Download Magnetic flux - Purdue Physics

Survey
yes no Was this document useful for you?
   Thank you for your participation!

* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project

Document related concepts

Magnetic stripe card wikipedia , lookup

Mathematical descriptions of the electromagnetic field wikipedia , lookup

Geomagnetic storm wikipedia , lookup

Magnetometer wikipedia , lookup

Friction-plate electromagnetic couplings wikipedia , lookup

Neutron magnetic moment wikipedia , lookup

Superconducting magnet wikipedia , lookup

Magnetic monopole wikipedia , lookup

Van Allen radiation belt wikipedia , lookup

Earth's magnetic field wikipedia , lookup

Giant magnetoresistance wikipedia , lookup

Multiferroics wikipedia , lookup

Electromagnetism wikipedia , lookup

Magnetotactic bacteria wikipedia , lookup

Magnet wikipedia , lookup

Magnetotellurics wikipedia , lookup

Magnetoreception wikipedia , lookup

Magnetohydrodynamics wikipedia , lookup

Ferrofluid wikipedia , lookup

Lorentz force wikipedia , lookup

Electromagnet wikipedia , lookup

Electromagnetic field wikipedia , lookup

Magnetism wikipedia , lookup

Electromotive force wikipedia , lookup

Force between magnets wikipedia , lookup

Eddy current wikipedia , lookup

History of geomagnetism wikipedia , lookup

Magnetochemistry wikipedia , lookup

Ferromagnetism wikipedia , lookup

Faraday paradox wikipedia , lookup

Transcript
 Magnetic flux () is a measure of how much
magnetic field is passing through a loop of wire.
It is at a maximum when the field lines are perpendicular to
the plane of the loop, and it is zero when the field lines are
parallel to the plane of the loop.
For a coil of N loops,
the flux through the
coil is equal to the
flux through one
loop, multiplied by
the number of loops:

𝜙 = 𝑁 ∙ 𝐵⊥ ∙ 𝐴
𝐵⊥ is the field
component
perpendicular to A.
1
Faraday’s Law

A voltage (electromotive force) is induced in a
circuit when there is a changing magnetic flux
passing through the circuit.

The induced voltage is equal to the rate of
change of the magnetic flux:




t
This process is called electromagnetic
inductance.
2
How to use Faraday’s law to
determine the induced current

direction
n
n
1.
determine the sign of ∆Φ. Here ∆Φ >0
2.
N
determine the sign of  using faraday’s law. Here  <0
3.
RHR determines the positive direction for EMF 
• Align you thumb approximately to the field
direction.
•
•
If >0, current follow the direction of the curled
fingers.
If <0, current goes to the opposite direction of
the curled fingers.
3
Conducting Loop in a Changing
Magnetic Field
Induced EMF has a direction such that it opposes
the change in magnetic flux that produced it.
approaching
 Magnetic moment 
created by induced currrent
I repels the bar magnet.
Force on ring is repulsive.
moving away
 Magnetic moment 
created by induced currrent
I attracts the bar magnet.
Force on ring is attractive.
4
Exercise
The magnetic field is increasing, what’s the direction of the
induced currents in the closed circular loop?
A. Clockwise
B. Counterclockwise
C. No induced currents.
5
6D-11 Jumping Ring
Is there any
differences in the
two rings ?
Why one can
jump up, the
other can’t ?
6
Inductor Radio (6D-15)
7
Electric Generator
Model (6B-16)
8
UHF Transmitter and
Dipole Receiver (6D-17)
9
The Existence of Atoms:
Evidence from Chemistry
 Why believe in the existence of something we
have never seen?

Observations can provide convincing evidence.

Much early evidence of atoms came from
chemistry, the study of the differences in
substances and how they can be combined to
form other substances.

Since certain substances were retrievable, early
scientists were also tempted to believe that certain
elements were made up of tiny indivisible atoms.
10
Cathode rays, Electrons, and X-rays
 By the end of the nineteenth century, chemists
were using the concept of atoms to explain their
properties.
 Physicists were less convinced.
 The discovery of cathode rays was the beginning of
atomic physics.
Two electrodes are sealed in a glass tube.
As the tube is evacuated, a glow discharge
appears in the gas between the electrodes.
With further evacuation, the discharge
disappears, and a glow appears on the end
of the tube opposite the cathode.
11
 Thomson’s discovery provided the first known subatomic
particle.



The mass of an electron is 9.1 x 10-31 kg.
The charge of an electron is 1.6 x 10-19 C.
The electron was the first possible candidate for a building block of
atoms.
 The study of cathode rays led Roentgen to discover yet
another type of radiation.
12
 He noticed that a fluorescent material
would glow when placed near his
covered cathode-ray tube.
 Cathode rays could not travel through
air, but this new radiation did.
 Because they were unknown, Roentgen
called this new radiation X-rays.
1st Nobel Prize Winner
Wikipedia: “print of
Roentgen’a first "medical" Xray, of his wife's hand, taken
on 22 December 1895”
13
Rutherford noticed when the beam of radiation from a uranium sample
passes through a magnetic field, it splits into three components.


Alpha deviates slightly to the left,
indicating positively charged
particles.
Beta is bent in the opposite
direction, indicating negatively
charged particles.


Beta is also bent much more,
indicating less massive particles
than those in the alpha beam.
Further study indicated that
these beta rays were electrons.
𝐹 = 𝑚𝑎 =

𝑚𝑣 2
𝑟
 𝑟 = 𝑚𝑣 2 /𝐹
The gamma rays were undeviated
by the magnetic field.

These are electromagnetic waves
similar to X-rays but with shorter
wavelengths.
14