Author: Nayan Jha

  • Force between two parallel current carrying linear conductors

    Force between two parallel current carrying linear conductors

    Force between two parallel current carrying linear conductors

    In this topic we will find the expression for Force between two parallel current carrying linear conductors when they are separated by some distance , and current flowing through them is in same direction ( also when current flowing through them is in different directions).

    Before to know about In this topic  expression for Force between two parallel current carrying linear conductors when they are separated by some distance, students must know the expression for current carrying conductors placed in uniform magnetic field. To know about this topic click here

    Force between two parallel current carrying linear conductors –

    Two long straight conductors are placed parallel two each other at distance ‘r’  and current flowing through them are I1 and I2 . Since each conductors are carrying current produces magnetic field and hence each conductor experience force on each other.

    As shown in figure (a) due to current I1 through C1D1­ magnetic field at a point P on the wire C2D2 is B1 , then   B1 =  μ0I1 /2∏r ,

    Since current flowing through the wire C2D2 is I2,

    Then force experienced on the wire C2D2 is given as ,

    F2 = B1 I2 l

    Then  , Force per unit length F2/l = B1 I2 = μ0I1I2 /2∏r (Towards left i.e. towards C1 D1) .

    Similarly , As shown in figure (b) due to current I2 through C2D2­ magnetic field at a point Q on the wire C1D1 is B2 , then   B2 =  μ0I2 /2∏r ,

    Since current flowing through the wire C1D1 is I1,

    Then force experienced on the wire C1D1 is given as ,

    F1 = B2 I1 l

    Then  , Force per unit length F1/l = B2 I1 = μ0I1I2 /2∏r (Towards right i.e. towards C2 D2) .

    So we can say if the current through each wire are in same direction then there will be force of attraction between them .

    If the direction of current in the both the wires are opposite then there will be force of repulsion between them, as shown in figure ( c )below, with the same force  μ0I1I2 /2∏r .

  • Complete assignment of magnetic effect of current

    Complete assignment of magnetic effect of current

    Complete assignment of magnetic effect of current

    In this assignment Complete assignment of magnetic effect of current all kind of questions , objective , short answer type questions, long answer type questions and all kind of numericals with hots questions.

    Before to solve this assignment students must know the syllabus  and notes related to this chapter magnetic effect of current.

    After solving these questions students will be able to solve the all kind of questions related to this chapter. Specially objective type question will help the students to solve the questions for all competitive examinations like JEE and NEET along with board examinations.

    TO download complete assignment of magnetic effect of current click here-

    Some of the examples of Multiple choice – ( Answers of all the multiple type questions given below ; after the multiple type questions)

    1. Magnetic induction is measured in:
    • (a)weber (b) weber/m
    • (c) weber/m2    (d) weber/m3
    1. The force acting on a charge q moving with a velocity ʋ in a magnetic field of induction B is given by:
    • (a)q/(ʋ ₓ B)   (b) (ʋ ₓ B)/q
    • (c) q/(ʋ ₓ B)  (d) (ʋ . B)q
    1. Two free parallel wire carrying currents in the opposite directions:
    • (a) attract each other
    • (b) repel each other
    • (c) do not affect each other
    • (d) get rotated to be perpendicular to each other
    1. Two parallel wires carrying currents in the same direction attract each other because of:
    • (a) potential difference between them
    • (b) mutual inductance between them
    • (c) electric forces between them
    • (d) magnetic force between them
    1. A free charged particle moves through a magnetic field. The particle may undergo a change in:
    • (a)speed         (c) direction of motion
    • (b)energy       (d) none these

    To download complete assignment of Complete assignment click on the link given below-

    complete assignment of magnetic effect of current

     

     

     

  • Force acting on the current carrying conductor placed in magnetic field

    Force acting on the current carrying conductor placed in magnetic field

    Force acting on the current carrying conductor placed in magnetic field

    In this topic we will discuss about Force acting on the current carrying conductor placed in magnetic field, where magnetic field is uniform and current carrying coil is laced at some angle with the magnetic field.

    Before to know about this topic students must know these topics –

    (i)force on a moving charged particle in uniform magnetic field and . To get the notes on this topic click here-

    (ii) Motion of a charged particle in uniform magnetic field . To get the notes on this topic click here-

    Force acting on the current carrying conductor placed in magnetic field –

    Suppose a cylinder of length ‘l’ area of cross-section ‘A’ carrying current ‘I’ , placed in uniform magnetic field ‘B’.

    Angle between them is ‘ϴ’ as shown in figure. If it is considered that ‘n’ is the number density of electron,Then total number of electrons present in the conductor is given as,

    N = A l n. [ where volume V = Al ]

    As we know when a charge moves in a magnetic force , force experienced on it is given by

    f =  q v B sinϴ  [ ϴ is the angle between v and B]

    so for each electron f=e vd B sinϴ ( where vd is the drift velocity of the electron) ‘,

    So, net force on the electrons F = Nf = N e vd B sinϴ =  Aln e vd B sinϴ = n e A vd l B sinϴ

    But we know from I = neAvd  ,

    So, we can write  F = I l B sinϴ……………eq.

    Special case-

    (i)  if ϴ=00 or 1800 then ,

    Force F = 0 . i.e. a linear conductor carrying current placed parallel or anti parallel to the magnetic field experience no force.

    (ii) If ϴ= 900 then, sinϴ=sin90 = 1

    Then force will be maximum given by F = BIl .

    The direction of the force is given by the Fleming’s left hand rule.

  • Lorentz force and velocity filter

    Lorentz force and velocity filter

    Lorentz force and velocity filter

    In this topic we will discuss about Lorentz force and velocity filter.In which we will know different conditions for Lorentz force and complete explanation of velocity filter .

    Lorentz force-

    The force experienced by a charged particle due to both electric and magnetic field at a space called Lorentz’s force .

    Suppose a charge particle of mass ‘m’ and charge ’q’ is moving in the both electric and magnetic field of Field intensity ’E’ and ‘B’ respectively.

    Then force due to electric field is given as Fe= q E

    And force due to magnetic field will be Fb=  q v B sinϴ ( where ϴ is the angle between v and B).

    Then, Lorentz force F = FE+FB  = q( E + v B sinϴ)………………Eq.

    Special cases –

    Case 1- When v , E and B all are collinear –

    In this case Fe = q E ,

    And Fb= o ( since ϴ= 0 ; sin 0 = 0 )

    acceleration a = Fe/m =  qE/m ,

    case 2 – When v , E and B are mutually perpendicular to each other –

    then net force F = Fe +Fb = 0

    therefore acceleration  a= 0 . It means particle will move without any deflection with the same velocity .

    Velocity filter –

    It is an arrangement of cross electric and magnetic field in a space which help to select from a beam , charged particles of given velocity irrespective of their charge and mass.

    It consist two slits S1 and S2 placed parallel , with common axis at some distance . Uniform electric field ( E ) and magnetic field(B) applied  which are perpendicular to each other , which is shown in figure. When a beam of charged particles of different charges and masses after passing through S1 enters into the region where crossed electric and magnetic field are present . The particles which is moving with velocity ‘v’ the electrostatic force and magnetic force are equal and opposite , then    q E = q v B   ,

    Or, v= E/B

    Such kind of particles go without changes its path and filtered out the region through the slits S2. Therefore the particles emerging from S2 will have the same velocity even though their charges and masses may be different.

    Velocity filter is used in mass spectrograph which help to find the mass and specific charge of the charged particle.

     

     

  • Motion of a charged particle in uniform magnetic field

    Motion of a charged particle in uniform magnetic field

    Motion of a charged particle in uniform magnetic field

    In this topic Motion of a charged particle in uniform magnetic field we will discuss about how a charged particle moves in uniform magnetic field, when it is projected with some velocity at an angle with magnetic field.

    Before to know about this topic students must know about the force acting on a charge particle when it moves in a uniform magnetic field. To know about this topic force on a charge particle in uniform magnetic field click here.

    Motion of a charged particle in uniform magnetic field –

    Suppose a charged particle of mass ‘m’ and charge ‘q’ is projected  with velocity ‘v’ at angle ‘ϴ’ with the magnetic field  ‘B’ as shown in figure (a) . Here v has two components  (v1= vcosϴ ) along x -axis and ( v2= v sinϴ) along y-axis.

    Due to v1 it moves along x-axis and due to v2 a force F acts which is given as F = qv2 B = qvBsinϴ. Since this force F acts perpendicular to the velocity and magnitude of v2 not changes hence it moves on a circular path.  As shown in fig(b).

    let r is the radius of the circular path , due to these two components of v1 and v2 particle follows a helical path as shown in fig(a) .

    As we know when body moves on a circular path the centripetal forc F = mv22/r = mv2sin2ϴ/r ;

    Which is provided by magnetic force F= qvBsinϴ

    So we can write  mv2sin2ϴ/r = qvBsinϴ;

    So, r = mvsinϴ/qB ……………….(1)

    or vsinϴ=qBr/m …………………….(2)

    angular velocity  ω= vsinϴ/r = Bqr/mr = Bq/m ……………..(3)

    here frequency  f=ω/2∏ = Bq/2∏m  ( here frequency is independent of velocity)………….(4)

    and time period T = 1/f = 2∏m/Bq ……………………………(5).

    The pitch of the helix = vcosϴ x T = v cosϴ 2∏m/Bq .

    Special cases –

    Case (i) -If ϴ=00 i.e. v1=v and v2=0

    So there will be no force and particle will move in the direction of B .

    Case (ii) – if ϴ=900 then v1=0 and v2=v  i.e. body will move only in the circular path

    And radius of the circular path  r= mv/qB  or  r= v/(q/m)B .

     

  • Newton’s second law of motion is the real law of motion

    Newton’s second law of motion is the real law of motion

    Newton’s second law of motion is the real law of motion

    Before to know Newton’s second law of motion is the real law of motion we must know all three equations of motion.

    To know, Newton’s first law of motion click here–

    To know, Newton’s second law of motion click here-

    To know, Newton’s third law of motion click here-

     

    Second law of motion  is the real law of motion –

    The question may be asked as , show that second law of motion is the real law of motion . 

    ***This question is very important for the class 11th examination point of view .

    To show it we must prove two things (i) First law contained in the second law and (ii) Third law contained in second law.

    (i) ) First law contained in the second law –  As we know according to Newtons second law of motion

    Force F = Ma ,

    If there is no external force

    then F = 0

    Or, Ma =0    then we can say    M=0 or a=o , but mass of the body can’t be zero.

    Therefore only possible thing is that only acceleration is zero .

    But , we know acceleration a= v-u/t ( where , v- final velocity and  u- initial velocity) .

    So we can write , v-u/t = 0  i.e v-u=0 or v=u

    Since V (final velocity) = u ( initial velocity).

    So we can say if body initially is in rest will be in rest and if it is moving with some velocity it will remain in the motion with the same velocity( which is the statement of first law ) . So we can say first law contained in the second law .

    To watch the video of this topic Newton’s second law is the real law of motion , click on the link given below-

    (ii) Third law contained in the second law –  suppose an isolated system of two objects A and B , they interact mutually with one another . Then obviously they will apply force on each other .

    Let,  FAB – Force on A due to B ,

    And  FBA – Force on B due to A .

    Let dpa and dpb is the change in momentum in A and B respectively in small time dt .

    Then from Newton’s second law –

    FAB = dpA/dt   ………………………(i)

    and, FBA= dpB/dt …………………..(ii)

    FAB+ FBA= dpB/dt + dpA/dt   ……….(iii)

    In the absence of external force , the rate in change in momentum of the system will be zero .

    i.e. dpB/dt + dpA/dt  = 0

    Therefore , FAB+ FBA=0 ;

    Or, FAB= -FBA ( which is third law )

    So we can say Newtons third law contained in the second law .

    Therefore we can say Newton’s second law of of motion is the real law of motion.

    What is the syllabus removed in class 12th physics (CBSE) for 2021 board examination , click on the link given below-

     

     

  • Apparent weight of a man in a lift

    Apparent weight of a man in a lift

    Apparent weight of a man in a lift

    In this topic we will discuss about , a man of mass m standing in a lift . What will be its apparent weight of a man in a lift when lift has some motion with uniform acceleration or velocity?

    But before to know about this topic students must know Newton’s third law of motion. To get the notes on Newton’s third law of motion click here-

    Apparent weight of a man in a lift  (elevator)  –

    Suppose a man of mass ‘m’ is standing on a weighing machine placed inside a lift . initially when the lift is in rest weight of the man acts vertically downward direction which acts on the   weighing machine and machine offers a resistance ‘R’ against its weight shows the actual weight which is mg .

    Case i – When the lift is in rest or moving with uniform velocity (fig-c)- In that case there is no acceleration in the lift and man , and hence reaction force is equal to the weight of the man.

    In that case , R  = mg

    i.e  Apparent weight = Actual weight

    Case ii – When lift moves upward with acceleration ‘a’ fig (a).

    Since there is upward motion then  ;

    So  R-mg =ma

    Or , R = mg+ma = m(g+a)

    i.e. R ( apparent weight) > mg(actual weight) ;

    i.e  Weighing machine shows more weight the actual .

    Case iii – When lift moves downward with acceleration ‘a’ fig (b).

    Since there is downward motion then  ;

    So  mg-R =ma

    Or , R = mg-ma = m(g-a)

    i.e. R ( Apparent weight) < mg(Actual weight) ;

    i.e  Weighing machine shows less weight the actual .

    case iv– When the lift falls freely –  In that case lift accelerates downward with acceleration ‘a=g’

    So we can write , R= mg-ma = mg-mg ( since a=g) = o

    Show apparent weight of the man will be zero . So person feel’s weightlessness.

     

  • Horse and cart problem

    Horse and cart problem

    Horse and cart problem

    This is the topic  Horse and cart problem which explain the one of the important illustration of Newton’s third law of motion.

    But before to learn the topic Horse and cart problem students must know, Newton’s third law of motion. To get the notes on Newton’s third law of motion click here-

    To get the Notes on Newton’s first law and inertia click here-

    To get the Notes on Newton’s second law and impulse click here-

    Horse and cart problems –

    Suppose a cart is connected  with a  horse by a light inextensible string. When horse start to walk horse press the ground F ( action ) with their feet in the slightly backward direction and ground  exert an equal reaction R , as shown in figure . then R has two component H = R cosϴ in horizontal direction  and V= R sinϴ in vertical direction . V balance the weight of the horse and H makes the horse to move in forward direction . While pulling the cart produces a tension T in the string .

     

    If H > T then cart starts moving in the forward direction with acceleration ‘a’ .

    Net force acting on the horse = H-T= ma.( where m is the mass of the horse)……………..(i)

    If f is the frictional force between tyre of cart and ground then for cart we can write

    T-F= Ma  ( M is the mass of the cart ) …………………………(ii)

    From equations (i) and (ii) we get ,

    H-f = ( M+m ) a ;

    So, acceleration   a  =  H-f/ (M+m ) ;

    The whole system will move if H>f ;

     

  • Newton’s third law of motion

    Newton’s third law of motion

    Newton’s third law of motion

    In this topic we will discuss about Newton’s third law of motion and some important illustrations of Newton’s third law of motion .

    Before to go with this topic students must know Newton’s first and second law .

    For Newton’s first law and inertia click here-

    For Newton’s second law and impulse click here-

     

    Newton’s third law of motion-

    According to this law every action has equal and opposite reaction.

    Forces in nature always occur between pairs of bodies. Let two objects A and B colliding as shown in figure.

    FAB force on A due to B ,and FBA force on B due to A .

    Then according to Newton’s third law of motion FAB = -FBA .

    For example- When a man walk on the ground then man push the road backward and road push the man in forward direction. This example shows , single force never exist and force always exist in pair.

    Important point of Newton’s third law we must know –

    (i) Action and reaction always acts on different bodies.

    (ii) No action occur without reaction.

    (iii) Action and reaction can’t cancel each other.

    (iv) action and reaction may be mechanical, gravitational, electrical or of any other nature.

    Some important illustration of Newton’s third law of motion.-

    1. Object kept on the table – suppose an object of mass ‘m’ placed on the table , then the weight ‘W’ applying a force equal ti its weight W = mg,  on the surface of table , and table applying a reaction R on the book , In this condition W = -R.

    1. 2. Walking of a man on the ground –

    While walking we press the ground F ( action ) with our feet in the slightly backward direction and ground  exert an equal reaction R , as shown in figure . then R has two component H = R cosϴ in horizontal direction  and V= R sinϴ in vertical direction . V balance the weight of the man and H makes the man to move in forward direction .

    1. It is difficult to walk on the slippery ground or sand-  It is because we are unable to push such a ground sufficiently hard . As a result force of reaction is not sufficient to help a person move in forward direction.
    2. While swimming , a person pushes water with his hand in the backward direction and water in turns reacts and pushes the swimmer in forward direction.
  • Newton’s second law of motion and Impulse

    Newton’s second law of motion and Impulse

    Newton’s second law of motion and Impulse

    In this topic Newton’s second law of motion and Impulse  , we will explain Newton’s second law of motion , expression for force, Impulse and application of concept of impulse . The reasoning questions of this topic and numericals ( specially based on Impulse) is very important for class examination and also for other competitive examination like JEE/NEET .

    But before to know this topic, it is necessary the students must  have the concept of Newtons first law of motion and inertia .                                                                                                    For  the notes on Newton’s first law and inertia click here- 

    Newtons second law of motion and impulse –

    As we know from Newton’s first law of motion ‘every body remain in its position of rest or of uniform motion in a straight line , till no external force acts on it’ . Just think what will happen when external force acts on the body . This effect of  acting a force on the body is described by Newton’s second law of motion .

    To watch the video on Newton’s second law – click on the link given below-

     

    Newtons second law of motion ( Force law)-

    Newton’s second law of motion states that , when an external force applied on a body , then rate in change in momentum is directly proportional to the applied force , and change takes place in the direction of applied force . this law is also known as the law of force.

    We have to take care of its two parts (i) rate of change of momentum is directly proportional to the applied force and , (ii) change in momentum occurs in the direction of applied force .

    Expression of force from newtons second law of motion –

    Let a body of mass ‘m’ moving with velocity ‘v’ .

    Then , its linear momentum will be  p = mv ;

    As newton’s second law states  force F α dp/dt   ;  or  F= k dp/dt  ……………..(i)

    But here ,  p=mv .

    So putting this value of p in equation (i) we get

    F=k d(mv)/dt =k m (dv/dt) = k ma; [where dv/dt=a( acceleration) ],

    Experimentally it is found k=1

    So we can say,  F =ma ;

    Unit of force is  kg-m/s2  or kg-ms-2 OR Newton (N)

    Its dimension is  [ M L T-2] ;

     

    IMPULSE-

    To know the impulse we must know . What is impulsive force?

    Impulsive force – It a large force acts on a body for short time which is the cause of change in momentum . example-  Blow a hammer on a nail, force exerted by a bat when it hits a ball, etc.

    Impulse – When a large force acts on a body for short time which is the cause of change in momentum, then the product of force and time for which it acts on the body is called impulse or Impulse of force which is equal to the change in linear momentum of the body.

    So we can write impulse I = Fav. x  t   = Pf – Pi = Δp

    Proof–   From Newton’s second law we know ;

    Force F = dp /dt  ;

    But momentum P = mv ( m- mass of the body and v is its velocity);

    So we can write  F dt = dp ;

    Integrating both sides with appropriate limits we get ,

    ∫ Fdt =∫dp = p2-p1 

    Or ,  Fav.t = p2-p1  = I

    So we can say if the force varying with time ( or force is the function of time ) then we can write

    Impulse I = ∫F dt .

    If we plot the force v/s time curve , then the area under the curve gives the impulse .

    A. When a constant force acts on a body then force v/s time graph is given below . the area under the line AB gives the impulse .

    B. When a variable force acts on a body then force v/s time graph is given below . the area under the line ABC gives the impulse ;

    The unit and dimension of the impulse is same as linear momentum .

    Application of concept of impulse – ( It also work as reasoning questions in your class examinations)

    (a) Automobiles are provided with shockers.

    (b) China wares are packed under straw paper.

    (c) A cricket players lower his hand while catching a ball.

    (d) A person falling from a certain height gets more injuries when he falls on a cemented or tough floor than when he falls from a heap of sand.

    If we goes to the reason of all the points mentioned above then answers of all the questions will be same .

    As we know,  impulse = F x t = change in momentum

    For the same impulse force F = impulse / time . i.e. F α 1/t

    when time of impact increases due to some processes then force acts on the body decreases .

    To watch of the video of this topic click here-