/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 18 Let \(\mathbf{F}_{1}\) and \(\ma... [FREE SOLUTION] | 91Ó°ÊÓ

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Let \(\mathbf{F}_{1}\) and \(\mathbf{F}_{2}\) be differentiable vector fields and let \(a\) and \(b\) be arbitrary real constants. Verify the following identities. a. \(\nabla \cdot\left(a \mathbf{F}_{1}+b \mathbf{F}_{2}\right)=a \nabla \cdot \mathbf{F}_{1}+b \nabla \cdot \mathbf{F}_{2}\) b. \(\nabla \times\left(a \mathbf{F}_{1}+b \mathbf{F}_{2}\right)=a \nabla \times \mathbf{F}_{1}+b \nabla \times \mathbf{F}_{2}\) c. \(\nabla \cdot\left(\mathbf{F}_{1} \times \mathbf{F}_{2}\right)=\mathbf{F}_{2} \cdot \nabla \times \mathbf{F}_{1}-\mathbf{F}_{1} \cdot \nabla \times \mathbf{F}_{2}\)

Short Answer

Expert verified
Identities a, b, and c are verified using linearity and known vector calculus identities.

Step by step solution

01

Understand the Identity A

For identity a, we have to show \( abla \cdot \left(a \mathbf{F}_{1} + b \mathbf{F}_{2}\right) = a abla \cdot \mathbf{F}_{1} + b abla \cdot \mathbf{F}_{2} \). We recognize this is a distributive property of the divergence operator applied to the linear combination of vector fields.
02

Solve Identity A

Using the linearity of the divergence operator, we calculate the divergence of \( a \mathbf{F}_{1} + b \mathbf{F}_{2} \) as:\[abla \cdot (a \mathbf{F}_{1} + b \mathbf{F}_{2}) = abla \cdot (a \mathbf{F}_{1}) + abla \cdot (b \mathbf{F}_{2})\]Applying the property \( abla \cdot (c \mathbf{G}) = c abla \cdot \mathbf{G} \) for constants \(c\):\[aabla \cdot (a \mathbf{F}_{1}) + abla \cdot (b \mathbf{F}_{2}) = aabla \cdot \mathbf{F}_{1} + babla \cdot \mathbf{F}_{2}\]This proves identity a.
03

Understand the Identity B

For identity b, we are tasked to verify \( abla \times (a \mathbf{F}_{1} + b \mathbf{F}_{2}) = a abla \times \mathbf{F}_{1} + b abla \times \mathbf{F}_{2} \). This expression illustrates the distributive property of the curl operation on linearly combined vector fields.
04

Solve Identity B

By using the linearity of the curl operator, calculate:\[abla \times (a \mathbf{F}_{1} + b \mathbf{F}_{2}) = abla \times (a \mathbf{F}_{1}) + abla \times (b \mathbf{F}_{2})\]Applying \( abla \times (c \mathbf{G}) = c abla \times \mathbf{G} \) for scalar \(c\):\[aabla \times (a \mathbf{F}_{1}) + abla \times (b \mathbf{F}_{2}) = a abla \times \mathbf{F}_{1} + b abla \times \mathbf{F}_{2}\]This verifies identity b.
05

Understand the Identity C

Identity c requires verification that \( abla \cdot (\mathbf{F}_{1} \times \mathbf{F}_{2}) = \mathbf{F}_{2} \cdot abla \times \mathbf{F}_{1} - \mathbf{F}_{1} \cdot abla \times \mathbf{F}_{2} \). This is known as a common identity involving divergence and curl in vector calculus.
06

Use Known Vector Identity for C

Apply the known vector calculus identity for the divergence of a cross product:\[abla \cdot (\mathbf{F}_{1} \times \mathbf{F}_{2}) = \mathbf{F}_{2} \cdot (abla \times \mathbf{F}_{1}) - \mathbf{F}_{1} \cdot (abla \times \mathbf{F}_{2})\]Thus, the identity is directly verified using this fundamental identity from vector calculus.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Divergence
Divergence is a fundamental concept in vector calculus that measures how much a vector field spreads out or converges at a given point. Generally, for a three-dimensional vector field \( \mathbf{F} = (F_x, F_y, F_z) \), the divergence is defined by the scalar field \( abla \cdot \mathbf{F} = \frac{\partial F_x}{\partial x} + \frac{\partial F_y}{\partial y} + \frac{\partial F_z}{\partial z} \).
This operation can tell us if a point is a source, sink, or neither:
  • If the divergence is positive at a point, it can be considered a source, meaning vectors are diverging from it.
  • If it's negative, the point acts as a sink, indicating convergence to that point.
  • Zero divergence suggests no net flow in nor out of the point.
When solving vector problems, particularly those involving identities, recognize that divergence is linear. This linearity means you can find the divergence of a sum of vector fields by summing their individual divergences. This crucial property allows us to handle complex expressions with ease by breaking them down into simpler parts. Remember: recognizing patterns such as this helps in verifying textbook identities.
Curl
Curl measures the rotation or "twisting" effect of a vector field in three-dimensional space. It specifically applies to vector fields where we want to know if there is rotational motion. For a vector field \( \mathbf{F} = (F_x, F_y, F_z) \), the curl is given by: \[abla \times \mathbf{F} = \left( \frac{\partial F_z}{\partial y} - \frac{\partial F_y}{\partial z}, \frac{\partial F_x}{\partial z} - \frac{\partial F_z}{\partial x}, \frac{\partial F_y}{\partial x} - \frac{\partial F_x}{\partial y} \right)\]The result is another vector field.
  • A non-zero curl at a point suggests local rotational flow.
  • A zero curl indicates the field is irrotational there.
In the context of verifying textbook identities, the curl is likewise a linear operator. As seen in the problem, when computing the curl of sums or scalar multiples of vector fields, it behaves predictably. Knowing that operations distribute over addition—just like in simple arithmetic—simplifies calculations and lends confidence in the process.
Vector Fields
Vector fields provide a way to represent how vectors vary in space, making them essential in describing physical phenomena like fluid flow, electromagnetic fields, and more. At any given point in a space defined by a vector field, a vector represents characteristics such as direction and magnitude of the phenomenon being studied.
Understanding vector fields involves identifying component functions, visualizing the field's behavior, and performing operations like divergence and curl.
  • Regularity: Many exercises assume differentiable vector fields, ensuring smoothness and continuity, which are important for the solutions.
  • Context: Knowing about common operations like divergence and curl helps you use vector fields to model real-world scenarios with accuracy.
Grasping these aspects enables one to confidently tackle mathematical problems involving vector fields, analyze them, and understand the implications of their algebra in phenomena being modeled.

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Most popular questions from this chapter

Bendixson's criterion The streamlines of a planar fluid flow are the smooth curves traced by the fluid's individual particles. The vectors \(\mathbf{F}=M(x, y) \mathbf{i}+N(x, y) \mathbf{j}\) of the flow's velocity field are the tangent vectors of the streamlines. Show that if the flow takes place over a simply connected region \(R\) (no holes or missing points) and that if \(M_{x}+N_{y} \neq 0\) throughout \(R\) , then none of the streamlines in \(R\) is closed. In other words, no particle of fluid ever has a closed trajectory in \(R .\) The criterion \(M_{x}+N_{y} \neq 0\) is called Bendixson's criterion for the nonexistence of closed trajectories.

In Exercises \(1-6,\) use the surface integral in Stokes' Theorem to calculate the circulation of the field \(\mathbf{F}\) around the curve \(C\) in the indicated direction. \(\mathbf{F}=\left(y^{2}+z^{2}\right) \mathbf{i}+\left(x^{2}+z^{2}\right) \mathbf{j}+\left(x^{2}+y^{2}\right) \mathbf{k}\) \(C :\) The boundary of the triangle cut from the plane \(x+y+z=1\) by the first octant, counterclockwise when viewed from above

In Exercises \(25-28\) , find the circulation and flux of the field \(F\) around and across the closed semicircular path that consists of the semicircular arch \(\mathbf{r}_{1}(t)=(a \cos t) \mathbf{i}+(a \sin t) \mathbf{j}, 0 \leq t \leq \pi,\) followed by the line segment \(\mathbf{r}_{2}(t)=t \mathbf{i},-a \leq t \leq a\) $$ \mathbf{F}=-y \mathbf{i}+x \mathbf{j} $$

Conservation of mass \(\quad\) Let \(\mathbf{v}(t, x, y, z)\) be a continuously differ- entiable vector field over the region \(D\) in space and let \(p(t, x, y, z)\) be a continuously differentiable scalar function. The variable \(t\) represents the time domain. The Law of Conservation of Mass asserts that $$\frac{d}{d t} \iiint_{D} p(t, x, y, z) d V=-\iint_{S} p \mathbf{v} \cdot \mathbf{n} d \sigma$$ where \(S\) is the surface enclosing \(D\) a. Give a physical interpretation of the conservation of mass law if \(v\) is a velocity flow field and \(p\) represents the density of the fluid at point \((x, y, z)\) at time \(t .\) b. Use the Divergence Theorem and Leibniz's Rule, $$\frac{d}{d t} \iiint_{D} p(t, x, y, z) d V=\iiint_{D} \frac{\partial p}{\partial t} d V$$ to show that the Law of Conservation of Mass is equivalent to the continuity equation, $$\nabla \cdot p \mathbf{v}+\frac{\partial p}{\partial t}=0$$ (In the first term \(\nabla \cdot p \mathbf{v}\) , the variable \(t\) is held fixed, and in the second term \(\partial p / \partial t,\) it is assumed that the point \((x, y, z)\) in \(D\) is held fixed.)

In Exercises \(21-26,\) find the flux of the field \(\mathbf{F}\) across the portion of the sphere \(x^{2}+y^{2}+z^{2}=a^{2}\) in the first octant in the direction away from the origin. $$ \begin{array}{c}{\mathbf{F}(x, y, z)=x \mathbf{i}+y \mathbf{j}+z \mathbf{k}} \\\ {x \mathbf{i}+y \mathbf{j}+z \mathbf{k}}\end{array} $$

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