Fix the mistake: Electromagnetism and Circuits
Electric Current, Magnetic Field, and Ampère’s Law
Electric current produces a magnetic field, and a magnetic field exerts force on electric current. We will study the core of the interaction in electromagnetism.
Basic Knowledge
Magnetic field produced by a straight current (Ampère’s law):
At a point a distance r from current I: B = μ₀I/(2πr)
Direction: right-hand screw rule (when a right-handed screw advances in the direction of the current, the direction of rotation is the direction of the magnetic field)
Magnetic field at the center of a circular current:B = μ₀I/(2r) (r: radius of the circle)
Magnetic field inside a solenoid:B = μ₀nI (n: number of turns per unit length)
Permeability of free space: μ₀ = 4π × 10⁻⁷ T·m/A
Force acting on a current in a magnetic field (Ampère force):F = BIL sinθ (L: length of the current, θ: angle between the magnetic field and current)
Magnetic flux density B (magnetic flux density) (Strength of the magnetic field. Unit: T = Wb/m²)
Permeability μ₀ (Permeability of free space. 4π × 10⁻⁷ T·m/A)
Right-hand screw rule (When a right-handed screw advances in the current direction, the magnetic field follows the rotation direction)
Ampère force (Force experienced by a current in a magnetic field. F = BIL sinθ)
Solenoid (An electromagnet made by closely winding a coil. The inside has a uniform magnetic field)
Further Study (Background and Significance)
The attraction and repulsion of two parallel currents is an application of the Ampère force: currents in the same direction attract, while currents in opposite directions repel. The unit of current, the “ampere,” was formerly defined using this force (before the 2019 revision).
The magnetic field of a solenoid, B = μ₀nI, does not depend on the length or cross-sectional area of the coil. MRI (magnetic resonance imaging) systems use superconducting coils to create powerful uniform magnetic fields (several teslas).
The tesla (T), the basic unit of magnetic field, represents a very strong field: Earth’s magnetic field is approximately 5 × 10⁻⁵ T, MRI systems are 1.5 to 3 T, and experimental superconducting magnets can achieve more than 20 T.
- Magnetic field of a straight current: B = μ₀I/(2πr)
- Direction: right-hand screw rule
- Center of a circular current: B = μ₀I/(2r)
- Inside a solenoid: B = μ₀nI
- Ampère force: F = BIL sinθ
- μ₀ = 4π × 10⁻⁷ T·m/A
- Currents in the same direction→attraction, opposite directions→repulsion
Points to Note (Easily Confused)
① Always determine the magnetic-field direction using the right-hand screw rule (do not confuse it with the left-hand screw rule). ② Determine the direction of the Ampère force using Fleming’s left-hand rule (middle finger: current, index finger: magnetic field, thumb: force). ③ F = BIL applies when θ = 90°. In general, do not forget sinθ. ④ “Magnetic field H” and “magnetic flux density B” are different quantities. In high-school physics, B is used.
Practice
- Find the magnetic flux density at a point 0.10 m from a straight current of 5.0 A (μ₀ = 4π × 10⁻⁷ T·m/A).
- Find the magnetic flux density inside a solenoid (n = 1000 turns/m, I = 2.0 A).
- Find the force on a 0.20 m current carrying 3.0 A, placed perpendicular to a magnetic field with flux density 0.50 T.
Previous and next lessons in this course
- Previous lesson: Fix the mistake: Electric Field and Potential
- Next lesson: Fix the mistake: Electromagnetism and Circuits