Math Problem Statement

G3.) Consider the vector field vec F = \langleP, Q\rangle = \langle(- y)/((x - y) ^ 2), x/((x - y) ^ 2)\rangle; mathcal D =\ (x, y) in mathbb R ^ 2 |y<x\ . on the domain ()(1 pt) Make a picture of the set D. Is D simply connected? (ii) (1 pt) Show that partial P partial y = partial Q partial x on the domain D. (iii) (1 pt) Based on the partial derivative test from part (ii) and your answer to (i), is it safe to conclude that vec F is conservative on the set D? Explain your answer. (Your explanation should reference the type of domain you have here.) (iv) (2 pts) Using the standard procedure for finding potentials, find a potential function g for vec F . (v) (1 pt) Using the fundamental theorem of calculus for line integrals and part (iv), compute the integral int gamma vec F * d vec r , where gamma is a curve in the domain D starting at the point (0, - 1) and terminating at the point (1,0).

Solution

Let's go through each part of the question step-by-step:

Given Data:

The vector field is given by: F=P,Q=y(xy)2,x(xy)2\vec{F} = \langle P, Q \rangle = \left\langle \frac{-y}{(x - y)^2}, \frac{x}{(x - y)^2} \right\rangle The domain is: D={(x,y)R2  y<x}\mathcal{D} = \{(x, y) \in \mathbb{R}^2 \ | \ y < x\}

Solution:

(i) Picture of the Set DD and Simple Connectedness

The set DD consists of points (x,y)(x, y) where y<xy < x. This is the region below the line y=xy = x in the xyxy-plane. A sketch would show the half-plane under this line.

Now, to determine if DD is simply connected:

  • A region is simply connected if it has no holes, meaning any closed loop within the region can be continuously contracted to a point without leaving the region.
  • Since y<xy < x creates a half-plane with no holes, DD is indeed simply connected.

(ii) Verifying Py=Qx\frac{\partial P}{\partial y} = \frac{\partial Q}{\partial x}

  1. Calculate Py\frac{\partial P}{\partial y}: P=y(xy)2P = \frac{-y}{(x - y)^2} Differentiate PP with respect to yy: Py=1(xy)2(y)(2)(xy)(1)(xy)4=(xy)22y(xy)(xy)3=x(xy)3\frac{\partial P}{\partial y} = \frac{-1 \cdot (x - y)^2 - (-y)(2)(x - y)(-1)}{(x - y)^4} = \frac{- (x - y)^2 - 2y(x - y)}{(x - y)^3} = \frac{x}{(x - y)^3}

  2. Calculate Qx\frac{\partial Q}{\partial x}: Q=x(xy)2Q = \frac{x}{(x - y)^2} Differentiate QQ with respect to xx: [ \frac{\partial Q}{\partial x} = \frac{1 \cdot (x - y)^2 - x \cdot 2(x - y)}{(x - y)^4} = \frac{(x - y) - 2x(x - y)}

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Math Problem Analysis

Mathematical Concepts

Vector Fields
Conservative Fields
Partial Derivatives
Potential Functions
Line Integrals

Formulas

Partial derivatives: \frac{\partial P}{\partial y} and \frac{\partial Q}{\partial x}
Fundamental theorem for line integrals: \int_{\gamma} \vec{F} \cdot d\vec{r} = g(b) - g(a)

Theorems

Fundamental Theorem for Line Integrals
Conservative Vector Field Test

Suitable Grade Level

College-Level Calculus