Answer on Question #46086, Physics-Mechanics-Kinematics-Dynamics
If the force field defined by vector F ⃗ = ( 3 x 2 y z − 3 y ) i ⃗ + ( x 3 z − 3 x ) j ⃗ + ( x 3 y + 2 z ) k ⃗ \vec{F} = (3x^{2}yz - 3y)\vec{i} + (x^{3}z - 3x)\vec{j} + (x^{3}y + 2z)\vec{k} F = ( 3 x 2 yz − 3 y ) i + ( x 3 z − 3 x ) j + ( x 3 y + 2 z ) k conservative? if so, find the scalar potential associated with the vector F F F .
Solution
F ⃗ = ( 3 x 2 y z − 3 y ) i ⃗ + ( x 3 z − 3 x ) j ⃗ + ( x 3 y + 2 z ) k ⃗ = M ( x , y , z ) i ⃗ + N ( x , y , z ) j ⃗ + P ( x , y , z ) k ⃗ \vec{F} = (3x^{2}yz - 3y)\vec{i} + (x^{3}z - 3x)\vec{j} + (x^{3}y + 2z)\vec{k} = M(x,y,z)\vec{i} + N(x,y,z)\vec{j} + P(x,y,z)\vec{k} F = ( 3 x 2 yz − 3 y ) i + ( x 3 z − 3 x ) j + ( x 3 y + 2 z ) k = M ( x , y , z ) i + N ( x , y , z ) j + P ( x , y , z ) k
Then, F ⃗ \vec{F} F is conservative if and only if
∂ P ∂ x = ∂ M ∂ z , ∂ N ∂ x = ∂ M ∂ y , ∂ P ∂ y = ∂ N ∂ z . \frac{\partial P}{\partial x} = \frac{\partial M}{\partial z}, \frac{\partial N}{\partial x} = \frac{\partial M}{\partial y}, \frac{\partial P}{\partial y} = \frac{\partial N}{\partial z}. ∂ x ∂ P = ∂ z ∂ M , ∂ x ∂ N = ∂ y ∂ M , ∂ y ∂ P = ∂ z ∂ N . ∂ P ∂ x = ∂ ∂ x ( x 3 y + 2 z ) = 3 x 2 y . \frac{\partial P}{\partial x} = \frac{\partial}{\partial x}(x^{3}y + 2z) = 3x^{2}y. ∂ x ∂ P = ∂ x ∂ ( x 3 y + 2 z ) = 3 x 2 y . ∂ P ∂ y = ∂ ∂ y ( x 3 y + 2 z ) = x 3 . \frac{\partial P}{\partial y} = \frac{\partial}{\partial y}(x^{3}y + 2z) = x^{3}. ∂ y ∂ P = ∂ y ∂ ( x 3 y + 2 z ) = x 3 . ∂ M ∂ y = ∂ ∂ y ( 3 x 2 y z − 3 y ) = 3 x 2 z − 3. \frac{\partial M}{\partial y} = \frac{\partial}{\partial y}(3x^{2}yz - 3y) = 3x^{2}z - 3. ∂ y ∂ M = ∂ y ∂ ( 3 x 2 yz − 3 y ) = 3 x 2 z − 3. ∂ M ∂ z = ∂ ∂ z ( 3 x 2 y z − 3 y ) = 3 x 2 y . \frac{\partial M}{\partial z} = \frac{\partial}{\partial z}(3x^{2}yz - 3y) = 3x^{2}y. ∂ z ∂ M = ∂ z ∂ ( 3 x 2 yz − 3 y ) = 3 x 2 y . ∂ N ∂ x = ∂ ∂ x ( x 3 z − 3 x ) = 3 x 2 z − 3. \frac{\partial N}{\partial x} = \frac{\partial}{\partial x}(x^{3}z - 3x) = 3x^{2}z - 3. ∂ x ∂ N = ∂ x ∂ ( x 3 z − 3 x ) = 3 x 2 z − 3. ∂ N ∂ z = ∂ ∂ z ( x 3 z − 3 x ) = x 3 . \frac{\partial N}{\partial z} = \frac{\partial}{\partial z}(x^{3}z - 3x) = x^{3}. ∂ z ∂ N = ∂ z ∂ ( x 3 z − 3 x ) = x 3 .
So ∂ P ∂ x = ∂ M ∂ z = 3 x 2 y \frac{\partial P}{\partial x} = \frac{\partial M}{\partial z} = 3x^{2}y ∂ x ∂ P = ∂ z ∂ M = 3 x 2 y , ∂ N ∂ x = ∂ M ∂ y = 3 x 2 z − 3 \frac{\partial N}{\partial x} = \frac{\partial M}{\partial y} = 3x^{2}z - 3 ∂ x ∂ N = ∂ y ∂ M = 3 x 2 z − 3 , ∂ P ∂ y = ∂ N ∂ z = x 3 \frac{\partial P}{\partial y} = \frac{\partial N}{\partial z} = x^{3} ∂ y ∂ P = ∂ z ∂ N = x 3 and the force field F ⃗ \vec{F} F is conservative.
Let's find the scalar potential f f f associated with the vector F ⃗ \vec{F} F
∂ f ∂ x = M = ( 3 x 2 y z − 3 y ) , \frac{\partial f}{\partial x} = M = (3x^{2}yz - 3y), ∂ x ∂ f = M = ( 3 x 2 yz − 3 y ) , ∂ f ∂ y = N = ( x 3 z − 3 x ) , \frac{\partial f}{\partial y} = N = (x^{3}z - 3x), ∂ y ∂ f = N = ( x 3 z − 3 x ) , ∂ f ∂ z = P = ( x 3 y + 2 z ) . \frac{\partial f}{\partial z} = P = (x^{3}y + 2z). ∂ z ∂ f = P = ( x 3 y + 2 z ) .
If we integrate the first of the three equations with respect to x x x , we find that
f ( x , y , z ) = ∫ ( 3 x 2 y z − 3 y ) d x = x 3 y z − 3 y x + g ( y , z ) . f(x,y,z) = \int (3x^{2}yz - 3y)dx = x^{3}yz - 3yx + g(y,z). f ( x , y , z ) = ∫ ( 3 x 2 yz − 3 y ) d x = x 3 yz − 3 y x + g ( y , z ) .
where g ( y , z ) g(y,z) g ( y , z ) is a constant dependent on y y y and z z z variables. We then calculate the partial derivative with respect to y y y from this equation and match it with the equation of above.
∂ f ∂ y = ∂ ∂ y ( x 3 y z − 3 y x + g ( y , z ) ) = x 3 z − 3 x + ∂ g ∂ y = ( x 3 z − 3 x ) . \frac{\partial f}{\partial y} = \frac{\partial}{\partial y}\big(x^{3}yz - 3yx + g(y,z)\big) = x^{3}z - 3x + \frac{\partial g}{\partial y} = (x^{3}z - 3x). ∂ y ∂ f = ∂ y ∂ ( x 3 yz − 3 y x + g ( y , z ) ) = x 3 z − 3 x + ∂ y ∂ g = ( x 3 z − 3 x ) .
This means that the partial derivative of g g g with respect to y y y is 0, thus eliminating y y y from g g g entirely and leaving at as a function of z z z alone.
f ( x , y , z ) = x 3 y z − 3 y x + h ( z ) . f(x, y, z) = x^3 y z - 3 y x + h(z). f ( x , y , z ) = x 3 yz − 3 y x + h ( z ) .
We then repeat the process with the partial derivative with respect to z z z
∂ f ∂ z = ∂ ∂ z ( x 3 y z − 3 y x + h ( z ) ) = x 3 y + d h d z = ( x 3 y + 2 z ) \frac{\partial f}{\partial z} = \frac{\partial}{\partial z} \left(x^3 y z - 3 y x + h(z)\right) = x^3 y + \frac{d h}{d z} = (x^3 y + 2 z) ∂ z ∂ f = ∂ z ∂ ( x 3 yz − 3 y x + h ( z ) ) = x 3 y + d z d h = ( x 3 y + 2 z )
which means that
d h d z = ( 2 z ) \frac{d h}{d z} = (2 z) d z d h = ( 2 z )
so we can find h ( z ) h(z) h ( z ) by integrating:
h ( z ) = z 2 + c . h(z) = z^2 + c. h ( z ) = z 2 + c .
Therefore,
f ( x , y , z ) = x 3 y z − 3 y x + z 2 + c . f(x, y, z) = x^3 y z - 3 y x + z^2 + c. f ( x , y , z ) = x 3 yz − 3 y x + z 2 + c .
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