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A sphere of radius \(a\) and relative permeability \(\kappa_{m}\) is placed in a previously uniform magnetic field \(\mathbf{H}_{0}=H_{0} \hat{z}\). Find \(\mathbf{H}\) everywhere.

Short Answer

Expert verified
The magnetic field inside the sphere is \(\mathbf{H}=\kappa_{m} H_{0} \hat{z}\) for \(r=a\).

Step by step solution

01

Analyze the situation inside the sphere

Inside the sphere, we know the field is uniform and equals \( \mathbf{H}_{0}=H_{0} \hat{z}\). As the sphere magnetizes uniformly in the \(\hat{z}\) direction, the magnetic field inside does not change. So, the solution for the magnetic field inside the sphere is \( \mathbf{H}_{in}=\kappa_{m} \mathbf{H}_{0}= \kappa_{m} H_{0} \hat{z}.\)
02

Consider the situation outside the sphere

Outside the sphere, we understand that there is no magnetic source or sink. Hence, using the divergence property of the magnetic field, i.e., \(\nabla \cdot \mathbf{H}_{out} = 0\), we must have it that outside the sphere the field should also be \(H_{0} \hat{z}\). So, the solution for the magnetic field outside the sphere is \( \mathbf{H}_{out}=H_{0} \hat{z}.\)
03

Present the final solution

After calculating the magnetic field inside and outside the sphere, we present the full solution as follows: \(\mathbf{H}=\kappa_{m} H_{0} \hat{z}\) for \(r=a\).

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Key Concepts

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

Relative Permeability
Relative permeability is a concept in electromagnetism that relates to how a material responds to a magnetic field. It is expressed as a unitless parameter \(\kappa_{m}\) and highlights the material's ability to support the formation of a magnetic field compared to free space. If a material has a high relative permeability, it means the material allows magnetic field lines to flow through it more easily than vacuum. Conversely, a low relative permeability indicates that the material is less conducive to supporting a magnetic field.

It's essential to note that relative permeability is crucial in determining how magnetic materials react to external magnetic fields. For instance, in our example, the sphere's relative permeability \(\kappa_{m}\) affects the magnetic field inside it by scaling the initial uniform magnetic field \(\mathbf{H}_{0}\). Understanding this concept helps in predicting the changes or distribution of the magnetic field in various materials.
  • High relative permeability: material supports magnetic field well (e.g., iron).
  • Low relative permeability: material does not support magnetic field as well (e.g., non-magnetic materials).
By analyzing \(\kappa_{m}\), we can determine important properties about the interaction between a material and a magnetic field.
Uniform Magnetic Field
A uniform magnetic field is characterized by having the same magnitude and direction at every point. In this exercise, a uniform magnetic field \(\mathbf{H}_{0} = H_{0} \hat{z}\) is established in the direction of the \hat{z}\-axis. This means that its strength and orientation remain constant throughout the space around and inside the sphere before considering any modifications by the sphere.

This consistency simplifies the analysis of magnetic fields, especially when determining the field inside objects such as our sphere. Within the sphere, given its relative permeability, the uniform magnetic field modifies by simply scaling with \(\kappa_{m}\). Since the field is uniform, both inside and outside the sphere, problem-solving involves straightforward calculations of magnetic intensity based on known parameters.
  • Beneficial for simplifying magnetic field calculations.
  • Assumes no external disturbances affect the field’s consistency and direction.
Maintaining a uniform field allows a clear approach to understanding magnetic interactions within varying materials and conditions.
Divergence Property of Magnetic Field
The divergence property of a magnetic field is a fundamental characteristic that describes how magnetic fields behave in a region. Mathematically, it's expressed as \(abla \cdot \mathbf{H} = 0\) in a sourceless region. This tells us that within a given volume of space, magnetic field lines do not converge or diverge; they maintain a consistent flow.

In the context of the exercise, this property explains why the magnetic field outside the sphere remains as \(\mathbf{H}_{0} = H_{0} \hat{z}\). Because there are no magnetic charges acting as sources or sinks, the magnetic field's divergence is zero, leading to a uniform field beyond the sphere.
  • No accumulation of magnetic field lines in a vacuum.
  • Helps determine field behavior in complex material arrangements.
Understanding the divergence property reinforces how we can predict magnetic field behavior and aids in constructing scientific models of magnetostatics accurately.

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Most popular questions from this chapter

A very long straight current \(I\) is parallel to the plane surface of a semiinfinite li.h. magnetic material and a distance \(d\) from it. Show that the magnetic field in the vacuum region can be obtained as the resultant of this current and an image current \(I^{\prime}=I\left(\kappa_{m}-1\right) /\left(\kappa_{m}+1\right)\) located a distance \(d\) inside the material. Find the current \(I^{\prime \prime}\), which will give the correct value of \(\mathbf{H}\) within the material if it is located at the same position as I. What is the force per unit length between \(I\) and the material? Is this force attractive or repulsive?

An electromagnet is made in the form of a torus with a rectangular cross section. The width of the cross section is 2 centimeters, while the inner and outer radii are 7 and 8 centimeters. The coil has 1000 turns and has a gap cut into the core of length \(0.25\) millimeters. When the flux produced in the ring is \(2.60 \times 10^{-4}\) webers, the permeability of the core is \(4250 \mu_{0}\). Find the induction, the reluctance, the current in the windings, the magnetic field in the gap and in the iron core, and the fraction of the total magnetomotive force that is "across" the gap.

A spherical shell of radii \(a\) and \(b\) has a relative permeability \(\kappa_{m}\) for \(a \leq r \leq b\). There is vacuum everywhere else. It is placed in a previously uniform magnetic field \(\mathbf{H}_{0}=H_{0} \hat{\mathbf{z}}\). Show that the "shielding factor," that is, the ratio \(H_{i} / H_{0}\) where \(H_{i}\) is the magnetic field in the cavity, is given by \(9 \kappa_{m}\left[\left(\kappa_{m}+2\right)\left(2 \kappa_{m}+1\right)\right.\) \(\left.2\left(\kappa_{m}-1\right)^{2}(a / b)^{3}\right]^{-1} .\)

A sphere of radius \(a\) has its center at the origin. Its magnetization is nonuniform and given by \(\mathbf{M}=\left(\alpha z^{2}+\beta\right) \hat{\mathbf{z}}\) where \(\alpha\) and \(\beta\) are constants. What are the units of \(\alpha\) and \(\beta ?\) Find the magnetization current densities \(\mathbf{J}_{m}\) and \(\mathbf{K}_{m}\) as expressed in spherical coordinates.

When you look up susceptibilities in tables, you will not generally find numerical values of \(\chi_{m}\). Instead, one usually finds either the mass susceptibility \(\chi_{m, \text { mass }}\) or the molar susceptibility \(\chi_{m, \text { molar }}\). These are defined so that \(\chi_{m, \text { mass }} H\) and \(\chi_{m, \text { molar }} H\) give the magnetic moment per unit mass and per mole, respectively. Find how \(\chi_{m}\) is related to each of these; you will need to use the symbols for the mass density \(d\) and molecular weight \(A\) as well.

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