Exact Equations — Question 10

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Question 10

For the exact form ω=(2xy+ex)dx+(x2+2y)dy,\omega=(2xy+e^x)\,dx+(x^2+2y)\,dy, compare two routes from A=(0,0)A=(0,0) to B=(1,1)B=(1,1). Route 1 goes horizontally to (1,0)(1,0) and then vertically to BB; Route 2 goes vertically to (0,1)(0,1) and then horizontally to BB.

For an axis-aligned segment, define its accumulated value as the integral of the coefficient of dxdx along a horizontal segment, or of the coefficient of dydy along a vertical segment, with the stated orientation.

Tasks

  1. Construct a potential FF normalized by F(0,0)=0F(0,0)=0.

  2. Compute both route totals directly as sums of ordinary single-variable integrals.

  3. Explain their equality using the chain rule and find the total around the closed route that follows Route 1 forward and Route 2 backward.

  4. For the differential equation ω=0\omega=0, decide whether one solution curve could pass through both AA and BB. Distinguish this question from the equality of the two route totals.

Original worksheet page 1: question and worked solution for 2-3-010
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Question 10 – Solution

Strategy. A potential measures accumulated change along a route; a solution of the equation ω=0\omega=0 must instead keep that potential constant.

Step 1: Construct a normalized potential. The cross partials are 2x2x. Integrating MM gives F=x2y+ex+h(y)F=x^2y+e^x+h(y); matching NN requires h′=2yh'=2y. Normalization yields F=x2y+ex+y2−1,F(B)=e+1.\boxed{F=x^2y+e^x+y^2-1},\qquad F(B)=e+1.

Step 2: Compute the routes directly. On Route 1, the horizontal and vertical contributions are ∫01exdx=e−1,∫01(1+2y)dy=2,\int_0^1 e^x\,dx=e-1,\qquad \int_0^1(1+2y)\,dy=2, so its total is e+1e+1. On Route 2 they are ∫012ydy=1,∫01(2x+ex)dx=e,\int_0^1 2y\,dy=1,\qquad \int_0^1(2x+e^x)\,dx=e, again totaling e+1\boxed{e+1}.

Step 3: Explain equality and the closed route. Along a differentiable parametrized segment, dF/dt=Fxx′(t)+Fyy′(t)=Mx′+Ny′dF/dt=F_x\,x'(t)+F_y\,y'(t)=Mx'+Ny'. Integration gives the endpoint difference of FF; these differences telescope across joined segments. Both routes therefore give F(B)−F(A)=e+1F(B)-F(A)=e+1. Reversing a route negates its integrals, so the closed-route total is 0\boxed{0}.

Step 4: Distinguish routes from solutions. A solution curve of ω=0\omega=0 has dF/dt=0dF/dt=0 and stays on one level. Since F(A)=0F(A)=0 and F(B)=e+1≠0F(B)=e+1\ne 0, no such curve can pass through both points. Equal route totals express endpoint dependence; they do not make either route a solution of the differential equation.

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Original worksheet page 2: question and worked solution for 2-3-010

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