SlideShare une entreprise Scribd logo
1  sur  20
Gaurav Kumar Yogesh
413115003
Department of Physics
NIT –Trichy 620015
 In electrodynamics, changing electric and magnetic field with time.
 Fields are time variables.
 Static magnetic field produced by steady current and static electric
field produced by the charge at rest.
 If the current is time dependent the magnetic field is also time
dependent.
 Thus, if magnetic field is dependent then electric is also time
dependent.
)()()( tEtBtI 
 Electromotive force is work done
per unit charge.
 If we have a wire connected to a
battery then it is conducting and
battery supply the force then the
free charge in a wire are in motion
and produce work.
 dlE.
 Only the part AB will acts as a battery.
And current will flow from A to B.
 If the direction of motion of closed loop is
opposite then direction of flow of current is
also get opposite
dt
d
dsBm




 .
 dsfmag .
)(
)(
veVBf
veBVf
mag
mag

 If charge is positive
If charge is negative
R
VBh
R
v
iiRv
VBh
dlVB
dlfmag








 .
Ans. Due to motion of the motion of the disc the charge in
the motion. So the magnetic force per unit charge is
Because of this force, the charge moves toward the outer
edge. So outer edge of the terminal becomes the +ve
charge and centre becomes –ve charge.
If the disc rotates oppositely, the direction of force is
opposite. Then the charge on the centre is +ve and
surface is –ve.
Question: A metal disc of radius ‘a’ rotates with angular velocity w about vertical
axis through a uniform magnetic field B pointing in the upward direction. A circuit
is made By connecting to one end of resistor to the axle and other to the sliding
contact which touches the outer edge of the disc. Find the current in the resistance
in the resistor with direction




ˆ
)ˆˆ(
ˆ
rV
rzrV
rV
z




rrBf
zrBf
zBrf
BVf
mag
mag
mag
mag
ˆ
)ˆˆ(
ˆ







2
.
2
0
Ba
drrB
a




 
Ans: (a) The potential is
Inside the rod the current flow from B to A
(b) The magnetic force is
And the force is acting toward the left side of the bar.
Velocity of bar is exponentially decreases with time.
Question: A metal bar of mass m slides frictionally o two parallel conduction rails. A
distance l apart a resistor R is connected across the rails and a uniform mag. Field B is
pointing into the page
(a) Find the magnitude of current and magnetic force on the bar.
(b) If V0 is the speed at the t = 0, then what is the speed at later time t.
R
VBl
iVBl
dlfmag

 

 .
R
lVB
lB
R
VBl
f
BdlIf
mag
mag
22
. 
 
t
mR
lB
o
o
eVV
t
mR
lB
V
V
Ct
mR
lB
V
dt
mR
lB
V
dV
mR
lVB
dt
dV
R
lVB
dt
dV
m
22
22
22
22
2222
)ln(
ln






Ans : square loop is pulled upward direction.
Magnetic field due to a wire is
Where s is variable, if the s is increases the flux trough the wire is decreases.
Question: A square loop of wire of side ‘a’ lies on a table at a distance s from a very
long straight wire carries a current I. if someone pulls the loop away from the wire at
speed V. What is the induced emf in the loop and also find the induced current.
)ln(
2
2
ˆ
2
,0
s
as
a
I
dxdy
s
I
dxdyds
s
I
B
o
m
assy
ax
o
m
o

















dt
ds
s
a
as
s
a
I
dt
d
o
m
))((
2 2









 As the loop is moving away from the wire (=s) here the flux is decreases,
so the induced current is try to induced it and flux is decreasing due to the
decrease in the magnetic field.
 Field due to the induced current will try to increase the magnetic field , to
do so., it will develop magnetic field opposite to the original.
 If we pull the loop toward the ire the flux and B is increase, so current try to
decrease it.
 If we pull the loop away from the wire. The induced current in such a way
that it increase the current in wire.
 If the loop run parallel to the wire the then no emf will generate to the wire.
If the loop is state of rest and B is changing.
Then EMF is
so we have induced electric field only if we
have B is changing with time. Here E is not
a conservative force because curl of E in not
equal to zero.
E- field lines – open curves
B- field lines – closed curves
Field lines in the closed curves due to induced
electric field is
 Properties of induced electric firld
1. Non conservative
2. Non electrostatic
3. Closed Curve
4. is because there is no charge
corresponds to it otherwise
If both loop and magnetic field is changing
dt
Bd
E
dsB
dt
d
E
dsEdsB
dt
d
dlEdsB
dt
d
dlE
dt
d
dlE
dlE
m













0).)((
).(.
..
.
0.
.





0.  E
0.  E
o
E


.






dlBVdsB
dt
d
dlfdsB
dt
d
dlEdsB
dt
d
mag
.)(.
..
..



Ans: we have
B is not function of distance i.e., B is uniform. So flux is
Direction of current is changing accordingly Sin(wt).
Question: A long solenoid of radius ‘a’ is driven by an alternating current such that
field inside the solenoid is . A circular loop of wire or radius “a/2”
and resistance R is placed inside the solenoid and coaxial with it. Find the current
induced in the loop as function of time
ztCosBtB o ˆ)()( 
ztCosBtB o ˆ)()( 
R
tSin
a
B
R
i
tSin
a
B
dt
d
tCos
a
B
a
B
o
o
m
om
m
)()
4
(
)()
4
(
)()
4
(
)
4
.(
2
2
2
2

















 We have
Flux is changing with time, the emf of the loop is obtained as
The current producing such that the magnetic field is clockwise.
Note: Induced current always less than the original current
except the case of superconductor
Question: A square loop of wire with side ‘a’ lies in the 1st quadrant of x-y plane with
one corner at the origin. In this region there is non-uniform time dependent magnetic field
is coming out of the page. Where k is some constant. Find the induced
EMF in the loop.
ztkytyB ˆ),( 23

44
.
.
ˆ),(
5
2
4
2
0
,0
23
23
a
kt
a
akt
dxdytky
dsB
ztkytyB
m
ay
ax
m
m











ztkytyB ˆ),( 23

2
)
4
(
5
5
2
kta
a
kt
dt
d




Ans:
The end becomes the Positively charged at the end A.
Question: A metallic rod AB with uniform velocity v in a uniform magnetic field B as
shown in figure.
(a) The rod become electrically charged
(b) (b) The end A becomes +ve charged
(c) The end B becomes +ve charged
(d) The rod becomes hot because of the joule heating
Ans: we know that rod having the angular momenta in z
Direction
So answer (b) is the correct option
The potential difference between the A and B is zero.
A rod of length ‘a’ rotates with a uniform angular velocity ‘w’ about its perpendicular
bisector. A uniform magnetic field B exists parallel to the axis of rotation. The potential
Difference between the centre of the rod and end is
(a) 0
(b) 1/8(B.a.a.w)
(c) ½(wB.a. a)
(d) Bl2w
8
.
ˆ
)ˆˆ(
ˆ
2
2/
0
a
B
rdrB
dlf
rV
rzrV
z
ar
r
mag
















 Since the copper tube can be understand as circular wire, so the flux is change
in the motion of the magnet. As the magnet passes it emf such that, it ca resist
the motion of magnet at the first end of the tube and it will induce the emf at
the second end such that induce motion also resist the motion of the magnet
and the motion inside the tube is almost constant.
 So the magnet move with constant velocity
Question: A bar is released from the rest along the axis of a very long vertical copper tube.
After some time the magnet:
(1) Will stop in the tube
(2) Will move with almost constant speed
(3) Will move with an acceleration g.
(4) Will oscillate
Ans: Induced electric field
If
1. Here B is increases wit t, as flux also increases. S the induce current or induce
field try to decrease the flux. So it will opposite to actual current. So the
direction of the induce current is clockwise
2. If B is decrease with time the induce current is opposite of the previous case.
Question: A uniform magnetic field B(t) pointing in the direction fills the circular region
as shown in the figure. If B is changing with time. what is induced electric field.
dt
tdBs
E
s
dt
tdB
SE
s
dt
tdB
dlE
stB
dsB
dt
d
dlE
m
m
m
)(
2
.
)(
2.
.
)(
.
).(
.
.
2
2
2














zatB ˆ2

 Bo is constant not depending on time
Then flux is
Now B is switched off i.e., B = 0, & flux = 0,
Force required to rotate the charge, electric
field will do work for rotation of charge
electric force
Question: A line charge lambda is uniformly distributed on the rim of a wheel of a radius
B which is then suspended horizontally as shown in the figure & and it is free to rotate.
In the central region up to a radius ‘a’ there is a uniform magnetic field B pointing in the
Up direction . Suppose someone turned off the magnetic field, then what is the angular
velocity in the wheel.
2
. aBm  
Frtorque
dt
dB
a
dt
d
dlE
o
m



2
.


)(
)(
.
.
2
2
tdBbaLd
dt
tdB
ba
dt
Ld
N
dlEbN
dlEF
Ef












When B= Bo, L=0 & B= 0, L=L;
So,
And mvrL
BbaL
dBbadL
oB
L


 


2
0
2
0
mb
Ba 

2

B
Ans: So, Magnetic field inside
the solenoid is
 If B is in Z direction & Ein
(induced) will be in phi
direction
Question: A long solenoid with radius ‘a’ & n turns per unit length carries a time
dependent current I(t) in the direction. Find the electric field both direction and
magnitude at distance s from the axis both inside and outside the solenoid.











ˆ)(
2
)(
ˆ)(
)(2.
))((
ˆ)(
2
)(
ˆ)(
)(2.
ˆ)(
)(.
))((
)(
.
2
2
2
2
2
2
dt
tdI
s
an
E
dt
tdI
ansE
atIn
dt
tdIsn
E
dt
tdI
snsE
dt
tdI
sndlE
stIn
tInB
dt
d
dlE
o
o
om
o
o
o
om
o
m










 Outside: Flux =
Although the magnetic flux outside the
Solenoid is zero, but induced magnetic
Field is not zero
If current is increases with time then induced
current oppose the flux, if current decreases with
time then create the flux.




ˆ)(
2
)(
ˆ)(
)(2.
))((
2
2
2
dt
tdI
s
an
E
dt
tdI
ansE
atIn
o
o
om



s
EsE outin
1
, 
ˆ
Ans: we know that
Question: A square loop of side a & resistance R lies at a distance s from an infinite
Straight wire that carries a current I. Now someone cut the wire such that I drops to
Zero. In what direction induce current in loop will flow. And calculate the total charge
Passes a given point in the loop during this time of current flow.
)ln(
2
)ln(
2
)ln(
2
)ln(
2
)ln(
2
.
)ln(
2
)]ln(
2
[
2
ˆ
2
.
0
s
as
R
Ia
Q
dI
s
as
R
a
dQ
dt
dI
s
as
R
a
dt
dQ
dt
dQI
dt
dI
s
as
R
a
I
dt
dI
s
asa
RI
dt
dI
s
asIa
s
asIa
dt
d
dy
s
Ia
dt
d
dxdyds
s
I
B
dt
d
dlE
o
I
o
o
o
loop
o
loop
o
o
ass
as
o
o
m














































 Direction of the induced current– Anticlockwise
If current decreases, the flux decreases so the
Induced will try to increase the flux.
Ans: Area is fixed, B is also fixed but the angles changes.
Question: A square loop of edge a having ‘n’ turns is rotated with a uniform angular
Velocity ‘w’ about one of its diagonal in horizontal position as shown in this figure.
Find the induced EMF in the coil and also plot the graph between induced current and
phase with respect.
R
tSinBa
R
i
tSinBa
dt
d
tCosBa
CosBa
m
m
m
)(
)(
)(
2
2
2
2










Any Queries
???

Contenu connexe

Tendances (20)

Energy band and energy gap by Pratimesh pathak
Energy band and energy gap by Pratimesh pathakEnergy band and energy gap by Pratimesh pathak
Energy band and energy gap by Pratimesh pathak
 
ELECTRIC DIPOLE
ELECTRIC DIPOLEELECTRIC DIPOLE
ELECTRIC DIPOLE
 
Semiconductor Diode: Introduction and Application
Semiconductor Diode: Introduction and ApplicationSemiconductor Diode: Introduction and Application
Semiconductor Diode: Introduction and Application
 
Electric potential
Electric potentialElectric potential
Electric potential
 
current&current density
current&current densitycurrent&current density
current&current density
 
Capacitors
CapacitorsCapacitors
Capacitors
 
CAPACITANCE
CAPACITANCECAPACITANCE
CAPACITANCE
 
Semiconductors
SemiconductorsSemiconductors
Semiconductors
 
12.1 - Lenz's law
12.1  - Lenz's law12.1  - Lenz's law
12.1 - Lenz's law
 
Capacitor Presentation
Capacitor PresentationCapacitor Presentation
Capacitor Presentation
 
Electric Fields
Electric FieldsElectric Fields
Electric Fields
 
Electric charge and electric field
Electric charge and electric fieldElectric charge and electric field
Electric charge and electric field
 
Introduction to semiconductor materials
Introduction to semiconductor materialsIntroduction to semiconductor materials
Introduction to semiconductor materials
 
Maxwell's equations
Maxwell's equationsMaxwell's equations
Maxwell's equations
 
CAPACITORS AND CAPACITANCE
CAPACITORS AND CAPACITANCECAPACITORS AND CAPACITANCE
CAPACITORS AND CAPACITANCE
 
Electrostatics
ElectrostaticsElectrostatics
Electrostatics
 
CURRENT ELECTRICITY
CURRENT ELECTRICITYCURRENT ELECTRICITY
CURRENT ELECTRICITY
 
Band theory of solid
Band theory of solidBand theory of solid
Band theory of solid
 
Magnetic flux
Magnetic fluxMagnetic flux
Magnetic flux
 
Electric Fields
Electric FieldsElectric Fields
Electric Fields
 

En vedette

Menu du 20 au 24 marspower point
Menu du 20 au 24 marspower pointMenu du 20 au 24 marspower point
Menu du 20 au 24 marspower pointlorenzo62920
 
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017Deny Corkrey
 
Criterios y procedimientos evaluación 100715
Criterios y procedimientos evaluación 100715Criterios y procedimientos evaluación 100715
Criterios y procedimientos evaluación 100715Luz Alonzo
 
synthesis of doped chromium oxide nanoparticles
synthesis of doped chromium oxide nanoparticlessynthesis of doped chromium oxide nanoparticles
synthesis of doped chromium oxide nanoparticlesGaurav Yogesh
 
Electrodynamics
ElectrodynamicsElectrodynamics
ElectrodynamicsSiyavula
 
Role of biofertilizer in agriculture
Role of biofertilizer in agricultureRole of biofertilizer in agriculture
Role of biofertilizer in agricultureravi kiran
 
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)Electrostatics free notes for cbse xii by anurag tyagi classes (atc)
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)ANURAG TYAGI CLASSES (ATC)
 
Introduction to electrodynamics
Introduction to electrodynamicsIntroduction to electrodynamics
Introduction to electrodynamicsAhmed Haider
 
LAWS OF ELECTROSTATICS
LAWS OF ELECTROSTATICSLAWS OF ELECTROSTATICS
LAWS OF ELECTROSTATICSKANNAN
 
PART VII.1 - Quantum Electrodynamics
PART VII.1 - Quantum ElectrodynamicsPART VII.1 - Quantum Electrodynamics
PART VII.1 - Quantum ElectrodynamicsMaurice R. TREMBLAY
 
2015 Upload Campaigns Calendar - SlideShare
2015 Upload Campaigns Calendar - SlideShare2015 Upload Campaigns Calendar - SlideShare
2015 Upload Campaigns Calendar - SlideShareSlideShare
 
What to Upload to SlideShare
What to Upload to SlideShareWhat to Upload to SlideShare
What to Upload to SlideShareSlideShare
 
Getting Started With SlideShare
Getting Started With SlideShareGetting Started With SlideShare
Getting Started With SlideShareSlideShare
 

En vedette (18)

Menu du 20 au 24 marspower point
Menu du 20 au 24 marspower pointMenu du 20 au 24 marspower point
Menu du 20 au 24 marspower point
 
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017
SIM, Wahyudiyanto, Hapzi Ali, Akuntansi, Universitas Mercu Buana, 2017
 
Criterios y procedimientos evaluación 100715
Criterios y procedimientos evaluación 100715Criterios y procedimientos evaluación 100715
Criterios y procedimientos evaluación 100715
 
-kyc-2017
-kyc-2017-kyc-2017
-kyc-2017
 
synthesis of doped chromium oxide nanoparticles
synthesis of doped chromium oxide nanoparticlessynthesis of doped chromium oxide nanoparticles
synthesis of doped chromium oxide nanoparticles
 
13 media q3
13 media q313 media q3
13 media q3
 
Electrodynamics
ElectrodynamicsElectrodynamics
Electrodynamics
 
Role of biofertilizer in agriculture
Role of biofertilizer in agricultureRole of biofertilizer in agriculture
Role of biofertilizer in agriculture
 
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)Electrostatics free notes for cbse xii by anurag tyagi classes (atc)
Electrostatics free notes for cbse xii by anurag tyagi classes (atc)
 
Waveguides12
Waveguides12Waveguides12
Waveguides12
 
Introduction to electrodynamics
Introduction to electrodynamicsIntroduction to electrodynamics
Introduction to electrodynamics
 
LAWS OF ELECTROSTATICS
LAWS OF ELECTROSTATICSLAWS OF ELECTROSTATICS
LAWS OF ELECTROSTATICS
 
8.02 introduction to electrodynamics 3e-griffiths
8.02 introduction to electrodynamics 3e-griffiths8.02 introduction to electrodynamics 3e-griffiths
8.02 introduction to electrodynamics 3e-griffiths
 
Electrostatics
ElectrostaticsElectrostatics
Electrostatics
 
PART VII.1 - Quantum Electrodynamics
PART VII.1 - Quantum ElectrodynamicsPART VII.1 - Quantum Electrodynamics
PART VII.1 - Quantum Electrodynamics
 
2015 Upload Campaigns Calendar - SlideShare
2015 Upload Campaigns Calendar - SlideShare2015 Upload Campaigns Calendar - SlideShare
2015 Upload Campaigns Calendar - SlideShare
 
What to Upload to SlideShare
What to Upload to SlideShareWhat to Upload to SlideShare
What to Upload to SlideShare
 
Getting Started With SlideShare
Getting Started With SlideShareGetting Started With SlideShare
Getting Started With SlideShare
 

Similaire à Electrodynamics

[L2 Sambhav] Electro magnetic induction.pdf
[L2 Sambhav] Electro magnetic induction.pdf[L2 Sambhav] Electro magnetic induction.pdf
[L2 Sambhav] Electro magnetic induction.pdfSaptakPaul
 
(P206)sheet electromagnetic induction_e
(P206)sheet electromagnetic induction_e(P206)sheet electromagnetic induction_e
(P206)sheet electromagnetic induction_eAshutoshPrajapati16
 
physics121_lecture11.ppt
physics121_lecture11.pptphysics121_lecture11.ppt
physics121_lecture11.pptTehreemAkhtar9
 
Electromagnetism material
Electromagnetism materialElectromagnetism material
Electromagnetism materialUmang Suthar
 
Ch 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionCh 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionScott Thomas
 
Faraday’s Law of Induction.pdf
Faraday’s Law of Induction.pdfFaraday’s Law of Induction.pdf
Faraday’s Law of Induction.pdfDiegoBetancourt32
 
Magnetic effects of_electric_current(_ncert_questions)
Magnetic effects of_electric_current(_ncert_questions)Magnetic effects of_electric_current(_ncert_questions)
Magnetic effects of_electric_current(_ncert_questions)AlkaVarshney2
 
4m electromagnetic induction__alternating_currents
4m electromagnetic induction__alternating_currents4m electromagnetic induction__alternating_currents
4m electromagnetic induction__alternating_currentsPrayash Mohapatra
 
electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )Priyanka Jakhar
 
Electromagnetic Induction.pdf
Electromagnetic Induction.pdfElectromagnetic Induction.pdf
Electromagnetic Induction.pdfrajatrokade185
 
Electricity and Magnetism
Electricity and MagnetismElectricity and Magnetism
Electricity and Magnetismmaliraza215
 
Electricity and Magnetism
Electricity and MagnetismElectricity and Magnetism
Electricity and Magnetismmaliraza215
 
1 electromagnetic induction
1 electromagnetic induction1 electromagnetic induction
1 electromagnetic inductionKoncept Classes
 
Electromagnetic Induction Class 12
Electromagnetic Induction Class 12 Electromagnetic Induction Class 12
Electromagnetic Induction Class 12 Self-employed
 
electromagnetic induction
electromagnetic inductionelectromagnetic induction
electromagnetic inductionx6tence Pillai
 

Similaire à Electrodynamics (20)

[L2 Sambhav] Electro magnetic induction.pdf
[L2 Sambhav] Electro magnetic induction.pdf[L2 Sambhav] Electro magnetic induction.pdf
[L2 Sambhav] Electro magnetic induction.pdf
 
(P206)sheet electromagnetic induction_e
(P206)sheet electromagnetic induction_e(P206)sheet electromagnetic induction_e
(P206)sheet electromagnetic induction_e
 
Ch28 ssm
Ch28 ssmCh28 ssm
Ch28 ssm
 
physics121_lecture11.ppt
physics121_lecture11.pptphysics121_lecture11.ppt
physics121_lecture11.ppt
 
Electromagnetism material
Electromagnetism materialElectromagnetism material
Electromagnetism material
 
MU PHYSICS.docx
MU PHYSICS.docxMU PHYSICS.docx
MU PHYSICS.docx
 
MU PHYSICS.docx
MU PHYSICS.docxMU PHYSICS.docx
MU PHYSICS.docx
 
Ch 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionCh 22 Electromagnetic Induction
Ch 22 Electromagnetic Induction
 
Faraday’s Law of Induction.pdf
Faraday’s Law of Induction.pdfFaraday’s Law of Induction.pdf
Faraday’s Law of Induction.pdf
 
Magnetic effects of_electric_current(_ncert_questions)
Magnetic effects of_electric_current(_ncert_questions)Magnetic effects of_electric_current(_ncert_questions)
Magnetic effects of_electric_current(_ncert_questions)
 
Faraday’s Law.pdf
Faraday’s Law.pdfFaraday’s Law.pdf
Faraday’s Law.pdf
 
4m electromagnetic induction__alternating_currents
4m electromagnetic induction__alternating_currents4m electromagnetic induction__alternating_currents
4m electromagnetic induction__alternating_currents
 
electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )electromagnetic induction ( part 1 )
electromagnetic induction ( part 1 )
 
Electromagnetic Induction.pdf
Electromagnetic Induction.pdfElectromagnetic Induction.pdf
Electromagnetic Induction.pdf
 
Electricity and Magnetism
Electricity and MagnetismElectricity and Magnetism
Electricity and Magnetism
 
Electricity and Magnetism
Electricity and MagnetismElectricity and Magnetism
Electricity and Magnetism
 
Magnetic
MagneticMagnetic
Magnetic
 
1 electromagnetic induction
1 electromagnetic induction1 electromagnetic induction
1 electromagnetic induction
 
Electromagnetic Induction Class 12
Electromagnetic Induction Class 12 Electromagnetic Induction Class 12
Electromagnetic Induction Class 12
 
electromagnetic induction
electromagnetic inductionelectromagnetic induction
electromagnetic induction
 

Dernier

FREE NURSING BUNDLE FOR NURSES.PDF by na
FREE NURSING BUNDLE FOR NURSES.PDF by naFREE NURSING BUNDLE FOR NURSES.PDF by na
FREE NURSING BUNDLE FOR NURSES.PDF by naJASISJULIANOELYNV
 
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubai
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In DubaiDubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubai
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubaikojalkojal131
 
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...Universidade Federal de Sergipe - UFS
 
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》rnrncn29
 
Speech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxSpeech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxpriyankatabhane
 
The dark energy paradox leads to a new structure of spacetime.pptx
The dark energy paradox leads to a new structure of spacetime.pptxThe dark energy paradox leads to a new structure of spacetime.pptx
The dark energy paradox leads to a new structure of spacetime.pptxEran Akiva Sinbar
 
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdf
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdfBUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdf
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdfWildaNurAmalia2
 
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdf
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdfPests of Blackgram, greengram, cowpea_Dr.UPR.pdf
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdfPirithiRaju
 
Microphone- characteristics,carbon microphone, dynamic microphone.pptx
Microphone- characteristics,carbon microphone, dynamic microphone.pptxMicrophone- characteristics,carbon microphone, dynamic microphone.pptx
Microphone- characteristics,carbon microphone, dynamic microphone.pptxpriyankatabhane
 
Pests of soyabean_Binomics_IdentificationDr.UPR.pdf
Pests of soyabean_Binomics_IdentificationDr.UPR.pdfPests of soyabean_Binomics_IdentificationDr.UPR.pdf
Pests of soyabean_Binomics_IdentificationDr.UPR.pdfPirithiRaju
 
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuine
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 GenuineCall Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuine
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuinethapagita
 
Good agricultural practices 3rd year bpharm. herbal drug technology .pptx
Good agricultural practices 3rd year bpharm. herbal drug technology .pptxGood agricultural practices 3rd year bpharm. herbal drug technology .pptx
Good agricultural practices 3rd year bpharm. herbal drug technology .pptxSimeonChristian
 
Base editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingBase editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingNetHelix
 
User Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationUser Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationColumbia Weather Systems
 
Vision and reflection on Mining Software Repositories research in 2024
Vision and reflection on Mining Software Repositories research in 2024Vision and reflection on Mining Software Repositories research in 2024
Vision and reflection on Mining Software Repositories research in 2024AyushiRastogi48
 
Davis plaque method.pptx recombinant DNA technology
Davis plaque method.pptx recombinant DNA technologyDavis plaque method.pptx recombinant DNA technology
Davis plaque method.pptx recombinant DNA technologycaarthichand2003
 
Pests of Bengal gram_Identification_Dr.UPR.pdf
Pests of Bengal gram_Identification_Dr.UPR.pdfPests of Bengal gram_Identification_Dr.UPR.pdf
Pests of Bengal gram_Identification_Dr.UPR.pdfPirithiRaju
 
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRCall Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRlizamodels9
 
Harmful and Useful Microorganisms Presentation
Harmful and Useful Microorganisms PresentationHarmful and Useful Microorganisms Presentation
Harmful and Useful Microorganisms Presentationtahreemzahra82
 
Environmental Biotechnology Topic:- Microbial Biosensor
Environmental Biotechnology Topic:- Microbial BiosensorEnvironmental Biotechnology Topic:- Microbial Biosensor
Environmental Biotechnology Topic:- Microbial Biosensorsonawaneprad
 

Dernier (20)

FREE NURSING BUNDLE FOR NURSES.PDF by na
FREE NURSING BUNDLE FOR NURSES.PDF by naFREE NURSING BUNDLE FOR NURSES.PDF by na
FREE NURSING BUNDLE FOR NURSES.PDF by na
 
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubai
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In DubaiDubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubai
Dubai Calls Girl Lisa O525547819 Lexi Call Girls In Dubai
 
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...
REVISTA DE BIOLOGIA E CIÊNCIAS DA TERRA ISSN 1519-5228 - Artigo_Bioterra_V24_...
 
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》《Queensland毕业文凭-昆士兰大学毕业证成绩单》
《Queensland毕业文凭-昆士兰大学毕业证成绩单》
 
Speech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptxSpeech, hearing, noise, intelligibility.pptx
Speech, hearing, noise, intelligibility.pptx
 
The dark energy paradox leads to a new structure of spacetime.pptx
The dark energy paradox leads to a new structure of spacetime.pptxThe dark energy paradox leads to a new structure of spacetime.pptx
The dark energy paradox leads to a new structure of spacetime.pptx
 
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdf
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdfBUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdf
BUMI DAN ANTARIKSA PROJEK IPAS SMK KELAS X.pdf
 
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdf
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdfPests of Blackgram, greengram, cowpea_Dr.UPR.pdf
Pests of Blackgram, greengram, cowpea_Dr.UPR.pdf
 
Microphone- characteristics,carbon microphone, dynamic microphone.pptx
Microphone- characteristics,carbon microphone, dynamic microphone.pptxMicrophone- characteristics,carbon microphone, dynamic microphone.pptx
Microphone- characteristics,carbon microphone, dynamic microphone.pptx
 
Pests of soyabean_Binomics_IdentificationDr.UPR.pdf
Pests of soyabean_Binomics_IdentificationDr.UPR.pdfPests of soyabean_Binomics_IdentificationDr.UPR.pdf
Pests of soyabean_Binomics_IdentificationDr.UPR.pdf
 
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuine
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 GenuineCall Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuine
Call Girls in Majnu Ka Tilla Delhi 🔝9711014705🔝 Genuine
 
Good agricultural practices 3rd year bpharm. herbal drug technology .pptx
Good agricultural practices 3rd year bpharm. herbal drug technology .pptxGood agricultural practices 3rd year bpharm. herbal drug technology .pptx
Good agricultural practices 3rd year bpharm. herbal drug technology .pptx
 
Base editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editingBase editing, prime editing, Cas13 & RNA editing and organelle base editing
Base editing, prime editing, Cas13 & RNA editing and organelle base editing
 
User Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather StationUser Guide: Magellan MX™ Weather Station
User Guide: Magellan MX™ Weather Station
 
Vision and reflection on Mining Software Repositories research in 2024
Vision and reflection on Mining Software Repositories research in 2024Vision and reflection on Mining Software Repositories research in 2024
Vision and reflection on Mining Software Repositories research in 2024
 
Davis plaque method.pptx recombinant DNA technology
Davis plaque method.pptx recombinant DNA technologyDavis plaque method.pptx recombinant DNA technology
Davis plaque method.pptx recombinant DNA technology
 
Pests of Bengal gram_Identification_Dr.UPR.pdf
Pests of Bengal gram_Identification_Dr.UPR.pdfPests of Bengal gram_Identification_Dr.UPR.pdf
Pests of Bengal gram_Identification_Dr.UPR.pdf
 
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCRCall Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
Call Girls In Nihal Vihar Delhi ❤️8860477959 Looking Escorts In 24/7 Delhi NCR
 
Harmful and Useful Microorganisms Presentation
Harmful and Useful Microorganisms PresentationHarmful and Useful Microorganisms Presentation
Harmful and Useful Microorganisms Presentation
 
Environmental Biotechnology Topic:- Microbial Biosensor
Environmental Biotechnology Topic:- Microbial BiosensorEnvironmental Biotechnology Topic:- Microbial Biosensor
Environmental Biotechnology Topic:- Microbial Biosensor
 

Electrodynamics

  • 1. Gaurav Kumar Yogesh 413115003 Department of Physics NIT –Trichy 620015
  • 2.  In electrodynamics, changing electric and magnetic field with time.  Fields are time variables.  Static magnetic field produced by steady current and static electric field produced by the charge at rest.  If the current is time dependent the magnetic field is also time dependent.  Thus, if magnetic field is dependent then electric is also time dependent. )()()( tEtBtI 
  • 3.  Electromotive force is work done per unit charge.  If we have a wire connected to a battery then it is conducting and battery supply the force then the free charge in a wire are in motion and produce work.  dlE.
  • 4.  Only the part AB will acts as a battery. And current will flow from A to B.  If the direction of motion of closed loop is opposite then direction of flow of current is also get opposite dt d dsBm      .  dsfmag . )( )( veVBf veBVf mag mag   If charge is positive If charge is negative R VBh R v iiRv VBh dlVB dlfmag          .
  • 5. Ans. Due to motion of the motion of the disc the charge in the motion. So the magnetic force per unit charge is Because of this force, the charge moves toward the outer edge. So outer edge of the terminal becomes the +ve charge and centre becomes –ve charge. If the disc rotates oppositely, the direction of force is opposite. Then the charge on the centre is +ve and surface is –ve. Question: A metal disc of radius ‘a’ rotates with angular velocity w about vertical axis through a uniform magnetic field B pointing in the upward direction. A circuit is made By connecting to one end of resistor to the axle and other to the sliding contact which touches the outer edge of the disc. Find the current in the resistance in the resistor with direction     ˆ )ˆˆ( ˆ rV rzrV rV z     rrBf zrBf zBrf BVf mag mag mag mag ˆ )ˆˆ( ˆ        2 . 2 0 Ba drrB a      
  • 6. Ans: (a) The potential is Inside the rod the current flow from B to A (b) The magnetic force is And the force is acting toward the left side of the bar. Velocity of bar is exponentially decreases with time. Question: A metal bar of mass m slides frictionally o two parallel conduction rails. A distance l apart a resistor R is connected across the rails and a uniform mag. Field B is pointing into the page (a) Find the magnitude of current and magnetic force on the bar. (b) If V0 is the speed at the t = 0, then what is the speed at later time t. R VBl iVBl dlfmag      . R lVB lB R VBl f BdlIf mag mag 22 .    t mR lB o o eVV t mR lB V V Ct mR lB V dt mR lB V dV mR lVB dt dV R lVB dt dV m 22 22 22 22 2222 )ln( ln      
  • 7. Ans : square loop is pulled upward direction. Magnetic field due to a wire is Where s is variable, if the s is increases the flux trough the wire is decreases. Question: A square loop of wire of side ‘a’ lies on a table at a distance s from a very long straight wire carries a current I. if someone pulls the loop away from the wire at speed V. What is the induced emf in the loop and also find the induced current. )ln( 2 2 ˆ 2 ,0 s as a I dxdy s I dxdyds s I B o m assy ax o m o                  dt ds s a as s a I dt d o m ))(( 2 2         
  • 8.  As the loop is moving away from the wire (=s) here the flux is decreases, so the induced current is try to induced it and flux is decreasing due to the decrease in the magnetic field.  Field due to the induced current will try to increase the magnetic field , to do so., it will develop magnetic field opposite to the original.  If we pull the loop toward the ire the flux and B is increase, so current try to decrease it.  If we pull the loop away from the wire. The induced current in such a way that it increase the current in wire.  If the loop run parallel to the wire the then no emf will generate to the wire.
  • 9. If the loop is state of rest and B is changing. Then EMF is so we have induced electric field only if we have B is changing with time. Here E is not a conservative force because curl of E in not equal to zero. E- field lines – open curves B- field lines – closed curves Field lines in the closed curves due to induced electric field is  Properties of induced electric firld 1. Non conservative 2. Non electrostatic 3. Closed Curve 4. is because there is no charge corresponds to it otherwise If both loop and magnetic field is changing dt Bd E dsB dt d E dsEdsB dt d dlEdsB dt d dlE dt d dlE dlE m              0).)(( ).(. .. . 0. .      0.  E 0.  E o E   .       dlBVdsB dt d dlfdsB dt d dlEdsB dt d mag .)(. .. ..   
  • 10. Ans: we have B is not function of distance i.e., B is uniform. So flux is Direction of current is changing accordingly Sin(wt). Question: A long solenoid of radius ‘a’ is driven by an alternating current such that field inside the solenoid is . A circular loop of wire or radius “a/2” and resistance R is placed inside the solenoid and coaxial with it. Find the current induced in the loop as function of time ztCosBtB o ˆ)()(  ztCosBtB o ˆ)()(  R tSin a B R i tSin a B dt d tCos a B a B o o m om m )() 4 ( )() 4 ( )() 4 ( ) 4 .( 2 2 2 2                 
  • 11.  We have Flux is changing with time, the emf of the loop is obtained as The current producing such that the magnetic field is clockwise. Note: Induced current always less than the original current except the case of superconductor Question: A square loop of wire with side ‘a’ lies in the 1st quadrant of x-y plane with one corner at the origin. In this region there is non-uniform time dependent magnetic field is coming out of the page. Where k is some constant. Find the induced EMF in the loop. ztkytyB ˆ),( 23  44 . . ˆ),( 5 2 4 2 0 ,0 23 23 a kt a akt dxdytky dsB ztkytyB m ay ax m m            ztkytyB ˆ),( 23  2 ) 4 ( 5 5 2 kta a kt dt d    
  • 12. Ans: The end becomes the Positively charged at the end A. Question: A metallic rod AB with uniform velocity v in a uniform magnetic field B as shown in figure. (a) The rod become electrically charged (b) (b) The end A becomes +ve charged (c) The end B becomes +ve charged (d) The rod becomes hot because of the joule heating
  • 13. Ans: we know that rod having the angular momenta in z Direction So answer (b) is the correct option The potential difference between the A and B is zero. A rod of length ‘a’ rotates with a uniform angular velocity ‘w’ about its perpendicular bisector. A uniform magnetic field B exists parallel to the axis of rotation. The potential Difference between the centre of the rod and end is (a) 0 (b) 1/8(B.a.a.w) (c) ½(wB.a. a) (d) Bl2w 8 . ˆ )ˆˆ( ˆ 2 2/ 0 a B rdrB dlf rV rzrV z ar r mag                
  • 14.  Since the copper tube can be understand as circular wire, so the flux is change in the motion of the magnet. As the magnet passes it emf such that, it ca resist the motion of magnet at the first end of the tube and it will induce the emf at the second end such that induce motion also resist the motion of the magnet and the motion inside the tube is almost constant.  So the magnet move with constant velocity Question: A bar is released from the rest along the axis of a very long vertical copper tube. After some time the magnet: (1) Will stop in the tube (2) Will move with almost constant speed (3) Will move with an acceleration g. (4) Will oscillate
  • 15. Ans: Induced electric field If 1. Here B is increases wit t, as flux also increases. S the induce current or induce field try to decrease the flux. So it will opposite to actual current. So the direction of the induce current is clockwise 2. If B is decrease with time the induce current is opposite of the previous case. Question: A uniform magnetic field B(t) pointing in the direction fills the circular region as shown in the figure. If B is changing with time. what is induced electric field. dt tdBs E s dt tdB SE s dt tdB dlE stB dsB dt d dlE m m m )( 2 . )( 2. . )( . ).( . . 2 2 2               zatB ˆ2 
  • 16.  Bo is constant not depending on time Then flux is Now B is switched off i.e., B = 0, & flux = 0, Force required to rotate the charge, electric field will do work for rotation of charge electric force Question: A line charge lambda is uniformly distributed on the rim of a wheel of a radius B which is then suspended horizontally as shown in the figure & and it is free to rotate. In the central region up to a radius ‘a’ there is a uniform magnetic field B pointing in the Up direction . Suppose someone turned off the magnetic field, then what is the angular velocity in the wheel. 2 . aBm   Frtorque dt dB a dt d dlE o m    2 .   )( )( . . 2 2 tdBbaLd dt tdB ba dt Ld N dlEbN dlEF Ef             When B= Bo, L=0 & B= 0, L=L; So, And mvrL BbaL dBbadL oB L       2 0 2 0 mb Ba   2  B
  • 17. Ans: So, Magnetic field inside the solenoid is  If B is in Z direction & Ein (induced) will be in phi direction Question: A long solenoid with radius ‘a’ & n turns per unit length carries a time dependent current I(t) in the direction. Find the electric field both direction and magnitude at distance s from the axis both inside and outside the solenoid.            ˆ)( 2 )( ˆ)( )(2. ))(( ˆ)( 2 )( ˆ)( )(2. ˆ)( )(. ))(( )( . 2 2 2 2 2 2 dt tdI s an E dt tdI ansE atIn dt tdIsn E dt tdI snsE dt tdI sndlE stIn tInB dt d dlE o o om o o o om o m            Outside: Flux = Although the magnetic flux outside the Solenoid is zero, but induced magnetic Field is not zero If current is increases with time then induced current oppose the flux, if current decreases with time then create the flux.     ˆ)( 2 )( ˆ)( )(2. ))(( 2 2 2 dt tdI s an E dt tdI ansE atIn o o om    s EsE outin 1 ,  ˆ
  • 18. Ans: we know that Question: A square loop of side a & resistance R lies at a distance s from an infinite Straight wire that carries a current I. Now someone cut the wire such that I drops to Zero. In what direction induce current in loop will flow. And calculate the total charge Passes a given point in the loop during this time of current flow. )ln( 2 )ln( 2 )ln( 2 )ln( 2 )ln( 2 . )ln( 2 )]ln( 2 [ 2 ˆ 2 . 0 s as R Ia Q dI s as R a dQ dt dI s as R a dt dQ dt dQI dt dI s as R a I dt dI s asa RI dt dI s asIa s asIa dt d dy s Ia dt d dxdyds s I B dt d dlE o I o o o loop o loop o o ass as o o m                                                Direction of the induced current– Anticlockwise If current decreases, the flux decreases so the Induced will try to increase the flux.
  • 19. Ans: Area is fixed, B is also fixed but the angles changes. Question: A square loop of edge a having ‘n’ turns is rotated with a uniform angular Velocity ‘w’ about one of its diagonal in horizontal position as shown in this figure. Find the induced EMF in the coil and also plot the graph between induced current and phase with respect. R tSinBa R i tSinBa dt d tCosBa CosBa m m m )( )( )( 2 2 2 2          