WEBVTT

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&gt;&gt; Welcome to the Cypress
College Math Review

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on Second Order Differential
Equations, Special Types.

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In general a 2nd order
differential equation can be

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written as a function of
the independent variable,

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the dependent variable and the
first and second derivatives.

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There are two special types of
2nd order differential equations

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where a substitution
reduces them

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to a 1st order differential
equation

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that we're able to solve.

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The first type has no dependent
variable or no x in this case.

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By substituting v equal dx
dt or the first derivative,

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the second derivative
becomes the derivative of v

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with respect to t or v prime.

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[ Pause ]

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In this first example t is
the independent variable

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and x is the dependent
variable and x is missing.

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This is a 2nd order
differential equation.

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So we let v equal dx dt which
means that the second derivative

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of x with respect to t will
equal dv dt or v prime.

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We make these substitutions.

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So t squared times v prime
plus v squared is equal

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to 2t times v. Interchanging
the last two terms.

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[ Pause ]

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Divide each term by t squared.

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[ Pause ]

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The left hand side looks like
we have a 1st order linear

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differential equation.

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But we look at the right hand
side and we recognize that no,

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we have instead a Bernoulli
differential equation.

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Here's the form for a
Bernoulli differential equation.

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So the first step to solve a
Bernoulli differential equation

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would be to divide
by y to the nth

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which in this case is v squared.

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So we have v to the negative
2, v prime minus 2 over t,

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v to the negative 1 is equal
to negative 1 over t squared.

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We make our substitution.

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We let u equal y to
the 1 minus n power.

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Well in this case u will be
v to the 1 minus 2 power.

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So that's v to the
negative 1 power.

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We also have to find
out what u prime is,

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so u prime would be negative v

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to the negative 2 times v
prime by the chain rule.

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So we replace v to
the negative 2 v prime

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with the opposite of u prime.

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We replace v to the
negative 1 with u.

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[ Pause ]

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Multiply both sides of this
equation by negative 1.

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[ Pause ]

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Now we have a 1st order linear
differential equation that's

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in standard form.

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[ Pause ]

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Now we solve this 1st order
linear differential equation.

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Here's our format.

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We need to find the
integrating factor mu.

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There's our formula for mu.

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P of x in this case
is positive 2

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over t. We simplify
to get t squared.

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So when we solve a 1st order
linear differential equation we

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get mu times y equals
the antiderivative

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of the product of q with mu.

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So in this case we'll have
the integrating factor mu

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which is t squared times
our function u is equal

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to the antiderivative of mu

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which is t squared times
the function q which is 1

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over t squared, we're
integrating that with respect

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to t. So we get t plus the
constant of integration.

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So u is equal to t plus
c sub 1 over t squared.

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And now we substitute back, u is
equal it v the negative 1 power

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so 1 over v is equal to this.

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[ Pause ]

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So let's take reciprocals.

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So v is equal to t
squared over t plus c sub 1

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and we substitute back.

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Recall that v is equal to dx dt.

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[ Pause ]

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We're going to need
to integrate that.

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So since the degree on top
is greater than or equal

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to the degree on the bottom,
we need to do long division.

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[ Pause ]

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So t squared divided by t is
t. So t times t is t squared,

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c sub 1 times t, change the
signs, divide negative c sub 1 t

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by t and I get negative c sub 1.

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Multiply negative c
sub 1 times 9 divisor

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and I get negative c sub
1t minus c sub 1 squared.

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Change the signs and
I get c sub 1 squared.

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So I'm integrating 1dx equals
and when I'm integrating

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over here on the right
side is my quotient

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which is t minus c sub
1 plus my remainder

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which is c sub 1 squared over my
divisor which is t plus c sub 1.

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I'm integrating with
respect to t.

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So on the left hand
side I get x,

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on the right hand
side I get t squared

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over 2 minus c sub 1 times t
plus c sub 1 squared times the

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natural log of the absent
value of my denominator

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which t plus c sub 1 plus a
new constant of integration.

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And notice that x equals another
constant is also a solution.

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[ Pause ]

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Here's another 2nd order
differential equation.

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The independent variable is t,

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the dependent variable
is x and x is missing.

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When you look at this term here
that's not the 2nd derivative,

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that's the second power
of the 1st derivative.

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So we make our substitutions.

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V is equal to dx dt and the 2nd
derivative is dv dt or v prime.

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So we get 2t times v prime
equals v squared minus 1.

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This is separable
differential equation.

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So we have 1 over the quantity
v squared minus 1 dv equals 1

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over the quantity 2t dt.

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To be able to integrate
that we have do a partial

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fraction decomposition.

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So we have 1 over the product
of v plus 1 with v minus 1.

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To set that up we would
have a over b plus 1 plus b

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over v minus 1, multiply
both sides

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by the least common denominator

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which is the original
denominator.

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So we get 1 equals a times v
minus 1 plus b times v plus 1,

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let v equal 1 and we get
that 1 is equal to 2 times b

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which gives that
b is equal to 1/2.

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If we then let v equal negative
1 we get that 1 is equal

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to negative 2a which tells us
that a is equal to negative 1/2.

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So now the integral on the
left hand side becomes a

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which is negative 1/2
over v plus 1 plus b

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which is 1/2 over v minus 1.

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On the right hand side we're
integrating 1/2 over t dt,

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multiply by 2 and we
get negative natural log

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of the absolute value of the
denominator plus natural log

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of the absolute value of the
denominator equals natural log

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of the absolute value

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of the denominator plus our
constant of integration.

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We're going to go ahead
and call our constant

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of integration the natural
log of the absolute value of c

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so that we're able to
combine these logarithms.

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That's a trick that you can use

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that makes things
easier for you.

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[ Pause ]

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Let's combine the logarithms.

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[ Pause ]

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Exponentiate both sides.

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[ Pause ]

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So now we have this
quotient equals plus

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or minus c t. We can
go ahead and call

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that a new constant c sub 1
times t. Now let's solve for v.

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So we cross multiply and we have
v minus 1 equals c sub 1 tv plus

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c sub 1 t. So v minus c sub
1 tv equals c sub 1 t plus 1.

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Factor out a v.

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[ Pause ]

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So v is equal to c
sub 1 t plus 1 divided

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by 1 minus c sub 1 times
t. Let's substitute back.

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V is equal to dx dt, separate.

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[ Pause ]

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And since the degree on top
is greater than or equal

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to the degree on the bottom
we have to do long division.

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[ Pause ]

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Divide c sub 1t by
negative c sub 1t

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and we simply get negative 1.

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Multiply negative
1 times my divisor

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and we get c sub 1 times t
minus 1, change the signs

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and we get 2 as our remainder.

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So on the right hand side
we're integrating negative 1

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which is our quotient
plus or remainder

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which is 2 over our divisor.

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So our answer x is equal to
negative t plus and we need

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to do a u substitution here
to be able to integrate this.

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U equals negative c sub 1t plus
1, so du is negative c sub 1 dt.

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So our integral turns
out to be negative 2

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over c sub 1 times natural
log of the absolute value

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of 1 minus c sub 1 times t plus
the constant of integration.

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That's the answer to our
differential equation.

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[ Pause ]

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Our second type of 2nd
order differential equation,

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a special type has no
independent variable,

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t is missing.

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In this case we replace dx dt
with v and our goal here is

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to make t completely disappear.

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So we have x in our equation.

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We're replacing dx dt
with v. Now we need

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to replace the 2nd
derivative with something

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that has no t's in it at all.

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So the 2nd derivative is equal
to dv dt but we need that t

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to be completely gone.

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We can't just call it v prime

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because v prime is
the same as dv dt.

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We need that t to be out
of the equation completely.

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By the chain rule dv dt is
equal dv dx times dx dt.

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Dx dt recall is equal to v.
So we make that substitution.

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So the 2nd derivative can
be written as dv dx times v.

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If we make that substitution
now our equation can be written

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in terms of x v and dv dx
times v. No t's at all.

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Now we can solve the
differential equation.

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Here's our first example.

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It's a 2nd order differential
equation and t is missing.

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So we make our substitutions.

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We're going to replace dx dt
with v and then we're going

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to replace the 2nd
derivative with dv dx times v.

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So x squared plus 1 times dv
dx times v equals 2x times

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v squared.

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This is a separable
differential equation.

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I get 1 over v dv equals 2x

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over the quantity x
squared plus 1 dx.

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So natural log of the absolute
value of v equals natural log

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of the absolute value of the
quantity x squared plus 1 plus

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and then I chose the form of
my constant of integration

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to be natural log of
the absolute value of c

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because all the other
terms are natural logs.

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So this is equal to natural
log of the absolute value

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of c times the quantity
x squared plus 1.

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I combine those logarithms
on the right hand side,

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exponentiate both sides.

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So I have absolute value
of v equals absolute value

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of c times the quantity
x squared plus 1.

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[ Pause ]

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So v is equal to plus or minus
c times the quantity x squared

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plus 1.

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So v is equal to a new
constant times that quantity.

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Replace v to what it's
equal to which is dx dt.

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[ Pause ]

00:20:09.716 --> 00:20:14.986 A:middle
And is a separable differential
equation so we have 1

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over the quantity x
squared plus 1 dx.

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And the right hand side we're
just integrating the constant.

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So on the left hand
side we get arctangent,

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the right hand side we get c sub
1 times t plus a new constant

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of integration.

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So x equals tangent
of this quantity.

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X equals a constant
is also a solution

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to this differential equation.

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[ Pause ]

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And that gives us the solutions
to this differential equation.

00:21:03.516 --> 00:21:13.076 A:middle
[ Pause ]

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On this next example we don't
even see what our independent

00:21:16.606 --> 00:21:17.526 A:middle
variable would be.

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Let's write it in terms
of [inaudible] notation

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and just choose an
independent variable.

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So it would be the
2nd derivative of y,

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let's say with respect to t plus
y times the 1st derivative cubed

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equals zero.

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So the independent
variable t is missing,

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we're going to make
our substitution.

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So v is equal to dy dt and
the 2nd derivative is equal

00:21:54.176 --> 00:22:00.406 A:middle
to dv dy times v. So we
replace the 2nd derivative

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with v times dv dy.

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And then we have plus y times
and the derivative gets replaced

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with v, so we have
the derivative cubed

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so we have v cubed and
that's equal to zero.

00:22:20.366 --> 00:22:26.066 A:middle
This is a separable differential
equation separating the terms.

00:22:26.866 --> 00:22:39.616 A:middle
We have v over v cubed
dv equals negative y dy.

00:22:40.696 --> 00:22:43.736 A:middle
On the left hand side we're
integrating v to the negative 2.

00:22:46.286 --> 00:22:48.816 A:middle
On the right hand side we're
integrating negative y.

00:22:51.396 --> 00:22:53.236 A:middle
So we get negative v

00:22:53.236 --> 00:22:57.426 A:middle
to the negative 1
equals negative y squared

00:22:57.426 --> 00:23:00.776 A:middle
over 2 plus c sub 1.

00:23:01.516 --> 00:23:10.446 A:middle
[ Pause ]

00:23:10.946 --> 00:23:23.436 A:middle
So we get 1 over v is equal
to, to multiply by negative 1

00:23:23.436 --> 00:23:25.686 A:middle
but let's also get a
common denominator here.

00:23:29.136 --> 00:23:31.946 A:middle
So 1 over v is equal

00:23:31.946 --> 00:23:38.646 A:middle
to y squared plus
new constant over 2.

00:23:45.396 --> 00:23:58.036 A:middle
So v is equal to 2 over
y squared plus c sub 2.

00:24:02.486 --> 00:24:03.766 A:middle
Now we substitute back.

00:24:05.796 --> 00:24:08.116 A:middle
So v is equal to dy dt.

00:24:09.516 --> 00:24:19.466 A:middle
[ Pause ]

00:24:19.966 --> 00:24:23.016 A:middle
So we integrate the
left hand side,

00:24:23.456 --> 00:24:29.656 A:middle
we're integrating y squared
plus c sub 2 with respect to y.

00:24:29.656 --> 00:24:34.746 A:middle
And the right hand side
we're integrating just 2.

00:24:41.686 --> 00:24:54.396 A:middle
So we have y cubed over 3 plus
c sub 2 times y equals 2t plus

00:24:54.626 --> 00:24:57.496 A:middle
another constant c sub 3 or
a constant of integration.

00:24:59.216 --> 00:25:07.886 A:middle
If I multiply 3 by 3 we have
y cubed plus 3 times cu sub 2,

00:25:07.886 --> 00:25:10.096 A:middle
so we have another
constant, a new constant,

00:25:10.626 --> 00:25:19.476 A:middle
we'll call it c sub 4 times y
equals 6t plus 3 times our old

00:25:19.476 --> 00:25:22.176 A:middle
constant c sub 3, we'll
call that c sub 5.

00:25:23.636 --> 00:25:27.196 A:middle
So here's our solution to
the differential equation.

00:25:29.446 --> 00:25:32.846 A:middle
Now you do need to note that
you have two different arbitrary

00:25:32.876 --> 00:25:33.686 A:middle
constants here.

00:25:33.736 --> 00:25:35.886 A:middle
I call them c sub 4 and c sub 5.

00:25:36.606 --> 00:25:39.176 A:middle
Your numbering scheme will
probably be different.

00:25:39.906 --> 00:25:42.616 A:middle
But you do have to note that you
do have two different arbitrary

00:25:42.616 --> 00:25:43.286 A:middle
constants here.

00:25:44.516 --> 00:25:53.466 A:middle
[ Pause ]

00:25:53.966 --> 00:25:56.746 A:middle
Here's some additional
problems to try on your own.

00:25:57.596 --> 00:26:02.486 A:middle
I encourage you to pause
the video, do these problems

00:26:03.286 --> 00:26:05.956 A:middle
and then check with
the solutions that are

00:26:05.956 --> 00:26:07.296 A:middle
at the end of the video.

00:26:08.516 --> 00:26:16.426 A:middle
[ Pause ]

00:26:16.926 --> 00:26:19.346 A:middle
Here are the solutions
to the practice problems.

00:26:20.516 --> 00:26:27.500 A:middle
[ Pause ]

