The given system of equations is:
(2x)ln2=(3y)ln3
3lnx=2lny
We begin by applying the natural logarithm,
ln, to both sides of the second equation:
3lnx=2lny
Using the power property
ln(ab)=blna, we bring the exponents down:
(lnx)(ln3)=(lny)(ln2)
We can now define the relationship between
lny and
lnx as:
lny=ln2(lnx)(ln3)
Next, we apply the logarithm to the first equation:
(2x)ln2=(3y)ln3
(ln2)ln(2x)=(ln3)ln(3y)
Applying the product property
ln(ab)=lna+lnb, we expand the expression:
(ln2)(ln2+lnx)=(ln3)(ln3+lny)
We substitute our expression for
lny from the previous phase into this equation:
(ln2)2+(ln2)(lnx)=(ln3)2+(ln3)(ln2(lnx)(ln3))
Expanding and grouping the terms involving
lnx on one side, we obtain:
(lnx)(ln2−ln2(ln3)2)=(ln3)2−(ln2)2
To simplify the left side, we find a common denominator:
(lnx)(ln2(ln2)2−(ln3)2)=(ln3)2−(ln2)2
Notice that
(ln3)2−(ln2)2=−((ln2)2−(ln3)2). Dividing both sides by the common term
((ln2)2−(ln3)2), we get:
ln2lnx=−1