30.8
La loi de Faraday
La loi de Faraday stipule que la force électromotrice induite est le changement négatif du flux magnétique par unité de temps. Tout changement dans le…
La loi de Faraday stipule que dans une boucle conductrice fermée, la f.é.m. induite est égale à la dérivée temporelle négative du flux magnétique à travers cette boucle. La direction de la f.é.m. induite a été donnée plus tard par Lenz.
Si la boucle conductrice est constituée d’un nombre N de spires identiques et que le flux passant par chacune d’elles est le même, alors le flux magnétique total est N fois le flux magnétique traversant chaque tour. Par conséquent, la f.é.m. induite totale sera N multipliée par le taux de variation du flux magnétique.
Considérons une bobine carrée de 0,25 mètre de long, qui se compose de 500 tours de fil étroitement enroulés. Cette bobine est placée dans le champ magnétique qui augmente au rythme de 0,2 tesla par seconde.
Ensuite, l'amplitude de la f.é.m. induite dans la bobine peut être calculée à l'aide de la loi de Faraday. En substituant les valeurs, l’amplitude de la f.é.m. induite peut être estimée.
Il est important d’observer que la f.é.m. peut être induite en modifiant l’un de ces paramètres ou une combinaison d’entre eux.
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Q1: What does Faraday's law state about induced emf in a conducting loop?
Faraday's law states that the induced emf in a closed conducting loop equals the negative time derivative of magnetic flux through that loop. This means the induced emf is directly proportional to how quickly the magnetic flux changes. The negative sign indicates the direction of the induced emf, which is determined by Lenz's law. Any change in the magnetic field or coil orientation induces a voltage.
Q2: How does the number of coil turns affect the total induced emf?
When a conducting loop consists of N identical turns with the same magnetic flux through each turn, the total magnetic flux is N times the flux through a single turn. Consequently, the total induced emf is N multiplied by the rate of change of magnetic flux. This relationship allows engineers to increase induced emf by adding more tightly wound turns to the coil.
Q3: What parameters can be changed to induce an emf in a coil?
An emf can be induced by changing the magnetic field strength, the orientation of the coil's area relative to the magnetic field, or a combination of both. For example, if a square coil is placed in an increasing magnetic field, the changing flux induces an emf. Similarly, rotating the coil changes the dot product of the magnetic field and area vectors, also inducing an emf.
Q4: How is magnetic flux calculated and what does it represent?
Magnetic flux measures the number of magnetic field lines passing through a given surface area. It is calculated as the integral of the dot product of the magnetic field vector and the area vector. This calculation accounts for both the field strength and the angle between the field and the surface. Understanding magnetic flux is essential for applying Faraday's law to real-world electromagnetic systems.
Q5: What are practical applications of Faraday's law in everyday devices?
Ground fault interrupter (GFI) devices use Faraday's law as a circuit breaker to prevent electrical shocks. Electric guitars employ the principle when a pick coil near a vibrating string detects changes in magnetic flux caused by the string's motion. This changing flux produces an emf that is amplified to create sound. These applications demonstrate how induced electric fields enable modern technology.
Q6: How would you calculate the induced emf in a specific coil using Faraday's law?
To calculate induced emf, substitute the known values into Faraday's law: emf equals negative N times the rate of change of magnetic flux. For a square coil with 500 turns and 0.25-meter sides in a magnetic field increasing at 0.2 tesla per second, multiply 500 by the area (0.0625 m²) and the field change rate to find the magnitude of induced emf.
Q7: Why is the negative sign important in Faraday's law?
The negative sign in Faraday's law describes the direction in which the induced emf drives current around a circuit, reflecting Lenz's law. This sign indicates that the induced current opposes the change in magnetic flux that created it. While the negative sign is mathematically important, the actual direction is most easily determined using Lenz's law as a practical guide.