Chapter 17: Problem 13
Sketch the following vector fields. $$\mathbf{F}=\langle x,-y\rangle$$
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Chapter 17: Problem 13
Sketch the following vector fields. $$\mathbf{F}=\langle x,-y\rangle$$
These are the key concepts you need to understand to accurately answer the question.
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Surface integrals of vector fields Find the flux of the following vector fields across the given surface with the specified orientation. You may use either an explicit or a parametric description of the surface. \(\mathbf{F}=\langle-y, x, 1\rangle\) across the cylinder \(y=x^{2},\) for \(0 \leq x \leq 1\) \(0 \leq z \leq 4 ;\) normal vectors point in the general direction of the positive y-axis.
Maximum surface integral Let \(S\) be the paraboloid \(z=a\left(1-x^{2}-y^{2}\right),\) for \(z \geq 0,\) where \(a>0\) is a real number. Let \(\mathbf{F}=\langle x-y, y+z, z-x\rangle .\) For what value(s) of \(a\) (if any) does \(\iint_{S}(\nabla \times \mathbf{F}) \cdot \mathbf{n} d S\) have its maximum value?
Prove that for a real number \(p\) with \(\mathbf{r}=\langle x, y, z\rangle, \nabla \cdot \nabla\left(\frac{1}{|\mathbf{r}|^{p}}\right)=\frac{p(p-1)}{|\mathbf{r}|^{p+2}}\).
Streamlines are tangent to the vector field Assume the vector field \(\mathbf{F}=\langle f, g\rangle\) is related to the stream function \(\psi\) by \(\psi_{y}=f\) and \(\psi_{x}=-g\) on a region \(R .\) Prove that at all points of \(R,\) the vector field is tangent to the streamlines (the level curves of the stream function).
Ampère's Law The French physicist André-Marie Ampère \((1775-1836)\) discovered that an electrical current \(I\) in a wire produces a magnetic field \(\mathbf{B}\). A special case of Ampère's Law relates the current to the magnetic field through the equation \(\oint_{C} \mathbf{B} \cdot d \mathbf{r}=\mu I,\) where \(C\) is any closed curve through which the wire passes and \(\mu\) is a physical constant. Assume the current \(I\) is given in terms of the current density \(\mathbf{J}\) as \(I=\iint_{S} \mathbf{J} \cdot \mathbf{n} d S,\) where \(S\) is an oriented surface with \(C\) as a boundary. Use Stokes' Theorem to show that an equivalent form of Ampere's Law is \(\nabla \times \mathbf{B}=\mu \mathbf{J}\).
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