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Prove the following properties of the divergence and curl. Assume \(\mathbf{F}\) and \(\mathbf{G}\) are differentiable vector fields and \(c\) is a real number. a. \(\nabla \cdot(\mathbf{F}+\mathbf{G})=\nabla \cdot \mathbf{F}+\nabla \cdot \mathbf{G}\) b. \(\nabla \times(\mathbf{F}+\mathbf{G})=(\nabla \times \mathbf{F})+(\nabla \times \mathbf{G})\) c. \(\nabla \cdot(c \mathbf{F})=c(\nabla \cdot \mathbf{F})\) d. \(\nabla \times(c \mathbf{F})=c(\nabla \times \mathbf{F})\)

Short Answer

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Question: Prove the following properties of divergence and curl: a) \(\nabla \cdot (\mathbf{F}+\mathbf{G}) = \nabla \cdot \mathbf{F} + \nabla \cdot \mathbf{G}\) b) \(\nabla \times(\mathbf{F}+\mathbf{G}) = \nabla \times \mathbf{F}+\nabla \times\mathbf{G}\) c) \(\nabla \cdot(c \mathbf{F}) = c(\nabla \cdot \mathbf{F})\) d) \(\nabla \times(c \mathbf{F}) = c(\nabla \times \mathbf{F})\) where \(\mathbf{F}\) and \(\mathbf{G}\) are differentiable vector fields, and \(c\) is a constant.

Step by step solution

01

Property a: Divergence of the Sum

To prove this property, we will use the definition of divergence: \(\nabla \cdot(\mathbf{F}+\mathbf{G})=\frac{\partial(F_x+G_x)}{\partial x}+\frac{\partial(F_y+G_y)}{\partial y}+\frac{\partial(F_z+G_z)}{\partial z}\) Now, we will apply the properties of the partial derivative: \(\nabla \cdot(\mathbf{F}+\mathbf{G})=\left(\frac{\partial F_x}{\partial x}+\frac{\partial G_x}{\partial x}\right)+\left(\frac{\partial F_y}{\partial y}+\frac{\partial G_y}{\partial y}\right)+\left(\frac{\partial F_z}{\partial z}+\frac{\partial G_z}{\partial z}\right)\) \(\nabla \cdot(\mathbf{F}+\mathbf{G})=(\nabla \cdot \mathbf{F})+(\nabla \cdot\mathbf{G})\)
02

Property b: Curl of the Sum

To prove this property, we will use the definition of curl: \(\nabla \times(\mathbf{F}+\mathbf{G})=\det\begin{pmatrix}\hat{\imath} & \hat{\jmath} & \hat{k}\\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z}\\ F_x+G_x & F_y+G_y & F_z+G_z\end{pmatrix}\) Expand the determinant using cofactor expansion and apply properties of partial derivatives: \(\nabla \times(\mathbf{F}+\mathbf{G})=(\nabla \times \mathbf{F})+(\nabla \times \mathbf{G})\)
03

Property c: Divergence of a Scaled Vector Field

To prove this property, we will use the definition of divergence: \(\nabla \cdot(c \mathbf{F})=\frac{\partial(cF_x)}{\partial x}+\frac{\partial(cF_y)}{\partial y}+\frac{\partial(cF_z)}{\partial z}\) Now, we will apply the properties of the partial derivative and constants: \(\nabla \cdot(c \mathbf{F})=c\left(\frac{\partial F_x}{\partial x}+\frac{\partial F_y}{\partial y}+\frac{\partial F_z}{\partial z}\right)=c(\nabla \cdot \mathbf{F})\)
04

Property d: Curl of a Scaled Vector Field

To prove this property, we will use the definition of curl: \(\nabla \times(c \mathbf{F})=\det\begin{pmatrix}\hat{\imath} & \hat{\jmath} & \hat{k}\\ \frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z}\\ cF_x & cF_y & cF_z\end{pmatrix}\) Expand the determinant using cofactor expansion and apply properties of partial derivatives and constants: \(\nabla \times(c \mathbf{F})=c(\nabla \times \mathbf{F})\) We have proven all four properties using the definitions of divergence and curl.

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Most popular questions from this chapter

The gravitational force between two point masses \(M\) and \(m\) is $$ \mathbf{F}=G M m \frac{\mathbf{r}}{|\mathbf{r}|^{3}}=G M m \frac{\langle x, y, z\rangle}{\left(x^{2}+y^{2}+z^{2}\right)^{3 / 2}} $$ where \(G\) is the gravitational constant. a. Verify that this force field is conservative on any region excluding the origin. b. Find a potential function \(\varphi\) for this force field such that \(\mathbf{F}=-\nabla \varphi\) c. Suppose the object with mass \(m\) is moved from a point \(A\) to a point \(B,\) where \(A\) is a distance \(r_{1}\) from \(M\) and \(B\) is a distance \(r_{2}\) from \(M .\) Show that the work done in moving the object is $$ G M m\left(\frac{1}{r_{2}}-\frac{1}{r_{1}}\right) $$ d. Does the work depend on the path between \(A\) and \(B\) ? Explain.

Find a vector field \(\mathbf{F}\) with the given curl. In each case, is the vector field you found unique? $$\operatorname{curl} \mathbf{F}=\langle 0,1,0\rangle$$

Let \(\mathbf{F}\) be a radial field \(\mathbf{F}=\mathbf{r} /|\mathbf{r}|^{p},\) where \(p\) is a real number and \(\mathbf{r}=\langle x, y, z\rangle .\) With \(p=3, \mathbf{F}\) is an inverse square field. a. Show that the net flux across a sphere centered at the origin is independent of the radius of the sphere only for \(p=3\) b. Explain the observation in part (a) by finding the flux of \(\mathbf{F}=\mathbf{r} /|\mathbf{r}|^{p}\) across the boundaries of a spherical box \(\left\\{(\rho, \varphi, \theta): a \leq \rho \leq b, \varphi_{1} \leq \varphi \leq \varphi_{2}, \theta_{1} \leq \theta \leq \theta_{2}\right\\}\) for various values of \(p\)

The heat flow vector field for conducting objects is \(\mathbf{F}=-k \nabla T,\) where \(T(x, y, z)\) is the temperature in the object and \(k>0\) is a constant that depends on the material. Compute the outward flux of \(\mathbf{F}\) across the following surfaces S for the given temperature distributions. Assume \(k=1\). \(T(x, y, z)=100 e^{-x-y} ; S\) consists of the faces of the cube \(|x| \leq 1,|y| \leq 1,|z| \leq 1\).

The heat flow vector field for conducting objects is \(\mathbf{F}=-k \nabla T,\) where \(T(x, y, z)\) is the temperature in the object and \(k>0\) is a constant that depends on the material. Compute the outward flux of \(\mathbf{F}\) across the following surfaces S for the given temperature distributions. Assume \(k=1\). \(T(x, y, z)=100 e^{-x^{2}-y^{2}-z^{2}} ; S\) is the sphere \(x^{2}+y^{2}+z^{2}=a^{2}\).

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