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Scaled-up ring \(*\) Consider two circular rings of copper wire. One ring is a scaled-up version of the other, twice as large in all regards (radius, crosssectional radius). If currents around the rings are driven by equal voltage sources, how do the magnetic fields at the centers compare?

Short Answer

Expert verified
The magnetic field at the center of the larger ring is half as much as at the center of the smaller ring.

Step by step solution

01

Understand the Biot-Savart Law

Biot-Savart law states that the magnetic field \( dB \) at point \( P \) due to an element \( dl \) carrying current \( I \) at a distance \( r \) is given as \( dB = \frac{{\mu I dl sin \theta}}{{4\pi r^2}} \) , where \( \mu \) is the permeability of the medium, \( \theta \) is the angle between \( dl \) and \( r \) and \(\mu = 4\pi \times 10^{-7} T m/A \)
02

Apply the Biot-Savart Law

In the current scenario, both rings have the same current due to the equal voltage sources. The magnetic field at the center is given by integrating \( dB \) over the entire circle, which simplifies to \( B = \frac{{\mu I r}}{{2 r^2}} = \frac{{\mu I}}{{2r}} \) since the cosine of the angle for the center of the ring is 1.
03

Compare the Magnetic Fields

We will denote \( B_1 \) and \( B_2 \) as magnetic fields of the smaller and larger ring respectively. Then \( B_2 = \frac{{\mu I}}{{2(2r)}} = \frac{{B_1}}{{2}} \). Hence, the magnetic field at the center of the larger ring is half of that of the smaller ring.

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Key Concepts

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

Magnetic Field
The magnetic field is a vector field that permeates space and describes the magnetic influence on moving electric charges, magnetic materials, and charged particles.

When electric current flows through a conductor, such as a wire, it generates a magnetic field around it. This field can be visualized as a pattern of circular lines surrounding the wire. The direction of these lines is given by the right-hand rule: if you point the thumb of your right hand in the direction of the current, your fingers will curl in the direction of the magnetic field lines.

The strength of the magnetic field produced depends on the magnitude of the current, the distance from the conductor, and the nature of the surrounding medium, which influences how the field propagates through space.
Circular Wire Rings
Circular wire rings are essentially coils of wire in the shape of a circle. In the context of generating magnetic fields, these rings are important because the cumulative effect of the current passing through each segment of wire strengthens the magnetic field at the center of the ring.

Role of Geometry in Magnetic Fields

One interesting aspect of circular wire rings is how their geometry affects the magnetic field produced at their center.
For example, let's consider a ring with current flowing through it. According to the Biot-Savart Law, each infinitesimal segment of the wire contributes to the magnetic field at the center. Since each segment is equidistant from the center in a perfect circle, the contributions add up uniformly, leading to a relatively strong and uniform magnetic field at the center of the ring.
Permeability of the Medium
The permeability of the medium, usually denoted by the Greek letter \( \mu \) in the Biot-Savart Law, describes how well a material supports the formation of a magnetic field within it. This property affects the strength and distribution of the magnetic field generated by a current.

Simplified, one can think of \( \mu \) as an indicator of the 'magnetic conductivity' of the material through which the field spreads. In a vacuum, the permeability is defined as the constant \( 4\pi \times 10^{-7} \, T\cdot m/A \) (tesla meter per ampere). In more magnetic materials, such as iron, the permeability is much higher, which means they can produce stronger magnetic fields with the same current.

Variation with Different Materials

Different materials have different permeabilities, and this can significantly alter the resulting magnetic field around a conductor. For instance, wrapping a wire ring with a ferromagnetic core can greatly intensify the magnetic field compared to a ring in air or a vacuum, due to the core material's high permeability. Understanding permeability is crucial in designing electromagnets and in various electrical engineering and physics applications.

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Most popular questions from this chapter

Proton beam \(* *\) A high-energy accelerator produces a beam of protons with kinetic energy \(2 \mathrm{GeV}\) (that is, \(2 \cdot 10^{9} \mathrm{eV}\) per proton). You may assume that the rest energy of a proton is \(1 \mathrm{GeV}\). The current is 1 milliamp, and the beam diameter is \(2 \mathrm{~mm}\). As measured in the laboratory frame: (a) what is the strength of the electric field caused by the beam \(1 \mathrm{~cm}\) from the central axis of the beam? (b) What is the strength of the magnetic field at the same distance? (c) Now consider a frame \(F^{\prime}\) that is moving along with the protons. What fields would be measured in \(F^{\prime}\) ?

Integral of \(A\), flux of \(B\) Show that the line integral of the vector potential \(\mathbf{A}\) around a closed curve \(C\) equals the magnetic flux \(\Phi\) through a surface \(S\) bounded by the curve. This result is very similar to Ampère's law, which says that the line integral of the magnetic field \(\mathbf{B}\) around a closed curve \(C\) equals (up to a factor of \(\mu_{0}\) ) the current flux \(I\) through a surface \(S\) bounded by the curve.

Field at the center of a disk * A disk with radius \(R\) and surface charge density \(\sigma\) spins with angular frequency \(\omega\). What is the magnetic field at the center?

Motion in \(E\) and B fields \(* * *\) The task of Exercise \(6.29\) is to show that if a charged particle moves in the \(x y\) plane in the presence of a uniform magnetic field in the \(z\) direction, the path will be a circle. What does the path look like if we add on a uniform electric field in the \(y\) direction? Let the particle have mass \(m\) and charge \(q\). And let the magnitudes of the electric and magnetic fields be \(E\) and \(B\). Assume that the velocity is nonrelativistic, so that \(\gamma \approx 1\) (this assumption isn't necessary in Exercise 6.29, because \(v\) is constant there). Be careful, the answer is a bit counterintuitive.

Field from an infinite wire \(* *\) Use the Biot-Savart law to calculate the magnetic field at a distance \(b\) from an infinite straight wire carrying current \(I\).

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