moving charges and magnetism

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magnets

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53 Terms

1
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inside current carrying conductor, electric field is zero

The electric field inside a current carrying conductor is not zero; it is the electric field outside the conductor that is zero in static conditions.

2
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force on charge outside current carrying element must be zero at rest and constant velocity because electric field is zero

no, force on charge is not zero if it has constant velocity because the magnetic field may exert a force on the moving charge.

3
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tesla and gauss relation

1 T= 104 Gauss

4
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Magnetic field vector or scalar and unit and dimension

Vector

unit Tesla si and Gauss cgs

M1L0T-2A-1

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small current element IdL is vector or scalar

vector

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Biot savarts law

B= u0/4n IdLsin0/ r2

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vector form of biot savarts law

vector form

<p>vector form</p>
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permeability of free space numerical value and dimension

u0 = 4n x 10-7

MLT-2A-2

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permittivity e dimensional formula

M-1L-3T4A2

10
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Magnetic field characteristics

  1. long range field

  2. produced by vector component IdL unlike electric field which is produced by a scalar source charge q

  3. direction of B is perpendicular to position vector r and current element IdL

  4. medium dependent

  5. follow superposition theorem

  6. follows inverse square law

  7. it depends on angle

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magnetic field at centre of any circle upto angle theta

B= u0I/2R (0/2n)

for full circle u0I/2R

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magnetic field at centre for half circle, 1/4th circle and 120 degrees circle

u0I/ 4R

u0 I/8R

u0 I/6R

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  1. Magnetic field if n number of loops kept together keeping radius contant

  2. If same wire is bent into n loops

nB

n2B

14
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magnetic field due to finite straight wire

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magnetic field due to infinite straight wire

u0I/2pieR

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If concentric circles with radius r, 2r, 4r, 8r, 16r kept with dirn of current opposite in alternate circles. Find field at centre

u0I/3R

17
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If point taken at lower side of a finite wire then mag field

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18
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term image

dont panic with so many things just mark the direction of mag field by the two current elements

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the magnetic field does not depend on diameter of conductor only the distance between conductor and point

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Two current components I and nI are in same direction. Find distance from I where field will be zero

x= r/n+1

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Two current components I and nI are in different direction. Find distance from I where field will be zero

x= r/n-1

22
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field at centre of current carrying square

2root2 u0I /  nL

23
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field at centre of current carrying hexagon

root3 u0I /  nL

24
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three identical current carrying loops placed perpendicular to each other with current I and radius R. find mag field at centre

root3 u0I/2R

root2 u0I/2R if two circular loop

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term image

dimension dekh lo ya ye dekhlo ki distance d plane se perpendicular hai to root le lenge current i1 i2 ka

26
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field at centre of a square loop where current enters through a and exits through a

Bnet not equal to zero

only zero for current aana jana from different location

27
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<p>why Bnet not equal to zero in first case</p>

why Bnet not equal to zero in first case

because if we section it into 2 halves along the current then we get two unequal conductors of two width

28
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<p>find field due to arc abc</p>

find field due to arc abc

B= u0i1/2R (0/2n)

where i1 = i(2n-0) / 2n

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first mark direction of B1 and B2 then find resultant

30
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<p>Bnet at centre</p>

Bnet at centre

Bnet at centre is not zero as 3 arrows present

two current elements with opposite direction will get cancelled

31
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locus nikalne bola hai bss current and distance ka relation nikalo

32
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Magnetic field on axis of circular loop

u0IR2 /2(R2+x2)3/2

33
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graph for magnetic field on axis of ring

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34
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difference b/w gauss law and amperes cicuital law

flux through closed surface= o = E.dA = qin/ eo

this is gauss law for 3d objects like sphere cube cylinder

it is not always applicable to calculate elec field only for symmetrical charge distribution

B.dL= u0 Iin

this is amperes circuital law for loops like ring, square loop not for closed surface

always valid always applicable for symmetric current distribution

35
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magnetic field inside infinite hollow cylindrical wire carrying current i and outside mag field

B inside= 0

B outside= same as infinite wire

36
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magnetic field inside infinite solid cylindrical wire carrying current i and outside mag field

B= u0Ir/2pieR2

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<p>find B.dL for the loops</p>

find B.dL for the loops

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38
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term image

torque= MB sin0

MB sin0= NIA Bsin0

where N= no of turns

I= current

A= area

B= mag field strength

angle not 30o because area vector is up and not horizontal with magnetic field

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Torque is produced when there is uniform magnetic field and

emf is produced when there is change in magnetic flux so emf not produced

40
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torque and potential energy vector or scalar 

torque vector

potential energy scalar

41
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find time taken by circular loop to turn by angle 90 and become parallel to magnetic field

T= 2n |root i/MB| 

time to turn 360 degrees = T in shm

time for 90 degrees= T/4

so time taken= 2n |root i/MB| /4

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44
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angular speed of square coil if it turns by 90 degree and becomes parallel to magnetic field

each arm of square of mass m and length l

root 3iB/m

where i= moment of inertia

B= magnetic field

m= mass of arm

<p>root 3iB/m</p><p>where i= moment of inertia</p><p>B= magnetic field</p><p>m= mass of arm</p>
45
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angular speed of circular coil if it turns by 90 degree and becomes parallel to magnetic field

root 4niB/m

i= moment of inertia

m= mass

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