Question #a9319
1 Answer
#(dy)/(dx) = -(2x + 2y + y^"1/3"x^-"2/3")/(2x + 2y + x^"1/3"y^-"2/3")#
You had:
#-(x+y)^2 - 3(root(3)(xy)) + 8pi = -12#
Well, with the constants, we can ignore those. Their derivatives with respect to any variable is zero. So, this is really going to have the same derivative as
#-(x+y)^2 - 3(root(3)(xy)) = C# ,
where
#-(x^2 + 2xy + y^2) - 3(x)^"1/3"(y)^"1/3" = C#
by expanding the square. Now the derivative becomes a bit easier. If we had stuck to
Taking this as
#-2x - 2(xcdot(dy)/(dx) + y) - 2y(dy)/(dx) - 3*[x^"1/3"1/3y^-"2/3"(dy)/(dx) + y^"1/3"cdot1/3x^-"2/3"] = 0#
Note that when you take the derivative with respect to
#(d)/(dx)[f(y)] = (df(y))/(dx) = (df(y))/(dy)(dy)/(dx)# .
For instance,
Simplify first, then try to separate out the
#-2x - color(red)(2x(dy)/(dx)) - 2y - color(red)(2y(dy)/(dx)) - color(red)(x^"1/3"y^-"2/3"(dy)/(dx)) - y^"1/3"x^-"2/3" = 0#
#-2x - 2y - y^"1/3"x^-"2/3" = color(red)(2x(dy)/(dx) + 2y(dy)/(dx) + x^"1/3"y^-"2/3"(dy)/(dx))#
#-(2x + 2y + y^"1/3"x^-"2/3") = (2x + 2y + x^"1/3"y^-"2/3")(dy)/(dx)#
#=> color(blue)((dy)/(dx) = -(2x + 2y + y^"1/3"x^-"2/3")/(2x + 2y + x^"1/3"y^-"2/3"))#
Wolfram Alpha gives:
#(dy)/(dx) = -(2x(xy)^"2/3"+2y(xy)^"2/3"+y)/(2x(xy)^"2/3"+2y(xy)^"2/3"+x)#
We could verify we got it by matching that; simply multiply by
#(xy)^"2/3"/(xy)^"2/3"[-(2x + 2y + y^"1/3"x^-"2/3")/(2x + 2y + x^"1/3"y^-"2/3")]#
#= -(2x(xy)^"2/3" + 2y(xy)^"2/3" + y^"1/3"x^-"2/3"(xy)^"2/3")/(2x(xy)^"2/3" + 2y(xy)^"2/3" + x^"1/3"y^-"2/3"(xy)^"2/3")#
#= -(2x(xy)^"2/3" + 2y(xy)^"2/3" + y^("1/3"+"2/3")x^(-"2/3"+"2/3"))/(2x(xy)^"2/3" + 2y(xy)^"2/3" + x^("1/3"+"2/3")y^(-"2/3"+"2/3")#
#= -(2x(xy)^"2/3" + 2y(xy)^"2/3" + y)/(2x(xy)^"2/3" + 2y(xy)^"2/3" + x# #color(blue)(sqrt"")#
Yep, we got it!