14Motion of a charged particle in the magnetic field
Оценка 4.8

14Motion of a charged particle in the magnetic field

Оценка 4.8
pptx
07.05.2020
14Motion of a charged particle in the magnetic field
14Motion of a charged particle in the magnetic field.pptx

Lorentz force. Motion of a charged particle in the magnetic field 1

Lorentz force. Motion of a charged particle in the magnetic field 1

Lorentz force. Motion of a charged particle in the magnetic field

1

Learning objective To investigate the effect of a magnetic field on moving charged particles; 2

Learning objective To investigate the effect of a magnetic field on moving charged particles; 2

Learning objective

To investigate the effect of a magnetic field on moving charged particles;

2

Thompson’s experiment In 1897 JJ

Thompson’s experiment In 1897 JJ

Thompson’s experiment

In 1897 JJ Thomson set out to prove that cathode rays originating from a heated cathode (electron gun), were actually a stream of small negatively charged particles called electrons.
Electrons are accelerated from the cathode.
They are deflected by electric and magnetic fields.
The beam of electrons strikes a fluorescent screen.
e/m was measured.
Today we will learn more together about it!

The charge-to-mass ratio of an electron

The charge-to-mass ratio of an electron

The charge-to-mass ratio of an electron

Since the electrons are moving in a circle, there must be centripetal force
Question: Which force is acting as the centripetal force?
Answer: The magnetic force!
Therefore, since FM = FC
We can equate the equations and solve for e/m
Task: Try to derive an expression
for e/m.

Solution Therefore, Bqv = mv2/r

Solution Therefore, Bqv = mv2/r

Solution

Therefore,  Bqv = mv2/r
Re-arranging the terms,
q/m = v/Br
Question: Which variable is hard to
measure?

Answer Velocity However we get around this using the electron gun equation:

Answer Velocity However we get around this using the electron gun equation:

Answer

Velocity
However we get around this using the electron gun equation:

The ratio e/m for an electron – its specific charge – may be determined using a fine-beam tube

The ratio e/m for an electron – its specific charge – may be determined using a fine-beam tube

The ratio e/m for an electron – its specific charge – may be determined using a fine-beam tube.
The path of electrons is made visible by having low-pressure gas in the tube: the radius of the orbit may be measured.
By accelerating the electrons through a known potential difference V, their speed on entry into the region of the magnetic field may be calculated:

The magnetic field is provided by a pair of current-carrying coils (Helmholtz coils,

The magnetic field is provided by a pair of current-carrying coils (Helmholtz coils,

The magnetic field is provided by a pair of current-carrying coils (Helmholtz coils, Figure 2).
Combining the equations
q/m = v/Br and

Then specific charge on electron
Values for the charge e and m are usually given as

Figure 2

(D) Video demonstration

(D) Video demonstration

(D) Video demonstration

Velocity Selector Used when all the particles need to move with the same velocity

Velocity Selector Used when all the particles need to move with the same velocity

Velocity Selector

Used when all the particles need to move with the same velocity
A uniform electric field is perpendicular to a uniform magnetic field
Use the active figure to vary the fields to achieve the straight line motion
When the force due to the electric field is equal but opposite to the force due to the magnetic field, the particle moves in a straight line

Net force: The forces balance if the speed of the particle is related to the field strengths by qvB = qE v =

Net force: The forces balance if the speed of the particle is related to the field strengths by qvB = qE v =

Net force:
The forces balance if the speed of the particle is related to the field strengths by qvB = qE

v = E/B (velocity selector)

Mass Spectrometer A mass spectrometer separates ions according to their mass-to-charge ratio

Mass Spectrometer A mass spectrometer separates ions according to their mass-to-charge ratio

Mass Spectrometer

A mass spectrometer separates ions according to their mass-to-charge ratio.
In one design, a beam of ions passes through a velocity selector and enters a second magnetic field.
After entering the second magnetic field, the ions move in a semicircle of radius r before striking a detector at P.
If the ions are positively charged, they deflect to the left.
If the ions are negatively charged, they deflect to the right.

The mass to charge (m/q) ratio can be determined by measuring the radius of curvature and knowing the magnetic and electric field magnitudes

The mass to charge (m/q) ratio can be determined by measuring the radius of curvature and knowing the magnetic and electric field magnitudes

The mass to charge (m/q) ratio can be determined by measuring the radius of curvature and knowing the magnetic and electric field magnitudes.


In practice, you can measure the masses of various isotopes of a given atom, with all the ions carrying the same charge.
The mass ratios can be determined even if the charge is unknown.

(f) Formative assessment

(f) Formative assessment

(f) Formative assessment

Reflection What has been learned

Reflection What has been learned

Reflection

What has been learned
What remained unclear
What is necessary to work on

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