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Determine if the differential equation (3x2y + e^y)dx + (x3 + xe^y − 2y)dy = 0 is exact and solve it.

Mathematics

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Answers

2 parts
a

x3y+xey−y2=Cx^3y + xe^y - y^2 = C

b

xsin⁡y+ycos⁡x=Cx \sin y + y \cos x = C

Step-by-step solution

6 steps

Here's how to determine if the differential equations are exact and solve them.

Part a· 3 steps

(3x2y+ey)dx+(x3+xey−2y)dy=0(3x^2y + e^y)dx + (x^3 + xe^y - 2y)dy = 0

  1. Identify M(x,y)M(x,y) and N(x,y)N(x,y).

    The differential equation is in the form M(x,y)dx+N(x,y)dy=0M(x,y)dx + N(x,y)dy = 0.

    M(x,y)=3x2y+eyM(x,y) = 3x^2y + e^y N(x,y)=x3+xey−2yN(x,y) = x^3 + xe^y - 2y
  2. Check for exactness.

    Calculate the partial derivatives ∂M∂y\frac{\partial M}{\partial y} and ∂N∂x\frac{\partial N}{\partial x}.

    ∂M∂y=∂∂y(3x2y+ey)=3x2+ey\frac{\partial M}{\partial y} = \frac{\partial}{\partial y}(3x^2y + e^y) = 3x^2 + e^y ∂N∂x=∂∂x(x3+xey−2y)=3x2+ey\frac{\partial N}{\partial x} = \frac{\partial}{\partial x}(x^3 + xe^y - 2y) = 3x^2 + e^y

    Since ∂M∂y=∂N∂x\frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}, the differential equation is exact.

  3. Find the potential function F(x,y)F(x,y).

    Integrate M(x,y)M(x,y) with respect to xx, treating yy as a constant:

    F(x,y)=∫(3x2y+ey)dx=x3y+xey+g(y)F(x,y) = \int (3x^2y + e^y) dx = x^3y + xe^y + g(y)

    Now, differentiate F(x,y)F(x,y) with respect to yy and set it equal to N(x,y)N(x,y):

    ∂F∂y=∂∂y(x3y+xey+g(y))=x3+xey+g′(y)\frac{\partial F}{\partial y} = \frac{\partial}{\partial y}(x^3y + xe^y + g(y)) = x^3 + xe^y + g'(y)

    Equating this to N(x,y)N(x,y):

    x3+xey+g′(y)=x3+xey−2yx^3 + xe^y + g'(y) = x^3 + xe^y - 2y g′(y)=−2yg'(y) = -2y

    Integrate g′(y)g'(y) with respect to yy to find g(y)g(y):

    g(y)=∫−2ydy=−y2+C0g(y) = \int -2y dy = -y^2 + C_0

    Substitute g(y)g(y) back into F(x,y)F(x,y):

    F(x,y)=x3y+xey−y2+C0F(x,y) = x^3y + xe^y - y^2 + C_0

    The general solution is F(x,y)=CF(x,y) = C, where CC is an arbitrary constant.

    x3y+xey−y2=C\boxed{x^3y + xe^y - y^2 = C}

Part b

xsin⁡y+ycos⁡x=Cx \sin y + y \cos x = C

(sin⁡y−ysin⁡x)dx+(xcos⁡y+cos⁡x)dy=0(\sin y - y \sin x)dx + (x \cos y + \cos x)dy = 0

  1. Identify M(x,y)M(x,y) and N(x,y)N(x,y).

    The differential equation is in the form M(x,y)dx+N(x,y)dy=0M(x,y)dx + N(x,y)dy = 0.

    M(x,y)=sin⁡y−ysin⁡xM(x,y) = \sin y - y \sin x N(x,y)=xcos⁡y+cos⁡xN(x,y) = x \cos y + \cos x
  2. Check for exactness.

    Calculate the partial derivatives ∂M∂y\frac{\partial M}{\partial y} and ∂N∂x\frac{\partial N}{\partial x}.

    ∂M∂y=∂∂y(sin⁡y−ysin⁡x)=cos⁡y−sin⁡x\frac{\partial M}{\partial y} = \frac{\partial}{\partial y}(\sin y - y \sin x) = \cos y - \sin x ∂N∂x=∂∂x(xcos⁡y+cos⁡x)=cos⁡y−sin⁡x\frac{\partial N}{\partial x} = \frac{\partial}{\partial x}(x \cos y + \cos x) = \cos y - \sin x

    Since ∂M∂y=∂N∂x\frac{\partial M}{\partial y} = \frac{\partial N}{\partial x}, the differential equation is exact.

  3. Find the potential function F(x,y)F(x,y).

    Integrate M(x,y)M(x,y) with respect to xx, treating yy as a constant:

    F(x,y)=∫(sin⁡y−ysin⁡x)dx=xsin⁡y−y(−cos⁡x)+g(y)F(x,y) = \int (\sin y - y \sin x) dx = x \sin y - y(-\cos x) + g(y) F(x,y)=xsin⁡y+ycos⁡x+g(y)F(x,y) = x \sin y + y \cos x + g(y)

    Now, differentiate F(x,y)F(x,y) with respect to yy and set it equal to N(x,y)N(x,y):

    ∂F∂y=∂∂y(xsin⁡y+ycos⁡x+g(y))=xcos⁡y+cos⁡x+g′(y)\frac{\partial F}{\partial y} = \frac{\partial}{\partial y}(x \sin y + y \cos x + g(y)) = x \cos y + \cos x + g'(y)

    Equating this to N(x,y)N(x,y):

    xcos⁡y+cos⁡x+g′(y)=xcos⁡y+cos⁡xx \cos y + \cos x + g'(y) = x \cos y + \cos x g′(y)=0g'(y) = 0

    Integrate g′(y)g'(y) with respect to yy to find g(y)g(y):

    g(y)=∫0dy=C0g(y) = \int 0 dy = C_0

    Substitute g(y)g(y) back into F(x,y)F(x,y):

    F(x,y)=xsin⁡y+ycos⁡x+C0F(x,y) = x \sin y + y \cos x + C_0

    The general solution is F(x,y)=CF(x,y) = C, where CC is an arbitrary constant.

    xsin⁡y+ycos⁡x=C\boxed{x \sin y + y \cos x = C}
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