: #7-14
Technique applies to first order linear DE, of the form y' + p(x) y = q(x)
Integrating factor is μ = e ^ int(p(x)) μ =![]()
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Technique: Calculate the integrating factor;
Omit the "+C" at this step, since any antiderivative works as an integrating factor
Then write y ∙ μ = int( q(x) ∙ μ )
Result is y ∙ μ = f(x) + C Exponential forms: If f(x) = eg(x), this becomes y ∙ μ = Ceg(x)
Solve for y: y = 1/μ ∙ f(x) + 1/μ ∙ C For the exponential form, we get y = 1/μ ∙ Ceg(x)
After getting this result, apply the initial condition to find and replace the value of C
Solve separable equations, finding general solution: #15-24
To be separable, you must be able to write the DE in the forms
dy/dx = f(x) ∙ g(y) result: g(y) dy = f(x) dx ...or
dy/dx = f(x) / g(y) result: dy / g(y) = f(x) dx
Then integrate both sides, putting the "+C" on only the right side
Solve for y if possible, to express the family of solutions as an explicit function of x
After getting this result, apply the initial condition to find and replace the value of C
Sketch several typical integral curves
Apps in later half of the asgn
Geometric (example 6)
Mixing problems (Example 7)
Free fall retarded by air resistance (Discussion in text, solved in X47)
9.2
Direction
Fields; Euler's Method OMIT
Lecture:
Slopefields
Manual technique: Ex, y' = x+y
Maple: with(DEtools);
dfieldplot(diff(y(x),x)=x+y(x),[y(x)],x=-3..3,y=-3..3)
TI-89:
TI-86:
Graphmatica: dy = y+x {0,1} -- to specify an initial condition
Show how to estimate the graph of a solution with a given initial condition
DEs for electronics: Explain the DEs for
RL circuit: E = L * dI/dL + RI
RC circuit: E = RI + Q/C, but since I = dQ/dt:
E = R * dQ/dt +Q/C
Note: Eqn for RL circuit becomes E = L * d2Q/dt2 + R * dQ/dt
and RLC circuit becomes E = L * Q'' + R * Q' + 1/C * Q
Hence, Second degree DE's are common in electronics
Omit the numerical approach for Euler's method
9.3 Modeling with First-Order Differential Equations
Fact: Modeling real-world phenomena often involves observing how fast quantities change;
since
rates of change are derivatives, the models are often differential equations
Def: a DE is an eqn that contains an unknown function and its derivatives
Classic example: unconstrained population growth:
model: growth is proportional to the population
mathematically,
dy/dt = ky, where k is the
constant of proportionality (the growth rate)
Sol of basic exp growth eqn dy/dt = ky yields y(t) = y0ekt
Note: k = growth rate
"Relative growth rate": k = y' / y
Growth: bacteria
Doubling time vs half-life
Radioactive decay
Half-life: show that in general, k = -ln(2) / halflife
Show how to set up eqn to calculate half-life
Continuous compound interest
Basic comp int formula
Take limit as n goes to ¥
A = Pert note r = interest rate
Example of constrained population growth (e.g. limited food supply, spread of disease)
dy/dt = ky(L-y), where L is the maximum sustainable level for the population
Note that there is no growth if y is 0 or L,
max growth if y is halfway between 0 and L
neg growth if y > L (N/A for disease in a population of L indiv)
Other Examples
by Hooke's Law, the force on a spring is proportional to the extension of the spring
F = -kx (negative because the force is opposite to the direction of the extension)
Since (
m * d2x/dt2 = -kx
This is a second order DE (order of a DE is the level of the highest derivative in the eqn, here, 2)
Analysis of y'=y(y-2): note techniques:
Constant solutions will be where y' = 0. Solve by factoring, in this case
y is increasing when y' >0 [you're now solving a polynomial inequality]
y is decreasing when y' <0
9.4
Second-Order
Linear Homogeneous Differential Equations; The Vibrating Spring OMIT
Orthogonal trajectories:
Ex: Graphs: y=ke^-x for several values of k; y=±sqrt(2x+c) for several values of c
Method: y'=-ke^-x; eliminate k: y' = -y; integrate neg recip y' = 1/y

If you do not eliminate k, you get a family that is orthogonal to a single graph (with a fixed k):
y=ke^-x; orthogonal graphs y=(1/k)e^x+c for several values of c and a fixed k=1)
Method: y'=-e^-x; integrate neg recip y' = e^x

Trig Identity Note
a cos t + b sin t = sqrt(a^2+b^2) sin (t + arctan(a/b))
Proof: Let a/sqrt(a^2+b^2) and b/ sqrt(a^2+b^2) = sinq and cosq, for rt triangle with legs a and b.
Mult and divide the expression a cos t + b sin t by sqrt(a^2+b^2) and sub in sinq and cosq.
Use identity for sin(q + t)
Return to: Merced College; Don Power Updated 10/08/07 by Don Power