Electromagnetic Induction Experiment

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    Experiment 9: Electromagnetic Induction

    Laboratory Report

    Department of Mathematics and PhysicsCollege of Science, University of Santo Tomas

    Espaa, Manila, Philippines

    1

    Abstract

    The purpose of the experiment is to

    determine how the production of current in

    the presence of a magnetic field.

    I. Introduction

    In 1831, Michael Faraday, an

    English physicist, performed a series of

    experiments to determine whether currents

    are produced in a magnetic field. He found

    out that when a stationary magnet is placed

    inside a coil of wire, it will not produce any

    current. He later realized that a sudden push

    or pull of pole of magnet inside the coil

    produces current as evidenced by the

    deflection of the needle of a galvanometer.

    Faradays Law of Electromagnetic

    Induction is perhaps considered to be the

    most important concept in electromagnetism

    as it bridges the gap between electricity and

    magnetism. Absence of this law will also

    lead to the absence of modern electronic

    gadgets such as television, generators,

    radios, telephones, and others to name a few.

    Hence, the objectives of the experiment are

    to determine how current is induced in a coil

    of wire, to identify the factors affecting the

    induced current, and to verift Lenzs Law.

    II. Theory

    A magnetic field is produced by

    electrical currents which could be found in

    wires or it could be associated with the

    currents produced by an electron orbiting an

    atom in accordance with the Lorentz Force

    Law. In symbols,

    Equation 2.0 Lorentz Force Law

    Where F= ForceE= Electric field

    q = electric charge

    v= velocity of the charge

    B= magnetic field

    III. Methodology

    In the experiment, two coils of wire

    was used. In the first coil, there are 100

    turns of wire. The magnet was then placed

    inside the coil facing its north pole. The coilwas connected to galvanometer having a

    scale of -10 to +10 and -5 to +5 between it.

    The magnet was then quickly pulled against

    the coil and the deflection of the needle of

    the galvanometer was recorded. The same

    was done with the south pole of the bar

    magnet. The deflection of the needle of the

    galvanometer was also recorded.

    In the second coil, having 50 number

    of turns, a bar magnet was placed in themiddle of the coil. Each pole was placed and

    then quickly pulled against the coil. The

    deflection of the galvanometer for each pole

    was recorded.

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    IV. Results and Discussions

    Table 4.0 Deflection of galvanometer

    Number of

    turns of coil

    50 100

    North 5 towardsthe negative

    10 towardsthe negative

    South 5 towards

    the positive

    10 towards

    the positive

    Table 4.0 shows the amount of deflection of the

    galvanometer corresponding to the number of

    turns in a coil of wire.

    A full-scale deflection of a

    galvanometer is usually small, about 10A.

    To determine the accurate amount ofcurrent, a shunt resistor must be connected

    in parallel with the galvanometer.

    From the table, in the 50 number of

    turns of a coil of wire, same amount of

    current was observed to both poles when it

    was quickly pulled but in different

    directions. In 100 number of turns of a coil,

    both poles deflect the same amount of

    current but in different directions. This

    corresponds to the fact that when the

    number of turns increases, magnetic field

    becomes stronger which makes the current

    also stronger.

    V. Conclusions

    From the experiment, it is highly

    evident that the current is induced when

    there is a sudden change of a magnetic field.

    Repeating the same procedure with adifferent number of turns of wire, the

    galvanometer still deflects its needle. This is

    similar to what Faraday had discovered

    which states that an electric will produce if a

    magnetic field is in relative motion.

    In Table 4.0, it is clearly manifested

    that a change in the number of turns of wire

    will correspond to the amount of current it

    will produce. This factor stems from the fact

    that the magnetic field strength is directly

    proportional to the current that will beproduced.

    V. References[1] Halliday, Resnick & Walker. (1997).

    Fundamentals of physics.New York,

    NY: Wiley.

    [2] Knight, R. (2009). Physics for

    scientists and engineers: Volume 4.New York, NY: Cengage Learning.

    [3] Griffiths, D. (2012). Introduction toelectrodynamics. New York, NY:

    Addison-Wesley.

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