Chapter 8: Problem 31
Let \(\mathbf{F}=x^{2} \mathbf{i}+(2 x y+x) \mathbf{j}+z \mathbf{k} .\) Let \(C\) be the circle \(x^{2}+y^{2}=1\) and \(S\) the disc \(x^{2}+y^{2} \leq 1\) within the plane \(z=0\) (a) Determine the flux of \(\mathbf{F}\) out of \(S\) (b) Determine the circulation of \(\mathbf{F}\) around \(C\) (c) Find the flux of \(\nabla \times \mathbf{F}\). Verify Stokes' theorem directly in this case.
Short Answer
Step by step solution
Understanding the Problem
Express \( \nabla \times \mathbf{F} \)
Calculate Flux through \( S \)
Calculating Circulation around \( C \)
Verify Stokes' Theorem
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Flux Calculation
This involves using the divergence theorem, which connects the flux through a closed surface to the volume integral of the divergence of the vector field inside. Mathematically, this is defined as:
\[ \text{Flux} = \iint_{S} \mathbf{F} \cdot \mathbf{n} \, dS = \iiint_{V} (abla \cdot \mathbf{F}) \, dV \]
For this problem, since the surface \( S \) is flat, the calculations simplify significantly. We've determined that \( abla \cdot \mathbf{F} = 2x + 1 \), and due to the symmetry of the disk, the integral results in a total flux of zero.
This highlights an interesting characteristic of symmetric fields: sometimes, they may yield zero net flux across symmetric surfaces.
Circulation
The theorem states:
\[ \oint_{C} \mathbf{F} \cdot d\mathbf{r} = \iint_{S} (abla \times \mathbf{F}) \cdot \mathbf{n} \, dS \]
Where \( abla \times \mathbf{F} = - \mathbf{j} + (2y + 1) \mathbf{k} \) from our earlier calculations. The normal vector \( \mathbf{n} \) to the plane \( z = 0 \) is \( \mathbf{k} \). Thus, only the \( k \)-component of \( abla \times \mathbf{F} \) affects the integral.
The resulting integral confirms that the circulation around \( C \) is zero, which aligns perfectly with the flux calculations, demonstrating the consistency across different forms of vector analysis.
Vector Calculus
The curl \( abla \times \mathbf{F} \) tells us about the rotation or 'twist' of the field, important in calculating circulation. Meanwhile, the divergence \( abla \cdot \mathbf{F} \) measures the 'spread' of the field, critical for flux calculations.
Stokes' Theorem in vector calculus provides a profound connection between these operations. It shows how the circulation around a curve is related to the curl over a surface bounded by that curve. This fundamental theorem can simplify many calculations, turning a difficult line integral into a potentially easier surface integral or vice versa.
Understanding vector calculus is not just about calculating rates and accumulations; it’s about unlocking relationships between geometric and physical interpretations of vector fields. This exercise beautifully demonstrates these relationships via concrete calculations.