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Electrons are emitted by a hot filament ...

Electrons are emitted by a hot filament and are accelerated by an electric field as shown in figure .The two stops at the left ensure that the electron beam has a uniform cross-section.

A

Linear momentum of electron increases from A to B.

B

The electric current is from right to left

C

The magnitude of the current is same at A and B.

D

The current density is same at A and B.

Text Solution

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The correct Answer is:
A, B, C, D
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Knowledge Check

  • The de Broglie wavelength of an electron accelerated by an electric field of V volt is given by:

    A
    `lamda=(1.23)/(sqrt(m))`
    B
    `lamda=(1.23m)/(sqrt(h))`
    C
    `(1.23)/(sqrt(V))nm`
    D
    `lamda=(1.23)/(V)`.
  • A beam of electorn emitted from the electron gun G is accelerated by an electic field E . The area of cross-section of the beam remains constant. A the beam moves away from G

    A
    the speed of the electrons increases
    B
    the current constituted by the beam increases
    C
    the number of electrons per unit volume in the beam increases
    D
    the number of electrons per unit volume in the beam decreases
  • Following experiment was performed by J.J. Thomson in order to measure ratio of charge e and mass m of electron. Electrons emitted from a hot filament are accelerated by a potential difference V. As the electrons pass through deflecting plates, they encounter both electric and magnetic fields. the entire region in which electrons leave the plates they enters a field free region that extends to fluorescent screen. The entire region in which electrons travel is evacuated. Firstly, electric and magnetic fields were made zero and position of undeflected electron beam on the screen was noted. The electric field was turned on and resulting deflection was noted. Deflection is given by d_(1) = (eEL^(2))/(2mV^(2)) where L = length of deflecting plate and v = speed of electron. In second part of experiment, magnetic field was adjusted so as to exactly cancel the electric force leaving the electron beam undeflected. This gives eE = evB . Using expression for d_(1) we can find out (e)/(m) = (2d_(1)E)/(B^(2)L^(2)) A beam of electron with velocity 3 xx 10^(7) m s^(-1) is deflected 2 mm while passing through 10 cm in an electric field of 1800 V//m perpendicular to its path. e//m for electron is

    A
    `1.5 xx 10^(11)Ckg^(-1)`
    B
    `2 xx 10^(11)Ckg^(-1)`
    C
    `2.5 xx 10^(11)Ckg^(-1)`
    D
    `3 xx 10^(11)Ckg^(-1)`
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