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Helmholtz coils One way to produce a very uniform magnetic field is to use a very long solenoid and work only in the middle section of its interior. This is often inconvenient, wasteful of space and power. Can you suggest ways in which two short coils or current rings might be arranged to achieve good uniformity over a limited region? Hint: Consider two coaxial current rings of radius \(a\), separated axially by a distance \(b\). Investigate the uniformity of the field in the vicinity of the point on the axis midway between the two coils. Determine the magnitude of the coil separation \(b\) that for given coil radius \(a\) will make the field in this region as nearly uniform as possible.

Short Answer

Expert verified
By arranging two coils of radius \(a\) coaxially and separating them by a distance of \(b = \sqrt{3}a\), a nearly uniform magnetic field can be achieved in a limited region.

Step by step solution

01

Biot-Savart law calculation

Use the Biot-Savart law to calculate the magnetic field \(B\) due to a single coil at a point on the axis. This is given by:\[B = \frac{\mu_0 I a^2}{2(a^2+x^2)^{3/2}}\] Where \(\mu_0\) is the magnetic constant (also known as the permeability of free space), \(I\) is the current, \(a\) is the radius of the coils, and \(x\) is the distance from the coil along the axis.
02

Magnetic field for two coils

We need to add the contribution of the second coil. The total magnetic field at a point \(P\) half way between the coils is double of the expression from Step 1 with \(x = \frac{b}{2}\). Therefore, the expression for \(B\) becomes: \[B = \frac{\mu_0 I a^2}{2(a^2+(b/2)^2)^{3/2}}\]
03

Differentiate and find minimum

To find the value of \(b\) that gives the most uniform field possible (i.e., the minimum value of \(B\)), we differentiate the expression for \(B\) from Step 2 with respect to \(b\) and set it to 0. Solving, \[b = \sqrt{3}a\]

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Key Concepts

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

Magnetic Field
A magnetic field is an invisible force that exerts influence on particles or objects that are in motion within the field. They are produced by moving electric charges, such as current flowing through a wire. A compass needle or other magnetic materials are affected by this field, showing its direction and relative strength. Magnetic fields are represented by magnetic field lines, which indicate the direction a north pole would move in the field. The strength of the magnetic field ( B ) can vary depending on the source of the field.

In the context of Helmholtz coils, the goal is often to create a magnetic field that is uniform over a specific area. A uniform magnetic field has the same strength and direction at every point in the chosen region. Challenges arise when trying to maintain uniformity of the magnetic field, as the field tends to weaken and change direction over larger distances from the source.
Biot-Savart Law
The Biot-Savart Law helps us understand the magnetic field created by a current-carrying wire. It provides a way to calculate the magnitude and direction of the magnetic field produced by a small segment of current-carrying wire. The law is expressed mathematically, showing how the magnetic field depends on factors like the strength of the current, the distance from the wire, and the angle between the wire and the point where the field is being measured:

\[ B = \frac{\mu_0 I a^2}{2(a^2+x^2)^{3/2}} \]

Here, \( \mu_0 \) is the permeability of free space, \( I \) is the current, \( a \) is the radius, and \( x \) is the distance along the axis from the wire. This calculation is crucial for designing systems like Helmholtz coils, where the magnetic field needs to be known and controlled accurately.
  • The Biot-Savart Law applies to any conductive path, from straight wires to complex coil systems.
  • For Helmholtz coils, it helps estimate how the magnetic fields from each coil combine and whether they form a uniform field.
Uniformity
Uniformity in a magnetic field is essential for experiments and technologies that require consistent force across a defined area. Such uniform fields are invaluable in fields like nuclear magnetic resonance (NMR) and in various physics experiments. Achieving a uniform magnetic field can be tricky since the field naturally decreases in strength and changes direction as one moves away from the source.

Helmholtz coils are specially designed to improve the uniformity of a magnetic field within a defined space. By carefully optimizing the spacing between two parallel coils, the field in the area between them becomes more uniform. For Helmholtz coils, this spacing is usually set to nearly equal the radius of the coils, which is mathematically approximated by the relation\[ b = \sqrt{3}a \]where \( b \) is the separation distance between the coils and \( a \) is their radius.
  • This setup minimizes variations in the magnetic field.
  • Uniform fields are crucial for precise measurements and sensitive experiments.
Solenoids
Solenoids are coils of wire that generate a magnetic field when an electric current passes through them. They are often used to create controlled and uniform magnetic fields in their interior regions. This makes solenoids particularly useful in devices like electromagnets and electric motors.

The challenge with long solenoids is that while they provide a uniform field, they require substantial space and resources. Helmholtz coils, being a type of solenoid, circumvent this issue by using two coils arranged parallel and coaxially. Placing these coils at a distance equal to their radius creates a highly uniform field in their center, without needing the length of a single large solenoid:
  • Solenoids rely on the principle of electromagnetic induction.
  • They convert electric energy into magnetic energy efficiently.
  • Helmholtz coils are essentially short solenoids, optimized for specific use-cases.

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Most popular questions from this chapter

A slab and a sheet \(* *\) A volume current density \(\mathbf{J}=J \hat{\mathbf{z}}\) exists in a slab between the infinite planes at \(x=-b\) and \(x=b\). (So the current is coming out of the page in Fig. 6.37.) Additionally, a surface current density \(\mathcal{J}=2 b J\) points in the \(-\hat{\mathbf{z}}\) direction on the plane at \(x=b\) (a) Find the magnetic field as a function of \(x\), both inside and outside the slab. (b) Verify that \(\nabla \times \mathbf{B}=\mu_{0} \mathbf{J}\) inside the slab. (Don't worry about the boundaries.)

Field at the tip of a cone \(* *\) A hollow cone (like a party hat) has vertex angle \(2 \theta\), slant height \(L\), and surface charge density \(\sigma\). It spins around its symmetry axis with angular frequency \(\omega\). What is the magnetic field at the tip?

Zero force in any frame \(* *\) A neutral wire carries current \(I\). A stationary charge is nearby. There is no electric field from the neutral wire, so the electric force on the charge is zero. And although there is a magnetic field, the charge isn't moving, so the magnetic force is also zero. The total force on the charge is therefore zero. Hence it must be zero in every other frame. Verify this, in a particular case, by using the Lorentz transformations to find the \(\mathbf{E}\) and \(\mathbf{B}\) fields in a frame moving parallel to the wire with velocity \(\mathbf{v}\).

Fields in a new frame \(*\) * In the neighborhood of the origin in the coordinate system \(x, y\), \(z\), there is an electric field \(\mathbf{E}\) of magnitude \(100 \mathrm{~V} / \mathrm{m}\), pointing in a direction that makes angles of \(30^{\circ}\) with the \(x\) axis, \(60^{\circ}\) with the \(y\) axis. The frame \(F^{\prime}\) has its axes parallel to those just described, but is moving, relative to the first frame, with a speed \(0.6 c\) in the positive \(y\) direction. Find the direction and magnitude of the electric field that will be reported by an observer in the frame \(F^{\prime}\). What magnetic field does this observer report?

The retarded potential \(* * *\) A point charge \(q\) moves with speed \(v\) along the line \(y=r\) in the \(x y\) plane. We want to find the magnetic field at the origin at the moment the charge crosses the \(y\) axis. (a) Starting with the electric field in the charge's frame, use the Lorentz transformation to show that, in the lab frame, the magnitude of the magnetic field at the origin (at the moment the charge crosses the \(y\) axis) equals \(B=\left(\mu_{0} / 4 \pi\right)\left(\gamma q v / r^{2}\right)\) (b) Use the Biot-Savart law to calculate the magnetic field at the origin. For the purposes of obtaining the current, you may assume that the "point" charge takes the shape of a very short stick. You should obtain an incorrect answer, lacking the \(\gamma\) factor in the above correct answer. (c) The Biot-Savart method is invalid because the Biot-Savart law holds for steady currents (or slowly changing ones, but see Footnote 8 ). But the current due to the point charge is certainly not steady. At a given location along the line of the charge's motion, the current is zero, then nonzero, then zero again. For non-steady currents, the validity of the Biot-Savart law can be restored if we use the so-called "retarded time." \(^{\prime 11}\) The basic idea with the retarded time is that, since information can travel no faster than the speed of light, the magnetic field at the origin, at the moment the charge crosses the \(y\) axis, must be related to what the charge was doing at an earlier time. More precisely, this earlier time (the "retarded time") is the time such that if a light signal were emitted from the charge at this time, then it would reach the origin at the same instant the charge crosses the \(y\) axis. Said in another way, if someone standing at the origin takes a photograph of the surroundings at the moment the charge crosses the \(y\) axis, then the position of the charge in the photograph (which will not be on the \(y\) axis) is the charge's location we are concerned with. \(^{12}\)

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