Problem 11
Question
Inductance of a Solenoid. A long, straight solenoid has \(N\) turms, uniform cross-sectional area \(A,\) and length \(l .\) Show that the inductance of this solenoid is given by the equation \(L=\mu_{0} A N^{2} / L\) Assume that the magnetic field is uniform inside the solenoid and zero outside. (Your answer is approximate because \(B\) is actually smaller at the ends than at the center. For this reason, your answer is actually an upper limit on the inductance.)
Step-by-Step Solution
Verified Answer
The inductance of the solenoid is \(L = \mu_0 A N^2 / l\).
1Step 1: Understand the Problem
We need to find the inductance \( L \) of a solenoid, which is characterized by its number of turns \( N \), cross-sectional area \( A \), and length \( l \). The inductance formula given is \( L = \mu_0 AN^2/l \). Here, \( \mu_0 \) is the magnetic constant or permeability of free space. The goal is to derive this formula based on the properties of the solenoid.
2Step 2: Identify the Magnetic Field
The magnetic field inside a long solenoid is given by the formula \( B = \mu_0 n I \), where \( n = \frac{N}{l} \) is the number of turns per unit length, and \( I \) is the current flowing through the solenoid. So, \( B = \mu_0 \frac{N}{l} I \).
3Step 3: Calculate the Magnetic Flux
The magnetic flux through one turn of the solenoid is \( \Phi = B \cdot A = (\mu_0 \frac{N}{l} I) \cdot A \). Since the solenoid has \( N \) turns, the total magnetic flux linkage is \( \lambda = N \Phi = \mu_0 \frac{N^2}{l} A I \).
4Step 4: Relate Flux Linkage to Inductance
The inductance \( L \) is defined as the ratio of the total magnetic flux linkage \( \lambda \) to the current \( I \). Thus, \( L = \frac{\lambda}{I} = \frac{\mu_0 N^2 A}{l} \). This matches the given formula for the inductance of the solenoid.
Key Concepts
Magnetic FieldMagnetic FluxPermeability of Free Space
Magnetic Field
A magnetic field is an invisible force field that surrounds a magnetic object or electrical current. It is a vector field, which means it has both direction and magnitude. In the context of a solenoid, which is a coil of wire, the magnetic field inside is due to the flow of electric current through the wire coils. This field can be calculated using the formula for a solenoid:
Remember, the assumption of zero magnetic field outside is simplification for calculations and is termed as the ideal behavior of long solenoids.
- The magnetic field inside a solenoid: \( B = \mu_0 \frac{N}{l} I \),where \( \mu_0 \) represents the permeability of free space, \( N \) is the number of turns, \( l \) is the length of the solenoid, and \( I \) is the current.
Remember, the assumption of zero magnetic field outside is simplification for calculations and is termed as the ideal behavior of long solenoids.
Magnetic Flux
Magnetic flux quantifies the amount of magnetic field passing through a surface area. It tells us how much field lines penetrate a certain area, expressed with the formula:
Each turn contributes to the overall linkage, enhancing the total field through the solenoid's core.
- Magnetic flux, \( \Phi = B \cdot A \), where \( B \) is the magnetic field and \( A \) is the area perpendicular to the field.
Each turn contributes to the overall linkage, enhancing the total field through the solenoid's core.
Permeability of Free Space
Permeability of free space, often represented as \( \mu_0 \), is a constant that measures the ability of a vacuum to allow the formation of a magnetic field. In SI units, it is valued at approximately \( 4\pi \times 10^{-7} \, \text{T}\cdot\text{m/A} \) (Tesla meter per Ampere). This constant is crucial in calculating the inductance of a solenoid because it directly relates magnetic field strength to current and coil geometry. It's used in the inductance formula:
- Inductance \( L = \mu_0 \frac{N^2 A}{l} \), emphasizing how magnetic flux density not only depends on the solenoid's material and construction but also on this universal constant.
Other exercises in this chapter
Problem 7
At the instant when the current in an inductor is increasing at a rate of 0.0640 \(\mathrm{A} / \mathrm{s}\) , the magnitude of the self-induced emf is 0.0160 \
View solution Problem 8
When the current in a toroidal solenoid is changing at a rate of 0.0260 \(\mathrm{A} / \mathrm{s}\) , the magnitude of the induced emf is 12.6 \(\mathrm{mV}\) .
View solution Problem 12
An inductor used in a de power supply has an inductance of 12.0 \(\mathrm{H}\) and a resistance of \(180 \Omega .\) It carries a current of 0.300 \(\mathrm{A}\)
View solution Problem 13
An air-filled toroidal solenoid has a mean radius of 15.0 \(\mathrm{cm}\) and a cross-sectional area of \(5.00 \mathrm{cm}^{2} .\) When the current is 12.0 \(\m
View solution