Conservative Vector Fields β€” Question 7

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Question 7

Suppose ff and gg are potential functions for the same continuous vector field 𝑭\mathbf F on a connected open region DD.

Tasks

  1. Prove that fβˆ’gf-g is constant on DD.

  2. Explain why connectedness is needed.

  3. State the resulting uniqueness principle for potential functions.

Original worksheet page 1: question and worked solution for 5-6-007
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Question 7 – Solution

Strategy. Subtract the two gradient equations and use paths inside the connected open region.

Step 1: Subtract gradients Since βˆ‡f=𝑭=βˆ‡g\nabla f=\mathbf F=\nabla g, βˆ‡(fβˆ’g)=𝟎.\nabla(f-g)=\mathbf 0. Let A,B∈DA,B\in D. An open connected region in ℝn\mathbb R^n is path connected, so choose a piecewise smooth curve CC in DD from AA to BB. Then (fβˆ’g)(B)βˆ’(fβˆ’g)(A)=∫Cβˆ‡(fβˆ’g)β‹…d𝒓=0.(f-g)(B)-(f-g)(A) =\int_C\nabla(f-g)\cdot d\mathbf r=0. Thus (fβˆ’g)(B)=(fβˆ’g)(A)(f-g)(B)=(f-g)(A) for every pair, and fβˆ’g=K on D.\boxed{f-g=K\text{ on }D}.

See the diagram in the original worksheet below.

Step 2: Why connectedness matters On separate components, the same zero gradient permits a different constant on each component because no path in DD joins them.

Step 3: Uniqueness principle A potential on a connected region is unique up to one additive constant. Adding a constant changes function values but leaves every partial derivative unchanged.

Verification If g=f+Kg=f+K, then βˆ‡g=βˆ‡f+βˆ‡K=βˆ‡f\nabla g=\nabla f+\nabla K=\nabla f, confirming that every additive constant really does produce another potential.

Original worksheet page 2: question and worked solution for 5-6-007

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