Math Problem Statement

Consider the vector field vec F = langle 3x ^ 2 + 2y ^ 2 + 3z; 4xy + 2y - z 3x - y - z). (i) Explain why vec F is conservative on the domain \mathcal{D} = \mathbb{R} ^ 3 . (ii) Find a potential function g(x, y, z) for vec F (iii) Compute the work done by vec F to move a particle from the point (- 1, 0, 1) to the point (0, 0, 1). (iv) Does this work depend on a path gamma used to get from the pint (- 1, 0, 1) to the point (0, 0, 1) ?

Solution

Let's analyze each part of the problem step-by-step:

(i) Explain why F\vec{F} is conservative on the domain D=R3\mathcal{D} = \mathbb{R}^3.

A vector field F\vec{F} is conservative if there exists a scalar potential function g(x,y,z)g(x, y, z) such that F=g\vec{F} = \nabla g. One equivalent condition for a vector field to be conservative in R3\mathbb{R}^3 is that its curl must be zero everywhere in the domain. So we check if ×F=0\nabla \times \vec{F} = \vec{0}.

Given: F=3x2+2y2+3z,4xy+2yz,3xyz\vec{F} = \langle 3x^2 + 2y^2 + 3z, 4xy + 2y - z, 3x - y - z \rangle

To compute ×F\nabla \times \vec{F}, we use the definition of the curl: ×F=(FzyFyz,FxzFzx,FyxFxy)\nabla \times \vec{F} = \left( \frac{\partial F_z}{\partial y} - \frac{\partial F_y}{\partial z}, \frac{\partial F_x}{\partial z} - \frac{\partial F_z}{\partial x}, \frac{\partial F_y}{\partial x} - \frac{\partial F_x}{\partial y} \right) where F=Fx,Fy,Fz\vec{F} = \langle F_x, F_y, F_z \rangle.

Calculating Components of the Curl

  1. Fzy=1\frac{\partial F_z}{\partial y} = -1
  2. Fyz=1\frac{\partial F_y}{\partial z} = -1

So, the first component of ×F\nabla \times \vec{F} is: FzyFyz=1(1)=0\frac{\partial F_z}{\partial y} - \frac{\partial F_y}{\partial z} = -1 - (-1) = 0

  1. Fxz=3\frac{\partial F_x}{\partial z} = 3
  2. Fzx=3\frac{\partial F_z}{\partial x} = 3

So, the second component of ×F\nabla \times \vec{F} is: FxzFzx=33=0\frac{\partial F_x}{\partial z} - \frac{\partial F_z}{\partial x} = 3 - 3 = 0

  1. Fyx=4y\frac{\partial F_y}{\partial x} = 4y
  2. Fxy=4y\frac{\partial F_x}{\partial y} = 4y

So, the third component of ×F\nabla \times \vec{F} is: FyxFxy=4y4y=0\frac{\partial F_y}{\partial x} - \frac{\partial F_x}{\partial y} = 4y - 4y = 0

Since all components of ×F\nabla \times \vec{F} are zero, we conclude: ×F=0\nabla \times \vec{F} = \vec{0} Therefore, F\vec{F} is conservative on R3\mathbb{R}^3.


(ii) Find a potential function g(x,y,z)g(x, y, z) for F\vec{F}.

Since F\vec{F} is conservative, there exists a potential function g(x,y,z)g(x, y, z) such that: F=g=(gx,gy,gz)\vec{F} = \nabla g = \left( \frac{\partial g}{\partial x}, \frac{\partial g}{\partial y}, \frac{\partial g}{\partial z} \right) We are given: Fx=gx=3x2+2y2+3zF_x = \frac{\partial g}{\partial x} = 3x^2 + 2y^2 + 3z Fy=gy=4xy+2yzF_y = \frac{\partial g}{\partial y} = 4xy + 2y - z Fz=gz=3xyzF_z = \frac{\partial g}{\partial z} = 3x - y - z

To find g(x,y,z)g(x, y, z), we integrate each component.

Integrating with respect to xx:

Integrate FxF_x with respect to xx: g(x,y,z)=(3x2+2y2+3z)dx=x3+2xy2+3xz+h(y,z)g(x, y, z) = \int (3x^2 + 2y^2 + 3z) \, dx = x^3 + 2xy^2 + 3xz + h(y, z) where h(y,z)h(y, z) is a function of yy and zz alone.

Differentiating with respect to yy:

gy=4xy+hy\frac{\partial g}{\partial y} = 4xy + \frac{\partial h}{\partial y} Comparing this with Fy=4xy+2yzF_y = 4xy + 2y - z, we find: hy=2yz\frac{\partial h}{\partial y} = 2y - z Integrating with respect to yy: h(y,z)=y2yz+k(z)h(y, z) = y^2 - yz + k(z) where k(z)k(z) is a function of zz alone.

Differentiating with respect to zz:

[ \frac{\partial g}{\partial z} = 3x - y - \frac{d}{dz}(yz) - \frac{d}{dz}

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Math Problem Analysis

Mathematical Concepts

Vector Calculus
Conservative Fields
Potential Functions
Work in Vector Fields

Formulas

∇ × F = 0 (curl of a conservative field)
∇g = F (gradient of a potential function equals the vector field)
Work done in a conservative field W = g(final point) - g(initial point)

Theorems

Conservative Vector Field Theorem
Fundamental Theorem of Line Integrals

Suitable Grade Level

Undergraduate (Calculus III level)