Magnetic force on -carrying wires is a key concept in electromagnetism. It explains how magnetic fields interact with electric currents, causing forces that can move wires or create torque on current loops.
This topic builds on previous knowledge of magnetic fields and electric currents. Understanding these forces is crucial for grasping the principles behind electric motors, generators, and other electromagnetic devices used in everyday technology.
Magnetic fields and conductors
Magnetic fields and conductors form the foundation of electromagnetism in Physics II
Understanding their interaction underpins many practical applications in modern technology
Properties of magnetic fields
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Top images from around the web for Properties of magnetic fields
Magnetic Fields Produced by Currents: Ampere’s Law | Physics View original
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22.3 Magnetic Fields and Magnetic Field Lines – College Physics View original
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22.7 Magnetic Force on a Current-Carrying Conductor – College Physics View original
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Magnetic Fields Produced by Currents: Ampere’s Law | Physics View original
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22.3 Magnetic Fields and Magnetic Field Lines – College Physics View original
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Magnetic fields exert forces on moving charges and current-carrying conductors
Represented by magnetic field lines indicating direction and strength
Measured in units of (T)
Produced by permanent magnets, moving charges, and changing electric fields
Current-carrying conductors
Conductors with electric current create their own magnetic fields
Field strength proportional to current magnitude
Field direction determined by
Interact with external magnetic fields, experiencing forces and torques
Lorentz force law
law describes the force experienced by charged particles in electromagnetic fields
Combines effects of both electric and magnetic forces on moving charges
Force on moving charges
Magnetic force on a moving charge given by F=qv×B
Force magnitude depends on charge (q), velocity (v), and (B)
Force direction perpendicular to both velocity and magnetic field vectors
Results in circular motion when velocity perpendicular to uniform magnetic field
Force on current-carrying wires
Current in a wire consists of moving charges, subject to magnetic force
Net force on wire given by F=IL×B
I represents current, L is the length vector of the wire segment
Force direction determined by right-hand rule
Magnetic force equation
Magnetic force equation quantifies the force experienced by current-carrying conductors in magnetic fields
Essential for analyzing and designing electromagnetic devices
Magnitude of magnetic force
Force magnitude given by F=ILBsinθ
θ represents the angle between the wire and magnetic field
Maximum force occurs when wire perpendicular to field (θ = 90°)
Force becomes zero when wire parallel to field (θ = 0° or 180°)
Direction of magnetic force
Determined using
Thumb represents current direction
Forefinger points in magnetic field direction
Middle finger indicates force direction
Always perpendicular to both current and magnetic field
Factors affecting magnetic force
Understanding these factors allows for precise control and manipulation of magnetic forces in various applications
Crucial for designing efficient electromagnetic devices and systems
Current intensity
Directly proportional to magnetic force
Doubling current doubles the force
Allows control of force magnitude by adjusting current
High currents can lead to heating and potential damage to conductors
Wire length
Force increases linearly with wire length in uniform magnetic field
Longer wires experience greater total force
Practical limitation on wire length due to resistance and power requirements
Magnetic field strength
Directly proportional to magnetic force
Stronger fields produce larger forces
Can be increased using stronger magnets or electromagnets
Field strength typically decreases with distance from source
Angle between wire and field
Force varies sinusoidally with angle between wire and field
Maximum force at 90° (perpendicular)
Zero force at 0° or 180° (parallel)
Allows for force control by adjusting wire orientation
Applications of magnetic force
Magnetic force on current-carrying conductors finds numerous practical applications in modern technology
Demonstrates the importance of electromagnetic principles in everyday devices
Electric motors
Convert electrical energy to mechanical energy
Utilize magnetic force on current-carrying loops to produce rotational motion
Commutator reverses current direction to maintain rotation
Found in various applications (electric vehicles, industrial machinery, household appliances)
Loudspeakers
Transform electrical signals into sound waves
Current-carrying coil in magnetic field moves diaphragm
Varying current produces corresponding variations in sound pressure
Frequency response determined by coil and diaphragm properties
Magnetic levitation
Supports objects using magnetic repulsion or attraction
Used in high-speed trains (maglev) for frictionless transportation
Employed in magnetic bearings for reduced wear and energy loss
Enables contactless suspension of objects in scientific experiments
Torque on current loops
Torque on current loops forms the basis for many rotating electrical machines
Essential concept for understanding the operation of motors and generators
Magnetic dipole moment
Measure of the strength of a current loop's magnetic field
Given by μ=IAn^
I represents current, A is loop area, n̂ is unit vector normal to loop plane
Determines the loop's interaction with external magnetic fields
Torque equation
Torque on current loop in uniform magnetic field given by τ=μ×B
Magnitude: τ=μBsinθ
θ is angle between magnetic moment and field vectors
Maximum torque occurs when loop perpendicular to field
Parallel vs perpendicular wires
Understanding forces between current-carrying wires is crucial for designing electrical systems
Helps in analyzing and preventing unwanted interactions in complex circuits