Solution. We write the equation as
dxdy=tan(x+y)1−1
dxdy=tan(x+y)1−tan(x+y
tan(x+y)dy=(1−tan(x+y))dx
(tan(x+y)−1)dx+tan(x+y)dy=0 Consider the equation as
M(x,y)dx+N(x,y)dy=0. Therefore
M(x,y)=tan(x+y)−1
N(x,y)=tan(x+y)
∂y∂M=cos2(x+y)1
∂x∂N=cos2(x+y)1∂y∂M=∂x∂N This equation is an equation in full differentials. Let U(x,y) is solution of the equation. Therefore
∂x∂U=tan(x+y)−1=cos(x+y)sin(x+y−1Integrating x we get
U(x,y)=−lncos(x+y)−x+C(y)
where C(y) is function of y. Hence
∂y∂U=tan(x+y)+C′(y)=tan(x+y)
C′(y)=0
C(y)=Cwhere C is constant. Therefore get
U(x,y)=−lncos(x+y)−x+Cwhere C is constant.
Answer.
U(x,y)=−lncos(x+y)−x+Cwhere C is constant.
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