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mv=integral(fdt)kuruman said:This is not a Faraday's law question. You need to calculate the impulse F dt given to the conductor and set it equal to its momentum change.
and the force i was giving before is it the force on each charged particle?kuruman said:This is not a Faraday's law question. You need to calculate the impulse F dt given to the conductor and set it equal to its momentum change.
Because a segment of wire of length ##\vec L## carrying current ##I## in a magnetic field ##\vec B## experiences a force ##\vec F=I\vec L \times \vec B##.Suyash Singh said:but why is force in my book given as b l i (i is current)
ohhhh ok. i already knew that formula it was written differently so i couldn't recognise it.kuruman said:Because a segment of wire of length ##\vec L## carrying current ##I## in a magnetic field ##\vec B## experiences a force ##\vec F=I\vec L \times \vec B##.
You don't need an integral for the impulse. Assume that the force is constant while it lasts in which case the impulse is J = F Δt.
The force on a conductor in a magnetic field is known as the Lorentz force, and it is equal to the product of the current in the conductor, the length of the conductor, the strength of the magnetic field, and the sine of the angle between the current and the magnetic field.
The direction of the force on a conductor in a magnetic field follows the right-hand rule, where the direction of the force is perpendicular to both the direction of the current and the direction of the magnetic field.
The force on a conductor in a magnetic field is affected by the strength of the magnetic field, the current running through the conductor, the length of the conductor, and the angle between the current and the magnetic field.
Yes, the force on a conductor in a magnetic field can be used to do work, as it can cause the conductor to move in the direction of the force and perform mechanical work.
The force on a conductor in a magnetic field has many applications, including electric motors, generators, and particle accelerators. It is also used in many everyday devices such as speakers, headphones, and MRI machines.