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Deflecting particles

Posted in Physics, Charge and field
Contents

Particles can be deflected using both electric fields and magnetic fields. Deflecting beams of charged particles is required in multiple applications from television sets to circular accelerators.

Deflection by electric field

A beam of electrons, like that from an electron gun, can be deflected if they pass through an electric field.

Electric field deflection

From the revision topic on electric fields the strength of the uniform electric field between the two plates above is given by:

Dynamic image 0

The vertical (in this case downwards) force acting on the particles is given by:

Dynamic image 1

Combing the two equations gives the vertical force on a particle being deflected through a uniform electric field as:

Dynamic image 2

This equation and be combined with newtons second law (Dynamic image 3) to create an equation for the vertical acceleration of the particle in the beam:

Dynamic image 4

Dynamic image 2

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The stronger the field the more the particle will be deflected.

Worked example

A beam of electrons are deflected by an electric field made from two parallel plates 2.5cm apart with a potential difference of 1000V. Calculate (a) the strength of the electric field (b) the vertical force acting on the electrons in the beam and (c) the acceleration of the particles in the beam

(a) the strength of the electric field is calculated like so:
Dynamic image 8

(b) the vertical force is given by Dynamic image 9 where q, in this example is the charge on the electron (Dynamic image 10)
Dynamic image 11

(c) acceleration is given by Dynamic image 12 where m, the mass of an electron, is Dynamic image 13:
Dynamic image 14

This acceleration may seem very large however the value is given in seconds but the particles are only accelerated for nanoseconds.

Deflection by magnetic fields

Magnetic fields exert a force on a moving charge of magnitude:

Dynamic image 15

Where: Dynamic image 16 is the charge
Dynamic image 17 is the speed of the charge
Dynamic image 18 is the magnetic field strength

As this force acts perpendicular to the a particle's motion it is centripetal and causes the particle to curve in an arc of a circle. The equation for centripetal force is:

Dynamic image 19

In a uniform field this equation can be combined with the force on a charge in a magnetic field equation above:

Dynamic image 20

This equation can then be rearranged to allow the radius of the arc and speed of the particle to both be easily calculated.

Worked example

An electron travelling at 10% the speed of light is deflected using a magnetic field with a strength of 0.1Tesla. Calculate (a) the force on the electron and (b) the radius of the arc the electron follows

(a) Firstly the speed of the electron must be calculated:
Dynamic image 21

Then the force can be calculated:
Dynamic image 22

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(b) To calculate the radius the Dynamic image 24 equation is used:
Dynamic image 25

Dynamic image 26 Multiply by Dynamic image 27

Dynamic image 28 divide by Dynamic image 29

Dynamic image 30 Cancel out one of the Dynamic image 17

The radius can now be calculated:
Dynamic image 32

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