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MAGNITISM (ANYLISIS OF MAGNETIC FIELD BY BY DIFFRENT TYPES OF CURRENT…

- - - - WIRE FORMULA DERIVATION :question:
      - INFINITE WIRE
      - SEMI INFINITE WIRE
        
        AT BASE
        
        ANY OTHER POINT
      - PROBLEMS BASED ON FINDING MAGNETIC FIELD AT OTHER POINTS OF WIRE
        
        PROBLEMS ON DIFFRENT ARRANGMENT OF WIRE , SEMI INFINITE , INFINTE WIRE
        
        N POLYGON PROBLEMS
    - - MAGNETIC FIELD DUE TO CIRCLE :question:
        
        MAGNETIC FIELD DUE TO ARC :question:
        
        PROBLEMS ON COMBINATION OF ARC AND ANY WIRE
        
        FIELD DUE TO ARRANGMENT OF RING,WIRE,ARC AT A POINT
      - DIRECTION
    - - INFINITE SOLONOID FIELD FORMULA :question:
        
        FIELD DIAGRAM
      - IDEAL SOLONOID FORMULA :question:
      - SOLONOID DERIVATION FORMULA AND HOW TO APPLY IT :question:
        
        MAGNETIC FIELD DIGRAM
  - - - DERIVATION OF FIELD BY AMPERS LAY
        
        WIRE HAVING CROSS SECTIONAL AREA
        
        FIELD BY TO SOLID WIRE
        
        OUTSIDE DERIVATION FORMULA :question:
        
        INCIDE DERAVATION FORMULA :!!: :question:
        
        WHEN J IS VARYING
        
        GRAPH
        
        FIELD DUE TO HOLLOW WIRE
        
        INCIDE THE HOLLOW AREA
        
        OUTSIDE
        
        ON THE HOLLOW SURFACE
        
        INTEGRATION IS INVOLVED
        
        GRAPH
        
        CAVITY PROBLEM
        
        MAGNETIC FIELD INCIDE NOT IN CAVITY REGION
        
        formula :question:
        
        field is constat incide cavity
        
        INCIDE CABITY
        
        OUTSIDE CAVITY
    - - FIELD INCIDE
      - OUTSIDE
      - INCIDE TORROID
  - - - FORMULA :question:
- - - - the particle will go straing withe acclaration due to electric field
      - what is acc due to electric field :question:
    - - helical path with increasing pirch
        
        the partical will do circulat and give T,R,F,angular velocity and etc sclar parameters
        
        in the parallel direction the motion will go on under consteant acc
        
        r as a function of t
    - - take components
        
        apply case of 90 to one
        
        the other will act as the inital velocity of the constant acc
        
        r as a function of t
  - - - diagram
      - frequency
      - total kinitic enery at lase
    - - magnetic and electric field anr crose a t90
      - formula
- - - - WHEN ANGLE IS 90 (including vector form)
        
        the motion is uniform circular
        
        radius :question:
        
        time period :!!: :!: :question:
        
        angular velocity :question:
        
        frequency :question:
        
        equ as r varies with time
        
        all the previus were sclar
        
        did not tell about he directio of circle
        
        the angle bw the field and velocity was 90 but still the velocity can have diffrent directions
        
        the veocity and filed can be give in i j just take magnitude the notation will tell the angle
        
        ALL THE PROBLEMS OF UNIFORM CIRCULAR MOTION IS APPLICABLE
      - WHEN ANGLE IS 0
        
        the particle will go undivated
        
        all the kinimatics problems can fool you
      - WHEN IT IS MAKING ANY OTHER ANGLE
        
        the path is helical
        
        take components of the velocity of in in i j notation take the ones not in direction of field
        
        the two components one in direction of field of perpenducular to it
        
        to the 90 component apply all the 90 casse
        
        to the other compone just dose not change goes forward
        
        pitch of helix :question:
        
        r as a function of t
      - WHEN ONLY A PART OF REGION IS FIELD
        
        all the facts of the circle apply
        
        angle of devation case :question:
        
        FINDING THE TIME INCIDE AND ETS BY CIRCULAR MOTION CASE