Joseph Henry and Michael Faraday had independently discovered the phenomenon of electromagnetic induction in the early 19th century.
Electromagnetic induction occurs when a conductor cuts across magnetic field lines.
Faraday’s law of electromagnetic induction states that the induced electromotive force (emf) in a circuit is directly proportional to the rate of change of magnetic flux through the circuit.
The induced emf (e) is given by the equation: e = -N(dΦ/dt), where N is the number of turns in the circuit coil and (dΦ/dt) is the rate of change of magnetic flux.
The negative sign indicates that the induced emf opposes the change in magnetic flux.
Mutual and Self-Inductance
Mutual inductance occurs when there are two or more coils in close proximity.
Self-inductance occurs when a single coil produces an induced emf in itself.
Both mutual and self-inductance are quantified by the property called inductance (L).
The unit of inductance is the Henry (H).
The inductance of a coil depends on factors like the number of turns, the geometry of the coil, and the presence of any core material.
Mutual Inductance and Faraday’s Law
Mutual inductance (M) is a measure of the extent to which a change in current in one coil induces an emf in an adjacent coil.
The mutual inductance between two coils is given by the equation: M = k√(L₁L₂), where k is the coupling coefficient, and L₁ and L₂ are the inductances of the coils.
Faraday’s law of electromagnetic induction can also be expressed in terms of mutual inductance: e₁ = -M(dI₂/dt), where e₁ is the induced emf in coil 1, and dI₂/dt is the rate of change of current in coil 2.
Self-Inductance and Faraday’s Law
Self-inductance occurs when a change in current in a coil induces an emf in the same coil.
The induced emf in a coil due to self-inductance is given by the equation: e = -L(dI/dt), where L is the self-inductance of the coil.
The negative sign indicates that the induced emf opposes the change in current.
Self-inductance depends on the geometry of the coil and the presence of any core material.
Induced EMF and Magnetic Field
According to Faraday’s law, the induced emf is directly proportional to the rate of change of magnetic flux.
Magnetic flux (Φ) through a loop of area (A) is given by the equation: Φ = B⊥A, where B⊥ is the magnetic field perpendicular to the area.
Therefore, we can rewrite Faraday’s law as: e = -N(d(B⊥A)/dt).
Magnetic field lines that are parallel or perpendicular to the area contribute to the magnetic flux, while those at other angles do not.
Lenz’s Law
Lenz’s law states that the direction of the induced current (or emf) is such that it opposes the change producing it.
This law is a consequence of the conservation of energy.
Lenz’s law helps us determine the direction of induced currents in circuits.
When a magnetic field through a loop increases, the induced current creates a magnetic field that opposes the increase.
When a magnetic field through a loop decreases, the induced current creates a magnetic field that opposes the decrease.
Examples of Faraday’s Law and Lenz’s Law
Example 1: A coil with 200 turns and an inductance of 0.05 H is subjected to a changing magnetic field with a rate of change of 50 T/s. Calculate the induced emf in the coil.
Example 2: A bar magnet is moved towards a coil. Determine the direction of the induced current in the coil, according to Lenz’s law.
Example 3: A solenoid coil is connected to a battery and a switch. When the switch is closed, the magnetic flux through the solenoid increases. Determine the direction of the induced current in the solenoid.
Applications of Faraday’s Law of Induction
Transformers: Transformers work on the principle of electromagnetic induction and are used to step-up or step-down voltage levels.
Generators: Electric generators convert mechanical energy into electrical energy through the process of electromagnetic induction.
Inductive Charging: Inductive charging is used to wirelessly recharge devices like smartphones and electric vehicles.
Magnetic Flow Meters: Magnetic flow meters measure the flow rate of conductive fluids using Faraday’s law of induction.
Summary
Faraday’s law of electromagnetic induction states that the induced emf in a circuit is directly proportional to the rate of change of magnetic flux through the circuit.
Mutual inductance occurs when there are two or more coils in close proximity, while self-inductance occurs when a single coil produces an induced emf in itself.
Lenz’s law states that the induced current opposes the change producing it.
Faraday’s law and Lenz’s law have various applications in transformers, generators, inductive charging, and magnetic flow meters.
Faraday’s Law of Induction
Joseph Henry and Michael Faraday discovered electromagnetic induction.
Induction occurs when a conductor cuts across magnetic field lines.
Faraday’s law states that induced emf is proportional to the rate of change of magnetic flux through a circuit.
Induced emf (e) = -N(dΦ/dt), where N is the number of coil turns.
The negative sign indicates the induced emf opposition to the change.
Mutual and Self-Inductance
Mutual inductance occurs between coils in close proximity.
Self-inductance occurs when a coil induces emf in itself.
Both are quantified by inductance (L) measured in Henry (H).
Inductance depends on factors like number of turns and coil geometry.
Inductance is also affected by the presence of core material.
Mutual Inductance and Faraday’s Law
Mutual inductance (M) measures the extent of induced emf between coils.
M = k√(L₁L₂), where k is the coupling coefficient.
Faraday’s law in terms of mutual inductance: e₁ = -M(dI₂/dt).
e₁ is the induced emf in coil 1 and dI₂/dt is the rate of change of current in coil 2.
Induced emf opposes changes in magnetic flux and current.
Self-Inductance and Faraday’s Law
Self-inductance occurs when a coil induces emf in itself.
The induced emf in a coil is given by: e = -L(dI/dt).
e is the induced emf, L is the self-inductance of the coil.
The negative sign indicates the induced emf opposes the change in current.
Self-inductance depends on coil geometry and core material.
Induced EMF and Magnetic Field
Induced emf is directly proportional to the rate of change of magnetic flux.
Magnetic flux (Φ) through a loop of area (A) = B⊥A.
Faraday’s law formula can be rewritten as: e = -N(d(B⊥A)/dt).
Magnetic flux is contributed by magnetic field lines parallel or perpendicular to the area.
Magnetic field lines at other angles do not contribute to the flux.
Lenz’s Law
Lenz’s law states that induced current opposes the change producing it.
It is a consequence of energy conservation.
Lenz’s law helps determine the direction of induced currents.
When the magnetic field through a loop increases, the induced current creates a field opposing the increase.
When the magnetic field decreases, the induced current opposes the decrease.
Examples of Faraday’s Law and Lenz’s Law
Example 1: A coil with 200 turns and inductance 0.05 H experiences a changing magnetic field with a rate of change of 50 T/s. Calculate the induced emf in the coil.
Example 2: A bar magnet is moved towards a coil. Determine the direction of the induced current in the coil according to Lenz’s law.
Example 3: A solenoid coil connected to a battery and a switch. When the switch is closed, the magnetic flux through the solenoid increases. Determine the direction of the induced current in the solenoid.
Applications of Faraday’s Law of Induction
Transformers: Step-up/Step-down voltage levels.
Generators: Convert mechanical energy to electrical energy through induction.
Inductive Charging: Wireless charging for smartphones and electric vehicles.
Magnetic Flow Meters: Measure flow rate of conductive fluids based on Faraday’s law.
Summary
Faraday’s law states induced emf is proportional to the rate of change of magnetic flux.
Mutual inductance occurs between close coils, self-inductance occurs within a coil.
Inductance depends on turns, geometry, and core material.
Faraday’s law in terms of mutual inductance: e₁ = -M(dI₂/dt).
Induced emf opposes magnetic flux and current change.
Summary (contd.)
Self-inductance formula: e = -L(dI/dt).
Induced emf opposes current change.
Lenz’s law states induced current opposes the change.
Applications include transformers, generators, inductive charging, and magnetic flow meters.
Understanding Faraday’s and Lenz’s laws is crucial for various aspects of electromagnetism.
Applications of Faraday’s Law of Induction (contd.)
Electromagnetic Brakes: Faraday’s law is used in electromagnetic brakes to convert electrical energy into mechanical energy to slow down or stop moving objects.
Eddy Currents: When a conductor moves through a magnetic field, eddy currents are induced, which resist the motion of the conductor and produce heat.
Magnetic Levitation: Faraday’s law is utilized in magnetic levitation systems to suspend objects in mid-air using the repulsion of magnetic fields.
Induction Heating: Induction heating is widely used in industry to heat metals and other conductive materials through the process of electromagnetic induction.
Magnetic Resonance Imaging (MRI): MRI machines use Faraday’s law to generate magnetic fields and measure the response of the body’s atoms to these fields, creating detailed images of internal body structures.
Wireless Power Transfer: Inductive coupling is used in wireless power transfer systems to transmit electrical energy between coils without the need for direct electrical connections.
Faraday’s Law and Electrical Generators
Electric generators are devices that convert mechanical energy into electrical energy using Faraday’s law of electromagnetic induction.
A generator consists of a coil of wire rotating within a magnetic field.
When the coil rotates, the magnetic field through the coil changes, inducing an emf according to Faraday’s law.
This induced emf produces a current in the coil, which can be extracted as electrical energy.
Faraday’s Law and Transformers
Transformers are devices that alter the voltage level of an alternating current (AC) without changing its frequency.
Transformers work based on the principle of mutual induction between primary and secondary coils.
The changing current in the primary coil produces a changing magnetic field, which induces an emf in the secondary coil according to Faraday’s law.
The ratio of the number of turns in the primary and secondary coils determines the voltage ratio of the transformer.
Faraday’s Law and Magnetic Flow Meters
Magnetic flow meters are used to measure the flow rate of conductive fluids.
These meters utilize Faraday’s law of electromagnetic induction.
A magnetic field is applied perpendicular to the flow of the fluid, and electrodes detect the voltage induced by the fluid passing through the magnetic field.
The induced voltage is proportional to the velocity of the fluid, allowing for the measurement of flow rate.
Faraday’s Law and Inductive Sensors
Inductive sensors are used to detect the presence or absence of metallic objects.
These sensors work based on Faraday’s law of electromagnetic induction.
When a metallic object enters the sensing region of the inductive sensor, it induces eddy currents in the object, which in turn induce an emf in the sensing coil.
The change in the induced emf is detected and used to determine the presence or absence of the object.
Faraday’s Law and Coils in Circuits
Coils with inductance play a crucial role in electrical circuits.
When the current through a coil changes, an induced emf opposes the change according to Faraday’s law.
This phenomenon is utilized in devices like inductors and solenoids.
Inductors are passive components that store energy in the form of a magnetic field when current flows through them.
Solenoids are coils with an iron core that produce a strong magnetic field when current passes through them.
Faraday’s Law and AC Generators
AC generators, also known as alternators, are used to produce alternating current (AC) electrical energy.
They work based on Faraday’s law of electromagnetic induction.
AC generators consist of rotating coils within a magnetic field.
As the coils rotate, the magnetic field through them changes, inducing an alternating current in the coils.
This alternating current can be used to power various electrical devices.
Faraday’s Law and Eddy Current Brakes
Eddy current brakes are used to slow down or stop moving objects.
They work based on Faraday’s law and Lenz’s law.
As a conductor moves through a magnetic field, eddy currents are induced in the conductor, which create a magnetic field opposing the motion.
The magnetic field of the eddy currents interacts with the magnetic field of the brake, generating a resisting force that slows down the object.
Faraday’s Law and Magnetic Resonance Imaging (MRI)
Magnetic resonance imaging (MRI) is a medical imaging technique that uses strong magnetic fields and radio waves to create detailed images of the body’s internal structures.
MRI machines work based on Faraday’s law of electromagnetic induction.
The magnetic fields produced by the machine cause the body’s atoms to align with the magnetic field.
Small radio frequency signals are then applied, causing the atoms to resonate.
The resonance signals are detected and used to create the images.
Faraday’s Law and Inductive Charging
Inductive charging is a wireless charging technology that uses Faraday’s law of electromagnetic induction.
It is commonly used for charging smartphones, electric toothbrushes, and electric vehicles.
Inductive charging pads generate a magnetic field, which induces an emf in a receiving coil in the device to be charged.
The induced emf is then rectified and used to charge the device’s battery.
Recap
Faraday’s law of induction states that the induced electromotive force (emf) in a circuit is directly proportional to the rate of change of magnetic flux through the circuit.
Mutual inductance occurs between two coils, while self-inductance occurs in a single coil.
Lenz’s law states that the induced current or emf in a circuit opposes the change producing it.
Faraday’s law and Lenz’s law have various applications, including transformers, generators, inductive charging, and magnetic flow meters.
Understanding Faraday’s law and its applications is essential for the study of electromagnetism.
Faraday’s Law of Induction Joseph Henry and Michael Faraday had independently discovered the phenomenon of electromagnetic induction in the early 19th century. Electromagnetic induction occurs when a conductor cuts across magnetic field lines. Faraday’s law of electromagnetic induction states that the induced electromotive force (emf) in a circuit is directly proportional to the rate of change of magnetic flux through the circuit. The induced emf (e) is given by the equation: e = -N(dΦ/dt), where N is the number of turns in the circuit coil and (dΦ/dt) is the rate of change of magnetic flux. The negative sign indicates that the induced emf opposes the change in magnetic flux.