Topics
Electrostatics
Electric Charges and Fields
- Electric Charges
- Conductors and Insulators
- Properties of Electric Charge
- Coulomb’s Law
- Forces between Multiple Charges
- Electric Field
- Electric Field Due to a System of Charges
- Physical Significance of Electric Field
- Electric Field Lines
- Electric Flux
- Electric Dipole
- Dipole in a Uniform External Field
- Continuous Charge Distribution
- Gauss’s Law
- Application of Gauss' Law
Current Electricity
Electrostatic Potential and Capacitance
- Electric Potential and Potential Energy
- Electrostatic Potential
- Electric Potential Due to a Point Charge
- Potential Due to an Electric Dipole
- Potential due to a System of Charges
- Equipotential Surfaces
- Relation Between Electric Field and Electrostatic Potential
- Potential Energy of a System of Charges
- Potential Energy of a Single Charge
- Potential Energy of a System of Two Charges in an External Field
- Potential Energy of a Dipole in an External Field
- Electrostatics of Conductors
- Dielectrics and Polarisation
- Capacitors and Capacitance
- The Parallel Plate Capacitor
- Effect of Dielectric on Capacitance
- Combination of Capacitors
- Energy Stored in a Charged Capacitor
Magnetic Effects of Current and Magnetism
Current Electricity
- Electric Current
- Electric Currents in Conductors
- Ohm's Law
- Drift of Electrons and the Origin of Resistivity
- Mobility of Electrons
- Limitations of Ohm’s Law
- Resistivity of Various Materials
- Temperature Dependence of Resistivity
- Electrical Energy and Power in Conductors
- Cells, EMF, and Internal Resistance
- Cells in Series and in Parallel
- Kirchhoff’s Laws
- Wheatstone Bridge
Moving Charges and Magnetism
- Electromagnetism
- Magnetic force
- Motion in a Magnetic Field
- Magnetic Field Due to a Current-carrying Conductor: Biot-savart's Law
- Applications of Biot-Savart's Law > Magnetic Field at the Axis of a Circular Current-carrying Loop
- Ampere’s Circuital Law
- Solenoid
- Force Between Two Parallel Currents (Ampere’s Law)
- Torque on a Rectangular Current Loop in a Uniform Magnetic Field
- Circular Current Loop as a Magnetic Dipole
- Moving Coil Galvanometer
- Kirchhoff’s Laws
Electromagnetic Induction and Alternating Currents
Magnetism and Matter
Electromagnetic Waves
Optics
Electromagnetic Induction
Alternating Current
Dual Nature of Radiation and Matter
Atoms and Nuclei
Electromagnetic Waves
Ray Optics and Optical Instruments
- Ray Optics Or Geometrical Optics
- Reflection of Light by Spherical Mirrors
- Sign Convention for Reflection by Spherical Mirrors
- Focal Length of Spherical Mirrors
- Mirror Equation of Spherical Mirrors
- Refraction of Light
- Total Internal Reflection
- Applications of Total Internal Reflection
- Refraction at a Spherical Surfaces
- Refraction by a Lens
- Power of a Lens
- Combined Focal Length of Two Thin Lenses in Contact
- Refraction of Light through a Prism
- Introduction to Optical Instruments
- Microscope and it’s types
- Telescope
Electronic Devices
Communication Systems
Wave Optics
- Introduction to Wave Optics
- Huygens Principle
- Refraction of a Plane Wave
- Refraction at a Rarer Medium
- Reflection of a Plane Wave by a Plane Surface
- Coherent and Incoherent Addition of Waves
- Interference of Light Waves and Young’s Experiment
- Diffraction of Light
- The Single Slit
- Seeing the Single Slit Diffraction Pattern
- Polarisation of Light
The Special Theory of Relativity
Dual Nature of Radiation and Matter
- Understanding Dual Nature of Radiation and Matter
- Electron Emission
- Photoelectric Effect - Hertz’s Observations
- Photoelectric Effect - Hallwachs’ and Lenard’s Observations
- Experimental Study of Photoelectric Effect
- Effects of Intensity and Frequency on Photocurrent
- Photoelectric Effect and Wave Theory of Light
- Einstein’s Photoelectric Equation: Energy Quantum of Radiation
- Particle Nature of Light: The Photon
- Wave Nature of Matter
Atoms
Nuclei
Semiconductor Electronics - Materials, Devices and Simple Circuits
Communication Systems
- Detection of Amplitude Modulated Wave
- Production of Amplitude Modulated Wave
- Basic Terminology Used in Electronic Communication Systems
- Sinusoidal Waves
- Modulation and Its Necessity
- Amplitude Modulation (AM)
- Need for Modulation and Demodulation
- Satellite Communication
- Propagation of EM Waves
- Bandwidth of Transmission Medium
- Bandwidth of Signals
The Special Theory of Relativity
- The Special Theory of Relativity
- The Principle of Relativity
- Maxwell'S Laws
- Kinematical Consequences
- Dynamics at Large Velocity
- Energy and Momentum
- The Ultimate Speed
- Twin Paradox
Definition: Solenoid
A long solenoid is a coil whose length is much greater than its radius, producing a uniform magnetic field inside and nearly zero field outside.
OR
A solenoid is a long helical coil of insulated wire with many closely spaced turns, whose length l is much greater than its radius R (i.e., l ≫ R), such that it produces a strong, uniform magnetic field inside and a negligible field outside.
Formula: Magnetic Field Inside a Long Solenoid
B = μ0nI
Where:
- μ0 = permeability of free space
- n = number of turns per unit length
- I = current
Construction
- A solenoid consists of a long cylindrical former (can be air-core, iron-core, or insulating rod).
- Enamelled copper wire is wound tightly in helical turns — insulation prevents short-circuiting between adjacent turns.
- Total turns: N; Length: l; Turns per unit length: n = \[\frac {N}{l}\]
- When current I flows → magnetic field is produced inside the windings.
Working Principle
- Each turn of the solenoid acts as a small current loop, producing a small magnetic field along the axis.
- In a long solenoid, the individual fields of each turn superpose constructively along the axis → uniform field inside.
- Outside the solenoid, fields from adjacent turns are in opposite directions and cancel → field ≈ 0 outside.
- The net effect: the solenoid behaves like a bar magnet with polarity determined by the direction of current (Right-Hand Thumb Rule).
Derivation of Magnetic Field Using Ampere's Law
Step 1 -S Set up the Amperian Loop:
Consider a rectangular Amperian loop abcd of length l, with side ab inside the solenoid (along the axis) and side cd outside.
Step 2 - Evaluate \[\oint\vec{B}\cdot d\vec{l}\] for each side:
| Side | Condition | Contribution |
|---|---|---|
| ab (inside, along axis) | \[\vec B\] || \[d\vec l\] | Bl |
| bc (perpendicular, inside→outside) | \[\vec B\] ⊥ \[d\vec l\] | 0 |
| cd (outside solenoid) | Boutside ≈ 0 | 0 |
| da (perpendicular, outside→inside) | \[\vec B\] ⊥ \[d\vec l\] | 0 |
\[\therefore\oint\vec{B}\cdot d\vec{l}\] = Bl
Step 3 - Calculate the enclosed current:
Number of turns inside loop = nl
∴ Total enclosed current = Ienc = n ⋅ l ⋅ I
Step 4 - Apply Ampere's Law:
Special Cases
| Location | Magnetic Field | Reason |
|---|---|---|
| Inside (ideal/infinite solenoid) | B = μ0nI | Superposition of all turns |
| At the ends (edge) | B = \[\frac {μ_0nI}{2}\] | Only half the turns contribute |
| Outside | B ≈ 0 | Cancellation of adjacent fields |
| With an iron core | B = μ0μrnI | Core amplifies permeability |
Solenoid vs. Toroid
| Feature | Solenoid | Toroid |
|---|---|---|
| Shape | Long straight cylinder | Solenoid bent into a closed ring (doughnut) |
| Field inside | B = μ0nI (uniform) | B = \[\frac {μ_0NI}{2πr}\] (varies with r) |
| Field outside | B ≈ 0 (not exactly zero) | B = 0 (exactly zero) |
| Field at ends | B = \[\frac {μ_0nI}{2}\] | No ends (closed loop) |
| Uniformity | Uniform inside (away from ends) | Not uniform; depends on radius |
| Application | Electromagnets, relays, MRI | Inductors, transformers, RF circuits |
Applications
- MRI Machines — superconducting solenoids produce the powerful, stable magnetic field required for imaging.
- Electric Motors and Generators — solenoids create the rotating magnetic fields needed for motor operation.
- Solenoid Valves — used in hydraulic and pneumatic systems to control fluid flow (e.g., washing machines, car engines).
- Circuit Breakers / Relays — electromagnetic solenoids open/close switches on detecting fault current.
- Hard Disks and Loudspeakers — solenoid-based actuators position read/write heads and drive speaker cones.
Example
Given:
-
Length of solenoid: l = 0.5 m
-
Radius: r = 1 cm = 0.01 m
-
Total number of turns: N = 500
-
Current: I = 5 A
Step 1- Find turns per unit length (n):
Step 2 - Check if it qualifies as a long solenoid:
Since l/r = 50 ≫ 1, i.e., l ≫ r, the solenoid qualifies as a long solenoid, and we can use the standard formula.
Step 3 - Apply the formula B = μ0nI:
Answer: The magnetic field inside the solenoid is approximately 6.28 × 10−3 T (or ≈ 6.3 × 10−3 T).
Test Yourself
Shaalaa.com | Moving Charge and Magnetism part 26 (Toroid)
Series: 1
01:05:53 undefined
00:10:06 undefined
00:10:51 undefined
00:11:52 undefined
00:13:10 undefined

