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Identify the following surfaces: (a) \(|\mathbf{r}|=k ;\) (b) \(\mathbf{r} \cdot \mathbf{u}=l ;\) (c) \(\mathbf{r} \cdot \mathbf{u}=m|\mathbf{r}|\) for \(-1 \leq m \leq+1\); (d) \(|\mathbf{r}-(\mathbf{r} \cdot \mathbf{u}) \mathbf{u}|=n\) Here \(k\). I. \(m\) and \(n\) are fixed scalars and \(u\) is a fixed unit yector.

Short Answer

Expert verified
(a) Sphere; (b) Plane; (c) Double-napped cone; (d) Cylinder.

Step by step solution

01

Understanding part (a)

The equation \(|\mathbf{r}| = k\) represents the set of all points \(|\mathbf{r}|\) that have a distance \(k\) from the origin. This describes a sphere centered at the origin with radius \(k\).
02

Understanding part (b)

The equation \(\mathbf{r} \cdot \mathbf{u} = l\) represents the set of all points \(\mathbf{r}\) whose dot product with a fixed unit vector \(\mathbf{u}\) is \(l\). This describes a plane perpendicular to \(\mathbf{u}\) and at a distance \(l\) from the origin.
03

Understanding part (c)

The equation \(\mathbf{r} \cdot \mathbf{u} = m|\mathbf{r}|\) where \(-1 \leq m \leq +1 \,\), represents points where the dot product of \(\mathbf{r}\) and \(\mathbf{u}\) is a scaled version of the magnitude of \(\mathbf{r}\). This describes a double-napped cone with \(\mathbf{u}\) as the axis, opening at an angle depending on \(m\).
04

Understanding part (d)

The equation \(|\mathbf{r}-(\mathbf{r} \cdot \mathbf{u}) \mathbf{u}| = n\) represents points \(\mathbf{r}\) which have a constant distance \(n\) from the line spanned by \(\mathbf{u}\). This describes a cylinder with radius \(n\) and axis along the vector \(\mathbf{u}\).

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Key Concepts

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

sphere equation
Understanding the equation of a sphere is fundamental in vector calculus. A sphere can be described with the equation \(|\mathbf{r}| = k\). Here, \(|\mathbf{r}|\) stands for the magnitude of vector \(\mathbf{r}\), which is the distance from the origin to point \(\mathbf{r}\). This equation tells us that every point \(\mathbf{r}\) on the sphere is exactly distance \(k\) from the origin.
In other words, think of a sphere as a perfect ball with all its surface points equidistant from a central point (the origin). The value \(k\) is called the radius of the sphere. For example, if \(k = 5\), the sphere has a radius of 5 units.
In a more general form, for a sphere not centered at the origin, the equation is: \((x - a)^2 + (y - b)^2 + (z - c)^2 = k^2\), where \((a, b, c)\) is the center and \(k\) is the radius.
plane equation
Next, we come to the equation of a plane. A plane in vector terms can be represented by \(\mathbf{r} \cdot \mathbf{u} = l\). Here, \(\mathbf{r}\) is any point on the plane, \(\mathbf{u}\) is a fixed unit vector perpendicular to the plane (normal vector), and \(l\) is the distance from the origin to the plane.
This equation tells us that every point \(\mathbf{r}\) on the plane creates a dot product with \(\mathbf{u}\) equal to \(l\). A dot product being equal to a constant means that the angle between \(\mathbf{r}\) and \(\mathbf{u}\) is maintained but varies in magnitude, keeping them at a consistent distance.
For example, if \(\mathbf{u} = (1, 0, 0)\) and \(l = 3\), the plane equation simplifies to \(x = 3\), which is a vertical plane 3 units away from the yz-plane.
cone equation
A cone in vector calculus can be tricky but fascinating! The equation \(\mathbf{r} \cdot \mathbf{u} = m|\mathbf{r}|\) (with \(- 1 \leq m \leq +1\)) represents a double-napped cone.
In simpler terms, this equation states that the dot product of vector \(\mathbf{r}\) and unit vector \(\mathbf{u}\) is a scaled version of the magnitude of \(\mathbf{r}\). The scalar \(m\) dictates the cone’s opening angle and direction.
Imagine \(\mathbf{u}\) as the central axis of the cone. The value of \(m\) determines the slant angle of the cone from this axis. When \(m = 0\), the cone opens symmetrically around \(\mathbf{u}\). When \(m = \pm 1\), the cone's sides are infinitely spread, resembling a plane.
cylinder equation
Finally, let's discuss the equation of a cylinder. The equation for a cylinder is given by \(|\mathbf{r} - (\mathbf{r} \cdot \mathbf{u}) \mathbf{u}| = n\), where \(n\) is the radius. Here, \(\mathbf{r}\) is any point on the cylinder, \(\mathbf{u}\) is the axis vector, and \(n\) is a fixed distance from the axis.
To break it down: \(\mathbf{r} \cdot \mathbf{u}\) calculates the projection of \(\mathbf{r}\) onto \(\mathbf{u}\). Subtracting this from \(\mathbf{r}\) gives a vector orthogonal to \(\mathbf{u}\). The magnitude of this vector is constantly \(n\), meaning every point \(\mathbf{r}\) is consistently \(n\) units away from the central axis, forming a cylinder.
For example, if \(\mathbf{u}=(0,1,0)\) and \(n=2\), the cylinder has a vertical axis along the y-axis and a radius of 2 units, like a soup can standing upright.

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Most popular questions from this chapter

Prove, by writing it out in component form, that $$ (a \times b) \times c=(a \cdot c) \mathbf{b}-(b \cdot c) a $$ and deduce the result, stated in (7.25), that the operation of forming the vector product is non-associative.

For four arbitrary vectors a, b, \(\mathbf{c}\) and d, evaluate $$ (\mathbf{a} \times \mathbf{b}) \times(\mathbf{c} \times \mathbf{d}) $$ in two different ways and so prove that $$ \mathbf{a}[\mathbf{b}, \mathbf{c}, \mathbf{d}]-\mathbf{b}[\mathbf{c}, \mathbf{d}, \mathbf{a}]+\mathbf{c}[\mathbf{d}, \mathbf{a}, \mathbf{b}]-\mathbf{d}[\mathbf{a}, \mathbf{b}, \mathbf{c}]=0 $$ Show that this reduces to the normal Cartesian representation of the vector d, i.e. \(d_{x} \mathbf{i}+d_{y} \mathbf{j}+d_{z} \mathbf{k}\) if \(\mathbf{a}, \mathbf{b}\) and \(\mathbf{c}\) are taken as \(\mathbf{i}, \mathbf{j}\) and \(\mathbf{k}\), the Cartesian base vectors.

By proceeding as indicated below, prove the parallel axis theorem, which states that, for a body of mass \(M\), the moment of inertia \(I\) about any axis is related to the corresponding moment of inertia \(I_{0}\) about a parallel axis that passes through the centre of mass of the body by $$ I=I_{0}+M a_{\perp}^{2} $$ where \(a_{\perp}\) is the perpendicular distance between the two axes. Note that \(I_{0}\) can be written as $$ \int(\hat{\mathbf{n}} \times \mathbf{r}) \cdot(\mathbf{\mathbf { n }} \times \mathbf{r}) d m $$ where \(\mathbf{r}\) is the vector position, relative to the centre of mass, of the infinitesimal mass \(d m\) and \(\hat{n}\) is a unit vector in the direction of the axis of rotation. Write a similar expression for \(I\) in which \(\mathbf{r}\) is replaced by \(\mathbf{r}^{\prime}=\mathbf{r}-\mathbf{a}\), where \(\mathbf{a}\) is the vector position of any point on the axis to which \(I\) refers. Use Lagrange's identity and the fact that \(\int \mathbf{r} d m=0\) (by the definition of the centre of mass) to establish the result

The vectors \(\mathbf{a}, \mathbf{b}\) and \(\mathbf{c}\) are coplanar and related by $$ \lambda \mathbf{a}+\mu \mathbf{b}+v \mathbf{c}=0 $$ where \(\lambda, \mu, v\) are not all zero. Show that the condition for the points with position vectors \(\alpha \mathbf{a}, \beta \mathbf{b}\) and \(\gamma \mathrm{c}\) to be collinear is $$ \frac{\lambda}{\alpha}+\frac{\mu}{\beta}+\frac{v}{\gamma}=0 $$

Show that the points \((1,0,1),(1,1,0)\) and \((1,-3,4)\) lie on a straight line. Give the equation of the line in the form $$ \mathbf{r}=\mathbf{a}+\lambda \mathbf{b} $$

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