ELECTROMAGNETIC PHENOMENA 1. Electromagnetic induction Magnetic flux is a measurement of the total magnetic field B which passes through a given area. It is a useful tool for helping describe the effects of the magnetic force on something occupying a given area. If the magnetic field is constant, the magnetic flux passing through a surface of area A is Og = B · A· cose Normal to A The SI unit of magnetic flux is the Weber (Wb). Faraday law When a current conducting wire or coil is moved through a magnetic field a voltage (EMF) is generated which depends on the magnetic flux through the area of the coil. This is an example of the phenomenon of electromagnetic induction; the current that flows in this situation is known as an induced current. Faraday's Law relates the average induced EMF in terms of the time rate of change of the total magnetic flux through a current B cos e * - BA cos e = B A conductor or coil. ДФв = N- At Finally, if a coil has N turns, an emf will be produced that is N times greater than for a single coil, so that emf is directly proportional to N. The magnetic field strength (magnitude) produced by a long straight current-carrying wire is found by experiment to be B = where I is the current, r is the shortest distance to the wire, and the constant 40 = 47×107T · m/A is the permeability of free space. Magnetic field produced by a current-carrying circular loop. There is a simple formula for the magnetic field strength at the center of a circular loop. It is B = where R is the radius of the loop. One way to get a larger field is to have N loops; then, the field is B = N . 2. Electromagnetic field At every instant the ratio of the magnitude of the electric field to the magnitude of the magnetic field in an electromagnetic wave equals the speed of light. Ho! 2R Emax E Bmax B 3. Electromagnetic waves The magnitudes electric field strength E and magnetic field strength B in electromagnetic wave vary with x and t according to the expressions E (x, t) = E,sin(kx – wt) B(x, t) = B,sin(kx – wt) Here k = and w with A the wavelength and Tthe period of the wave (T=1/fwhere fis the frequency of oscillation of the wave). The speed of the wave is given by v=c = w /k. There are many types of waves, such as water waves and even earthquakes. Among the many shared attributes of waves are propagation speed v, frequency f, and wavelength 2. These are always related by the expression: v = af Electromagnetic waves, like visible light, infrared, ultraviolet, X-rays, and gamma rays don't need a medium in which to propagate; they can travel through a vacuum. Speed of electromagnetic wave in vacuum Taking the permittivity of free space ɛ, = 8.85 - 10-12 F/m and permeability of free space lo = 4xx10 7 T-m/A , c = 3. 10° m/sec. Table Electromagetik Waves Life sclences Type of EM Issues Production Applications wave aspect Communications Remote controls Requires controls for band use Radio & TV Accelerating charges MRI Acelerating charges & thermal Communications Ovens Dep heating agkation Themal agitations & elecronic Thermal imaging transitions Microwaves Cell phone une Radar Absorbed by almosphere Photosynthesis Human vision Intrered Greenhouse efect Heaing Themal agkations & ekctronic ransitions Thermal agitations & electronic Sterilization Cancer |алtions mner elecronic transitions and Medical Security fast collisions Visitle All pervasive Ozone depletion Cancer causing Vitamin D production Utraviolet control Medical diagnosis Cancer therapy Medical diagnosis Cancer therapy | X-аую Cancer causing Nuclear medicinesecurity Cancer causing Radation damage Gamma rays Nuclear decay 4. Energy in eleetromagnetic wave Electromagnetic waves can bring energy into a system by virtue of their electric and magnetic fields. These fields can exert forces and move charges in the system and, thus, do work on them. Once electromagnetic wave has created, the fields carry energy away from a source. Intensity I of electromagnetic wave is energy per area A per time t or power P per area. Intensity is measured in W/m²:1 = Energy – The energy carried and the intensity I of an electromagnetic wave is proportional to E and B. In fact, for a continuous sinusoidal electromagnetic wave, the average intensity I is given by A-t where c is the speed of light, is the permittivity of free space, and Eo is the maximum electric field strength. The average intensity of an electromagnetic wave I can also be expressed in tems of the magnetic field strength I = 5. Radiation pressure is the pressure exerted upon any surface due to the exchange of momentum between the object and the electromagnetic field. The radiation pressure Pexerted on the perfectly absorbing surface is: P = 6. The electromagnetic wave intensity at distance r from the source I = - where Bo is the maximum magnetic field strength. here P is power.

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Chapter1: Units, Trigonometry. And Vectors
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The Earth reflects approximately 38.0% of the incident sunlight from its clouds and surface. (a) Given that the intensity of solar radiation is 1 340 W/m2, what is the radiation pressure on the Earth, in pascals, when the Sun is straight overhead? (b) Compare this to normal atmospheric pressure at the Earth’s surface, which is 101 kPa.

ELECTROMAGNETIC PHENOMENA
1. Electromagnetic induction
Magnetic flux is a measurement of the total magnetic field B which passes through a given
area. It is a useful tool for helping describe the effects of the magnetic force on something
occupying a given area. If the magnetic field is constant, the magnetic flux passing through a
surface of area A is
Og = B · A· cose
Normal to A
The SI unit of magnetic flux is the Weber (Wb).
Faraday law
When a current conducting wire or coil is moved through a
magnetic field a voltage (EMF) is generated which depends on
the magnetic flux through the area of the coil. This is an example
of the phenomenon of electromagnetic induction; the current
that flows in this situation is known as an induced current.
Faraday's Law relates the average induced EMF in terms of the
time rate of change of the total magnetic flux through a current
B cos e
* - BA cos e = B A
conductor or coil.
ДФв
= N-
At
Finally, if a coil has N turns, an emf will be produced that is N times greater than for a single
coil, so that emf is directly proportional to N.
The magnetic field strength (magnitude) produced by a long straight current-carrying
wire is found by experiment to be B = where I is the current, r is the shortest distance to
the wire, and the constant 40 = 47×107T · m/A is the permeability of free space.
Magnetic field produced by a current-carrying circular loop. There is a simple formula for
the magnetic field strength at the center of a circular loop. It is B = where R is the radius
of the loop. One way to get a larger field is to have N loops; then, the field is B = N .
2. Electromagnetic field
At every instant the ratio of the magnitude of the electric field to the magnitude of the magnetic
field in an electromagnetic wave equals the speed of light.
Ho!
2R
Emax E
Bmax B
3. Electromagnetic waves
The magnitudes electric field strength E and magnetic field
strength B in electromagnetic wave vary with x and t
according to the expressions
E (x, t) = E,sin(kx – wt)
B(x, t) = B,sin(kx – wt)
Here k = and w
with A the wavelength and Tthe period of the wave (T=1/fwhere fis the frequency of oscillation
of the wave). The speed of the wave is given by v=c = w /k.
There are many types of waves, such as water waves and even earthquakes. Among the many
shared attributes of waves are propagation speed v, frequency f, and wavelength 2. These are
always related by the expression:
v = af
Transcribed Image Text:ELECTROMAGNETIC PHENOMENA 1. Electromagnetic induction Magnetic flux is a measurement of the total magnetic field B which passes through a given area. It is a useful tool for helping describe the effects of the magnetic force on something occupying a given area. If the magnetic field is constant, the magnetic flux passing through a surface of area A is Og = B · A· cose Normal to A The SI unit of magnetic flux is the Weber (Wb). Faraday law When a current conducting wire or coil is moved through a magnetic field a voltage (EMF) is generated which depends on the magnetic flux through the area of the coil. This is an example of the phenomenon of electromagnetic induction; the current that flows in this situation is known as an induced current. Faraday's Law relates the average induced EMF in terms of the time rate of change of the total magnetic flux through a current B cos e * - BA cos e = B A conductor or coil. ДФв = N- At Finally, if a coil has N turns, an emf will be produced that is N times greater than for a single coil, so that emf is directly proportional to N. The magnetic field strength (magnitude) produced by a long straight current-carrying wire is found by experiment to be B = where I is the current, r is the shortest distance to the wire, and the constant 40 = 47×107T · m/A is the permeability of free space. Magnetic field produced by a current-carrying circular loop. There is a simple formula for the magnetic field strength at the center of a circular loop. It is B = where R is the radius of the loop. One way to get a larger field is to have N loops; then, the field is B = N . 2. Electromagnetic field At every instant the ratio of the magnitude of the electric field to the magnitude of the magnetic field in an electromagnetic wave equals the speed of light. Ho! 2R Emax E Bmax B 3. Electromagnetic waves The magnitudes electric field strength E and magnetic field strength B in electromagnetic wave vary with x and t according to the expressions E (x, t) = E,sin(kx – wt) B(x, t) = B,sin(kx – wt) Here k = and w with A the wavelength and Tthe period of the wave (T=1/fwhere fis the frequency of oscillation of the wave). The speed of the wave is given by v=c = w /k. There are many types of waves, such as water waves and even earthquakes. Among the many shared attributes of waves are propagation speed v, frequency f, and wavelength 2. These are always related by the expression: v = af
Electromagnetic waves, like visible light, infrared, ultraviolet, X-rays, and gamma rays don't
need a medium in which to propagate; they can travel through a vacuum.
Speed of electromagnetic wave in vacuum
Taking the permittivity of free space ɛ, = 8.85 - 10-12 F/m and permeability of free space lo
= 4xx10 7 T-m/A , c = 3. 10° m/sec.
Table Electromagetik Waves
Life sclences
Type of EM
Issues
Production
Applications
wave
aspect
Communications
Remote controls
Requires controls for
band use
Radio & TV
Accelerating charges
MRI
Acelerating charges & thermal Communications Ovens Dep heating
agkation
Themal agitations & elecronic Thermal imaging
transitions
Microwaves
Cell phone une
Radar
Absorbed by
almosphere
Photosynthesis Human
vision
Intrered
Greenhouse efect
Heaing
Themal agkations & ekctronic
ransitions
Thermal agitations & electronic Sterilization Cancer
|алtions
mner elecronic transitions and Medical Security
fast collisions
Visitle
All pervasive
Ozone depletion Cancer
causing
Vitamin D production
Utraviolet
control
Medical diagnosis
Cancer therapy
Medical diagnosis
Cancer therapy
| X-аую
Cancer causing
Nuclear
medicinesecurity
Cancer causing
Radation damage
Gamma rays
Nuclear decay
4. Energy in eleetromagnetic wave
Electromagnetic waves can bring energy into a system by virtue of their electric and magnetic
fields. These fields can exert forces and move charges in the system and, thus, do work on them.
Once electromagnetic wave has created, the fields carry energy away from a source. Intensity
I of electromagnetic wave is energy per area A per time t or power P per area. Intensity is
measured in W/m²:1 = Energy –
The energy carried and the intensity I of an electromagnetic wave is proportional to E and B.
In fact, for a continuous sinusoidal electromagnetic wave, the average intensity I is given by
A-t
where c is the speed of light,
is the permittivity of free space, and Eo is the
maximum electric field strength.
The average intensity of an electromagnetic wave I can also be expressed in tems of the
magnetic field strength I =
5. Radiation pressure is the pressure exerted upon any surface due to the exchange of
momentum between the object and the electromagnetic field. The radiation pressure Pexerted
on the perfectly absorbing surface is: P =
6. The electromagnetic wave intensity at distance r from the source I = -
where Bo is the maximum magnetic field strength.
here P
is power.
Transcribed Image Text:Electromagnetic waves, like visible light, infrared, ultraviolet, X-rays, and gamma rays don't need a medium in which to propagate; they can travel through a vacuum. Speed of electromagnetic wave in vacuum Taking the permittivity of free space ɛ, = 8.85 - 10-12 F/m and permeability of free space lo = 4xx10 7 T-m/A , c = 3. 10° m/sec. Table Electromagetik Waves Life sclences Type of EM Issues Production Applications wave aspect Communications Remote controls Requires controls for band use Radio & TV Accelerating charges MRI Acelerating charges & thermal Communications Ovens Dep heating agkation Themal agitations & elecronic Thermal imaging transitions Microwaves Cell phone une Radar Absorbed by almosphere Photosynthesis Human vision Intrered Greenhouse efect Heaing Themal agkations & ekctronic ransitions Thermal agitations & electronic Sterilization Cancer |алtions mner elecronic transitions and Medical Security fast collisions Visitle All pervasive Ozone depletion Cancer causing Vitamin D production Utraviolet control Medical diagnosis Cancer therapy Medical diagnosis Cancer therapy | X-аую Cancer causing Nuclear medicinesecurity Cancer causing Radation damage Gamma rays Nuclear decay 4. Energy in eleetromagnetic wave Electromagnetic waves can bring energy into a system by virtue of their electric and magnetic fields. These fields can exert forces and move charges in the system and, thus, do work on them. Once electromagnetic wave has created, the fields carry energy away from a source. Intensity I of electromagnetic wave is energy per area A per time t or power P per area. Intensity is measured in W/m²:1 = Energy – The energy carried and the intensity I of an electromagnetic wave is proportional to E and B. In fact, for a continuous sinusoidal electromagnetic wave, the average intensity I is given by A-t where c is the speed of light, is the permittivity of free space, and Eo is the maximum electric field strength. The average intensity of an electromagnetic wave I can also be expressed in tems of the magnetic field strength I = 5. Radiation pressure is the pressure exerted upon any surface due to the exchange of momentum between the object and the electromagnetic field. The radiation pressure Pexerted on the perfectly absorbing surface is: P = 6. The electromagnetic wave intensity at distance r from the source I = - where Bo is the maximum magnetic field strength. here P is power.
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