/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 66 A circular loop of wire \(50 \ma... [FREE SOLUTION] | 91Ó°ÊÓ

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A circular loop of wire \(50 \mathrm{~mm}\) in radius carries a current of \(100 \mathrm{~A}\). Find the (a) magnetic field strength and (b) energy density at the center of the loop.

Short Answer

Expert verified
(a) Magnetic field strength is 6.28 mT; (b) Energy density is 1.57 x 10^-5 J/m^3.

Step by step solution

01

Calculate Magnetic Field Strength Using Biot-Savart Law

The magnetic field strength at the center of a circular loop is given by the formula \( B = \frac{\mu_0 I}{2R} \), where \( \mu_0 = 4\pi \times 10^{-7} \; \text{T}\cdot\text{m/A} \) is the permeability of free space, \( I = 100 \; \text{A} \) is the current, and \( R = 50 \; \text{mm} = 0.05 \; \text{m} \) is the radius of the loop. Substitute these values into the formula:\[B = \frac{4\pi \times 10^{-7} \times 100}{2 \times 0.05} = \frac{4\pi \times 10^{-5}}{0.1} \text{ T}\]Evaluating the expression, we find:\[B = 2\pi \times 10^{-3} \text{ T} \approx 6.28 \times 10^{-3} \text{ T} = 6.28 \; \text{mT}\]So, the magnetic field strength at the center of the loop is \(6.28 \; \text{mT}\).
02

Calculate Energy Density of Magnetic Field

The energy density \( u \) of a magnetic field is calculated using the formula \( u = \frac{B^2}{2\mu_0} \). We have already found \( B \approx 6.28 \times 10^{-3} \; \text{T}\). Substitute this and \( \mu_0 = 4\pi \times 10^{-7} \; \text{T}\cdot\text{m/A} \) into the formula:\[u \= \frac{(6.28 \times 10^{-3})^2}{2 \times 4 \pi \times 10^{-7}} = \frac{39.4384 \times 10^{-6}}{8\pi \times 10^{-7}} \\]Simplify the calculation:\[ u = \frac{39.4384}{8\pi} \times 10^{-6} \approx 1.57 \times 10^{1} \times 10^{-6} = 1.57 \times 10^{-5} \; \frac{\text{J}}{\text{m}^3}\]Thus, the energy density at the center of the loop is \(1.57 \times 10^{-5} \; \text{J/m}^3 \).

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Key Concepts

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

Biot-Savart Law
The Biot-Savart Law is a fundamental principle in electromagnetism that helps us understand how magnetic fields are generated by electric currents. In simple terms, it shows us how the magnetic field is related to the current and the shape of the current-carrying wire.

In the context of a circular loop of wire carrying a current, this law tells us that the magnetic field at the center of the loop can be calculated by the formula:
  • \[B = \frac{\mu_0 I}{2R}\]
  • Here, \(B\) is the magnetic field strength, \(I\) is the current, \(R\) is the radius of the loop, and \(\mu_0\) is the permeability of free space.
This equation shows that the magnetic field strength at the center is directly proportional to the current and inversely proportional to the loop's radius. The Biot-Savart Law is crucial when working with circular loops as it simplifies the complexity of calculating the magnetism created by a more intricate current path.
Energy Density
Energy density in a magnetic field refers to the amount of energy stored in the field per unit volume. It's a critical concept, especially in understanding how energy is confined within a magnetic setup like inside a circular loop.

For magnetic fields, the energy density \(u\) is given by the formula:
  • \[u = \frac{B^2}{2\mu_0}\]
  • Where \(B\) is the magnetic field strength, and \(\mu_0\) is the permeability of free space.
This equation highlights that energy density increases with the square of the magnetic field strength. Because of this quadratic relationship, even small increases in magnetic field strength can significantly boost the energy density. Understanding energy density helps us know how much energy is present in a magnetic field and is vital in designing electromagnetic systems with efficiency and safety considerations.
Circular Loop
A circular loop of wire is a simple yet powerful configuration for generating magnetic fields. This loop is often used due to its symmetry and the straightforward application of laws like Biot-Savart.

The current flows along the wire, creating concentric circles of magnetic field lines. At the center of the loop, these field lines sum up to form a stronger magnetic field. This setup makes circular loops very useful in practical applications like electromagnets and inductors.

Key properties of a circular loop include:
  • The radius of the loop directly affects the magnetic field strength at its center—the smaller the radius, the stronger the field.
  • The same current flowing through a bigger loop results in a weaker magnetic field at the center.
By analyzing a circular loop, we gain insights into how magnetic fields behave in more complex looping current systems. This understanding is foundational for designing magnetic circuits.
Permeability of Free Space
The permeability of free space, denoted by \(\mu_0\), is a fundamental constant in physics that describes how a magnetic field spreads through a vacuum. It is essential for calculating magnetic fields generated by currents in free space using formulas like those provided by the Biot-Savart Law.

The value of permeability of free space is given by:
  • \[\mu_0 = 4\pi \times 10^{-7} \; \text{T}\cdot\text{m/A}\]
This constant unifies the relationships between magnetic fields and electric currents universally and also plays a crucial role in various equations of electromagnetic theory, including Ampère's Law.

Knowing \(\mu_0\) allows us to precisely calculate how an electrical current in space will influence its surroundings, providing the backbone for understanding magnetic field applications like solenoids, toroids, and more. It is a key parameter in determining how effective a medium is in supporting the formation of magnetic fields.

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Most popular questions from this chapter

A uniform magnetic field \(\vec{B}\) is perpendicular to the plane of a circular loop of diameter \(10 \mathrm{~cm}\) formed from wire of diameter \(2.5 \mathrm{~mm}\) and resistivity \(1.69 \times 10^{-8} \Omega \cdot \mathrm{m}\). At what rate must the magnitude of \(\vec{B}\) change to induce a \(10 \mathrm{~A}\) current in the loop?

Ttwo parallel loops of wire having a common axis. The smaller loop (radius \(r\) ) is above the larger loop (radius \(R\) ) by a distance \(x \geqslant R\). Consequently, the magnetic field due to the counterclockwise current \(i\) in the larger loop is nearly uniform throughout the smaller loop. Suppose that \(x\) is increasing at the constant rate \(d x / d t=v .\) (a) Find an expression for the magnetic flux through the area of the smaller loop as a function of \(x\).

Two inductors \(L_{1}\) and \(L_{2}\) are connected in series and are separated by a large distance so that the magnetic field of one cannot affect the other. (a) Show that the equivalent inductance is given by $$L_{\mathrm{eq}}=L_{1}+L_{2}$$ (Hint: Review the derivations for resistors in series and capacitors in series. Which is similar here?) (b) What is the generalization of (a) for \(N\) inductors in series?

One hundred turns of (insulated) copper wire are wrapped around a wooden cylindrical core of cross-sectional area \(1.20 \times 10^{-3} \mathrm{~m}^{2}\). The two ends of the wire are connected to a resistor. The total resistance in the circuit is \(13.0 \Omega\). If an externally applied uniform longitudinal magnetic field in the core changes from \(1.60 \mathrm{~T}\) in one direction to \(1.60 \mathrm{~T}\) in the opposite direction, how much charge flows through a point in the circuit during the change?

A wire forms a closed circular loop, of radius \(R=\) \(2.0 \mathrm{~m}\) and resistance \(4.0 \Omega\). The circle is centered on a long straight wire; at time \(t=0\), the current in the long straight wire is \(5.0 \mathrm{~A}\) rightward. Thereafter, the current changes according to \(i=5.0 \mathrm{~A}-\) \(\left(2.0 \mathrm{~A} / \mathrm{s}^{2}\right) t^{2}\). (The straight wire is insulated; so there is no electrical contact between it and the wire of the loop.) What is the magnitude of the current induced in the loop at times \(t>0\) ?

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