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Welcome to our Physics lesson on Magnetic Force on Moving Charges, this is the first lesson of our suite of physics lessons covering the topic of Magnetic Force on a Wire Moving Inside a Magnetic Field. Lorentz Force, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.
It is a known fact that current is a result of charges moving in a given direction. Stationary free charges do not produce any current, neither can the charges moving in random directions do. Therefore, if we want to deal with electric current, we will also take into account the magnetic effect it causes, and therefore the magnetic force produced.
In addition, since forces cause motion, it is expected the charges move even when they are not flowing through a conducting wire; the only condition for this, is the charges to be in one directional regular motion. However, in most cases we refer to electric charges moving through a conducting wire as this is the easiest method to obtain regular motion of charges.
The magnetic force F1 acting on each charge due to their directed motion in the conducting wire is calculated by dividing the total magnetic force Ftot by the number of charges n flowing in the entire length L of the wire. Mathematically, we have:
Since the above magnetic force is the same magnetic force we have discussed in the previous tutorial (Ampere's Force), we can write
Giving that the current I is
where ΔQ is the charge flowing through the wire in the time interval Δt and
where v is the velocity of moving charges throughout the wire, we obtain
In addition, the total charge flowing through the wire during the interval Δt is a multiple of elementary charge e (i.e. ΔQ = n ∙ e) we obtain
The vector form of the above equation is
Remark! The symbol e used above is not intended for electrons but for elementary charges despite in general there are the electrons the changes that can move.
We have always taken the direction of current from positive to negative. Therefore, to find the direction of magnetic force acting on a moving elementary charge we must assume it as positive, although we know that only negative charges (electrons) are able to move through a conductor (positive charges can move only inside an electrolyte). Since the above formula derives from that of Ampere's Force, the magnetic force on positive charges is found by using the Fleming's left hand rule. According to this rule the four fingers lie in the direction of motion of the positive charges, the palm is punched by magnetic field lines and the thumb shows the moving direction caused on the wire due to this interaction. But if the type of charge changes (i.e. if we consider a negative charge instead of a positive one), the direction of force will change as well. For example, the wire in the figure shown earlier moves in the onto-the-page direction. This is illustrated in the figure below.
Not always the direction of particles motion is perpendicular to the magnetic field lines. When these two vectors form another angle θ to each other, we have to consider this angle as well. The formula of magnetic force for an elementary electric charge in such conditions therefore becomes
However, the force vector will still be perpendicular to the plane of the other two vectors (v and B).
An electron is moving at 200 m/s at 300 to the direction of a 6mT magnetic field lines as shown in the figure.
Take the magnitude of elementary charge equal to 1.6 × 10-19 C.
We can use the same approach for larger charged objects as well. In this case, we apply the vector equation
or its scalar equivalent
to calculate the magnetic force of a charged object in motion. This force is the same force we have called earlier as "the Ampere's force". This is because
Let's consider another example in this regard.
A 20 cm long current carrying wire, which is able to carry 4A of current in 10 seconds is placed between the poles of a U-shaped (horseshoe) magnet as shown in the figure.
If the magnetic field produced by the magnet is 50 mT, calculate:
Clues:
L = 20 cm = 0.2 m
I = 4 A
t = 10 s
B = 50 mT = 0.05 T
You have reached the end of Physics lesson 16.4.1 Magnetic Force on Moving Charges. There are 3 lessons in this physics tutorial covering Magnetic Force on a Wire Moving Inside a Magnetic Field. Lorentz Force, you can access all the lessons from this tutorial below.
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