I \heartsuit Substitution!

Calculus Level 4

d y d x + y x = ln x × y 2 \frac{dy}{dx}+\frac{y}{x}=\ln x \times y^{2}

Let y = f ( x ) y=f(x) be a solution to the above differential equation such that f ( 1 ) = 1 f(1)=1 .

Given that f ( x ) = a x b ( c ln d x ) f(x)=\dfrac{a}{x^{b}\left(c-\ln^{d}x\right)} for positive real numbers a , b , c a,b,c and d d , find a + b + c + d a+b+c+d .


The answer is 7.

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3 solutions

Brandon Monsen
Feb 11, 2016

Let's start with the given differential equation:

d y d x + y x = ln ( x ) y 2 \frac{dy}{dx}+\frac{y}{x}=\ln(x)y^{2}

Now, divide both sides by y 2 -y^{-2} to get:

y 2 d y d x 1 x y = l n ( x ) -y^{-2}\frac{dy}{dx}-\frac{1}{xy}=-ln(x)

Let w = y 1 w=y^{-1} . This means that d w d x = y 2 d y d x \frac{dw}{dx}=-y^{-2}\frac{dy}{dx} . Substituting this in gets us:

d w d x w x = l n ( x ) \frac{dw}{dx}-\frac{w}{x}=-ln(x)

Multiply both sides by x x to get:

x d w d x w = x l n ( x ) x\frac{dw}{dx}-w=-xln(x)

Now comes the most crucial step - Let w = u x w=ux for some parameterization u u . This means that d w d x = u + x d u d x \frac{dw}{dx}=u+x\frac{du}{dx} . Now substituting this in gets us:

u x + x 2 d u d x u x = x l n ( x ) ux+x^{2}\frac{du}{dx}-ux=-xln(x) d u d x = l n ( x ) x \frac{du}{dx}=\frac{-ln(x)}{x}

Now this looks like something we know how to deal with!

d u = ln ( x ) x d x \int { du } =\int { \frac { -\ln { \left( x \right) } }{ x } dx }

Let v = l n ( x ) v=ln(x) . Then d v = 1 x d x dv=\frac{1}{x}dx , and so we have:

d u = v d v \int { du } =\int { -v \quad dv }

u = 1 2 v 2 + k u=\frac{-1}{2}v^{2}+k

u = 1 2 l n 2 ( x ) + k u=\frac{-1}{2}ln^{2}(x)+k

From the above information we know that u = w x = 1 x y u=\frac{w}{x}=\frac{1}{xy} , so:

1 x y = 1 2 l n 2 ( x ) + k \frac{1}{xy}= \frac{-1}{2}ln^{2}(x)+k

And finally:

y = 1 k x 1 2 x l n 2 ( x ) y=\frac{1}{kx-\frac{1}{2}xln^{2}(x)}

In order to get the equation in the form that the question asked for, multiply the RHS by 2 2 \frac{2}{2} and pull out the x x in the denominator in order to get:

y = f ( x ) = 2 x ( 2 k l n 2 ( x ) ) y=f(x)=\frac{2}{x(2k-ln^{2}(x))}

Now for the Initial Value piece of the problem. We know that f ( 1 ) = 1 f(1)=1 , and that

f ( 1 ) = 2 2 k f(1)=\frac{2}{2k}

so 2 k = 2 2k=2 , and we can FINALLY write f ( x ) f(x) as

f ( x ) = 2 x ( 2 l n 2 ( x ) ) f(x)=\frac{2}{x(2-ln^{2}(x))}

and so a + b + c + d = 2 + 1 + 2 + 2 = 7 a+b+c+d=2+1+2+2=\boxed{7} .

I'm quite surprised that none of the posted solutions mention that this is a standard Bernoulli differential equation (this being the n = 2 n=2 case).

Prasun Biswas - 5 years, 4 months ago

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There is nothing to be surprised. If required,without commenting about your surprise,you should directly post a solution.

asad bhai - 5 years, 3 months ago

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I didn't post a solution since there's a standard well-known method for solving Bernoulli differential equations (if solutions exist) :

For the Bernoulli equation with parameter n n , you multiply both sides by ( 1 n ) y n (1-n)y^{-n} and then make the substitutions V = y 1 n V=y^{1-n} with d V d x = ( 1 n ) y n d y d x \dfrac{\mathrm dV}{\mathrm dx}=(1-n)y^{-n}\dfrac{\mathrm dy}{\mathrm dx} and the differential equation reduces to a first order linear differential equation in V V which is then solved by integrating factor method .

Prasun Biswas - 5 years, 3 months ago

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@Prasun Biswas Actually my solution did use the I.F, I just didn't mention the name Bernoulli.

A Former Brilliant Member - 5 years, 3 months ago

d y d x + y x = ln x y 2 \dfrac{dy}{dx} + \dfrac{y}{x} = \ln x\cdot y^{2}
Dividing by y 2 y^{2}
1 y 2 d y d x + 1 x y = ln x \dfrac{1}{y^{2}} \dfrac{dy}{dx} + \dfrac{1}{xy} = \ln x
1 y = t 1 y 2 d y d x = d t d x \dfrac{1}{y} = t \rightarrow \dfrac{1}{y^{2}} \dfrac{dy}{dx} = \dfrac{-dt}{dx}
The differential transforms into,
d t d x t x = ln x \dfrac{dt}{dx} - \dfrac{t}{x} = - \ln x
This is a linear differential equation of the form d t d x + P t = Q \dfrac{dt}{dx} + Pt = Q
Integrating factor = e P d x = e d x x = 1 x e^{ \int P dx} = e^{ \int \dfrac{-dx}{x}} = \dfrac{1}{x}
Multiplying by 1 x \dfrac{1}{x} on both sides,



d t x d x t x 2 = ln x x \dfrac{dt}{xdx} - \dfrac{t}{x^{2}} = \dfrac{- \ln x}{x}
d ( t x ) d x = ln x x \dfrac{d\left(\dfrac{t}{x}\right)}{dx} = \dfrac{-\ln x}{x}
d ( t x ) = ln x x d x + c 2 \displaystyle \int d\left( \dfrac{t}{x} \right)= \displaystyle \int \dfrac{-\ln x}{x}dx + \dfrac{c}{2}
Integrating both sides,
2 t x = c ln 2 x \dfrac{2t}{x} = c - \ln^{2} x
2 x y = c ln 2 x \dfrac{2}{xy} = c - \ln^{2} x
Since, f ( 1 ) = 1 f(1) = 1
2 1 1 = c 0 c = 2 \dfrac{2}{1\cdot1} = c - 0 \rightarrow c = 2
y = 2 x ( 2 ln 2 x ) \therefore y = \dfrac{2}{x(2-\ln^{2} x)}
Comparing, a = 2 , b = 1, c = 2, d = 2
a + b + c + d = 2 + 2 + 2 + 1 = 7 a + b + c + d= 2 + 2 + 2 + 1 = 7

Fiki Akbar
Feb 12, 2016

First, rewrite the original equation as, x d y d x + y = x y 2 ln ( x ) x \frac{dy}{dx} + y = xy^2 \ln(x) in which can be written as, d ( x y ) d x = x y 2 ln ( x ) \frac{d(xy)}{dx} = xy^2 \ln(x) Define u = x y u = xy , then we have a separable differential equation, d u d x = u 2 x ln ( x ) \frac{du}{dx} = \frac{u^2}{x}\ln(x) Since ln ( x ) x d x = 1 2 ln 2 ( x ) + C \int\:\frac{\ln(x)}{x}\:dx = \frac{1}{2}\ln^2(x)+C , then we have u ( x ) = 1 1 2 ln 2 ( x ) + C u(x) = -\frac{1}{\frac{1}{2}\ln^2(x)+C} or, in original variable, y ( x ) = 1 x ( 1 2 ln 2 ( x ) + C ) y(x) = -\frac{1}{x(\frac{1}{2}\ln^2(x)+C)} The condition y ( 1 ) = 1 y(1)=1 imply C = 1 C=-1 . Hence, we have y ( x ) = 2 x ( 2 ln 2 ( x ) ) y(x) = \frac{2}{x(2-\ln^2(x))}

So, a + b + c + d = 7 a+b+c+d = 7 .

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