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Published byDerick Patrick Modified over 6 years ago
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Magnetism, Electromagnetism, & Electromagnetic Induction
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Magnetic Fields The source of all magnetism is moving electric charges. Iron is the element with the most magnetic properties due to its net electron spin of 4. Magnetic field lines are vectors with a direction from North to South. Magnetic field lines must not cross each other. Magnetic fields are measured in Teslas and is represented with the symbol B.
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Earth’s Magnetic Field
The angle between the magnetic and geographic poles is called the magnetic declination.
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Compasses Compass needles are magnetized and line up along magnetic field lines. The North magnetic pole of a compass points to the geographic north. Since opposites attract, the magnetic pole in the Northern Hemisphere is actually a South magnetic pole. The North pole of a compass points in the direction of the field lines.
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Magnetic Field around a straight current-carrying wire
A current moving through a wire creates a magnetic field around that wire. The magnetic field forms concentric circles around the wire. Right hand rule (see picture): thumb – points in direction of the current in the wire fingers curl – in direction of the magnetic field
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Electromagnets Electromagnets are temporary magnets formed by wrapping wire around an iron core. The iron becomes magnetized when the current is flowing due to the magnetic field being concentrated inside the coil of wire. Right-hand Rule: Fingers curl – in direction of the current (+ to -) Thumb – points in direction of the North pole N S
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Force of a magnetic field on a charged particle
A charged particle moving through a magnetic field will experience a force that will cause it to move in a circular path. The force is to both the velocity and the magnetic field direction. F = force(N), q = charge(C), v = velocity(m/s), B = mag. field strength(T), =angle between v & B
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Right-hand Rule (F=qvB)
Flat fingers – point in direction of the magnetic field (B) Thumb – points in the direction the charged particle is moving (v) Coming out of palm – direction of the force on the charged particle (F) Note – This rule is for a positively charged particle. For a negatively charged particle, force is negative and so the direction of the force is in the opposite direction of the right-hand rule.
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Magnitude of Force (F=qvB)
If Ө is zero, F = 0. So there is no force on the charged particle if the particle moves parallel to the magnetic field. If Ө is 90°, F = maximum. So there is a maximum force on the charged particle if the charged particle moves perpendicular to the magnetic field. If Ө is between 0 and 90°, the force will between 0 and a maximum. For the right-hand rules we will assume 90°.
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Force of a magnetic field on a current-carrying wire
A conductor with a current flowing through it in a magnetic field will experience a force. F = force(N), I = current(A), l = length of wire(m), B = mag. field strength(T), =angle between l & B
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Right-hand Rule ( Flat fingers – point in the direction of the magnetic field (B) Thumb – points in the direction the current or moving charges (I) Out of palm – direction of the force on the wire (F) Remember: magnetic field is from N to S, current is from + to -
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Magnitude of Force If Ө is zero, F = 0. So there is no force on the wire if the wire moves parallel to the magnetic field. If Ө is 90°, F = maximum. So there is a maximum force on the wire if the wire moves perpendicular to the magnetic field. If Ө is between 0 and 90°, the force will between 0 and a maximum. For the right-hand rules we will assume 90°.
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Force between 2 current-carrying wires
When 2 wires carry current near each other there will be an interaction (force) between the magnetic fields produced by each individual wire. Current going the same way – the wires are attracted. Current going the opposite way- the wires are repelled.
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Induced EMF (Voltage) A conductor in a changing magnetic field will have an EMF (voltage) induced . Either the conductor can be moving across field lines or the magnetic field can itself be changing. EMF EMF EMF = electromotive force or voltage(V), B = magnetic field strength (T), v = velocity of wire (m/s)
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Induced Current When a EMF (voltage, or potential difference) is present in a closed loop of conducting material current will flow. I=current(A), EMF = V = Voltage(V), R = resistance
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Lenz Law The voltage (and thus current) induced when a wire or conductor is moved through a magnetic field is induced in such a way that the magnetic field created by the induced current opposes the original magnetic field that induced the voltage or current.
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Motors vs. Generators Motors Generators
Electric current is changed to motion. A coil of wire with a current through it will be forced to turn in a magnetic field. Generators Motion is changed to electric current. Turning a coil in a magnetic field will induce an EMF (voltage), thus current is produced.
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AC Generator As the loop of wire is turned in the magnetic field, one side is moving up while the other is moving down, therefore a current is induced in opposite directions in the different sections of the loop. As the loop continues to turn, the sections of wire change places and so the current switches direction. This causes the current to change constantly as shown in the graph.
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AC/DC Alternating Current (AC)
current that switches direction of flow on regular time intervals 60 Hz in US created by EMF induced in a coil of wire turning in a magnetic field Direct Current (DC) current that flows in only one direction through a circuit supplied by batteries or electrochemical cells created by a chemical reaction that produces a potential difference (voltage) between the two electrodes (terminals)
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Effective vs. Maximum with AC Current
DC values are comparable to Effective AC values. AC circuits do not get the effect of the maximum current and voltage produced The power equivalent of AC to DC voltage is half.
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Transformers An alternating current flows through the primary coil creating an alternating magnetic field. This changing magnetic field induces an EMF (Voltage) in the secondary coil and thus current flows. In an ideal transformer, Power in = Power out
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To solve Transformer Problems
The ratio of voltages on the two coils is equal to the ratio of the number of turns in the coils.
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