Analyzing the Setup
We begin with the differential equation:
At first glance, this appears complex. However, we recognize that the term xdy−ydx is the numerator of the derivative of the quotient xy.
By dividing both sides of the equation by
x2, we transform the expression into a recognizable form:
The Elegance of Substitution
By separating the variables, we arrive at the following integral:
The left side is the standard integral for sin−1(xy), while the right side yields lnx+C. Applying the initial condition y(1)=0, we find that C=0.
This reveals the hidden curve:
y=xsin(lnx)
The Journey Through the Integral
We must find the area
A bounded by this curve from
x=1 to
x=eπ:
A=∫1eπxsin(lnx)dx
To solve this, we use the substitution t=lnx, which implies x=et and dx=etdt. The limits of integration change from [1,eπ] to [0,π].
The integral becomes:
A=∫0πe2tsintdt
Evaluating the Integral
We utilize the standard integration formula:
∫eatsinbtdt=a2+b2eat(asinbt−bcosbt)
Applying this with
a=2 and
b=1:
A=[5e2t(2sint−cost)]0π
Evaluating at the limits:
A=5e2π(2sinπ−cosπ)−5e0(2sin0−cos0)
A=5e2π(0−(−1))−51(0−1)
A=51e2π+51
Final Calculation
Comparing our result
A=51e2π+51 with the given form
αe2π+β, we identify:
α=51,β=51
The final required value is:
10(α+β)=10(51+51)=10(52)=4