Verifying a Solution for a First-Order Partial Differential Equation
Problem Statement and Given Solution
We are tasked with showing that the given function $u$ satisfies the following partial differential equation (PDE):
π₯ππ’ππ₯βπ¦ππ’ππ¦=π¦2π’3
The proposed solution is:
π’=(1+2π₯π¦+π¦2)β12
1. Calculate the Partial Derivative ππ’/ππ₯
Using the chain rule, we differentiate $u$ with respect to $x$:
ππ’ππ₯=β12(1+2π₯π¦+π¦2)β32β
(2π¦)=βπ¦(1+2π₯π¦+π¦2)β32
2. Calculate the Partial Derivative ππ’/ππ¦
Using the chain rule, we differentiate $u$ with respect to $y$:
ππ’ππ¦=β12(1+2π₯π¦+π¦2)β32β
(2π₯+2π¦)=β(π₯+π¦)(1+2π₯π¦+π¦2)β32
3. Substitute Derivatives into the Left-Hand Side (LHS)
We substitute the calculated partial derivatives into the expression $π₯ππ’ππ₯βπ¦ππ’ππ¦$:
π₯[βπ¦(1+2π₯π¦+π¦2)β32]βπ¦[β(π₯+π¦)(1+2π₯π¦+π¦2)β32]
Simplifying the signs:
=βπ₯π¦(1+2π₯π¦+π¦2)β32+π¦(π₯+π¦)(1+2π₯π¦+π¦2)β32
4. Factor and Simplify the LHS
We factor out the common term $(1+2π₯π¦+π¦2)β32$:
=(1+2π₯π¦+π¦2)β32[βπ₯π¦+π¦(π₯+π¦)]
Expand the terms inside the brackets:
=(1+2π₯π¦+π¦2)β32[βπ₯π¦+π₯π¦+π¦2]
The $xy$ terms cancel out, leaving the simplified LHS:
=(1+2π₯π¦+π¦2)β32[π¦2]
5. Express the Result in Terms of $u$
We relate the simplified LHS back to the original function $u$. Since $π’=(1+2π₯π¦+π¦2)β12$, we find $u^3$:
π’3=((1+2π₯π¦+π¦2)β12)3=(1+2π₯π¦+π¦2)β32
Substituting $u^3$ into the final LHS expression from Step 4:
π¦2(1+2π₯π¦+π¦2)β32=π¦2π’3
Thus, we have successfully shown that $π₯ππ’ππ₯βπ¦ππ’ππ¦=π¦2π’3$. The given solution satisfies the PDE.