Paper 3 Section B: Turning points in physics June 2025, Question 1 16 marks
Also involves Errors and uncertainties · Equations of uniformly accelerated motion · Projectile motion · Electric fields and field strength · Charged particles in magnetic fields
This question is about Thomson’s determination of the electron’s specific charge.
You should not use the values of the electron charge, mass or specific charge from the data and formulae booklet in this question.
Figure 1 shows part of the apparatus that Thomson used to measure the specific charge of the electron.
A modern version of Thomson’s apparatus uses thermionic emission in the production of the electron beam.
Suggest how the electron beam is produced in this modern version. You should include a labelled diagram and suitable values for the power supplies used.
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A potential difference (pd) of 750 V is applied between the horizontal parallel plates. Figure 2 shows the plates and the path of the electrons.
The electrons enter the electric field between the plates at S and leave it at T with speed v. Beyond T the electrons travel in a straight line at an angle θ. θ is read from a scale on a fluorescent screen.
The plates are of length 10.0 cm and are separated by a distance of 5.00 cm.
A uniform magnetic field of flux density 0.640 mT is now applied between the plates. This returns the electron beam to its undeflected position.
Show that the horizontal component of the velocity of the electrons is approximately
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The magnetic field is switched off and θ is measured to be 25°.
Show that the vertical component of the velocity of the electrons at T is approximately
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Show that the vertical acceleration of the electrons between the plates is
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Determine a value for the specific charge of the electron.
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Explain the significance of the result of Thomson’s determination.
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Some students are given a version of the apparatus to repeat Thomson’s experiment.
Figure 3 shows a section of the measuring scale on the fluorescent screen and the spot from the electron beam.
The students consider two methods for minimising the percentage uncertainty in the measurement of the angle.
Method 1:
• choose a magnetic flux density B
• then set the magnetic flux density to B with no pd
• then adjust only the pd until the beam is horizontal
• then switch off the magnetic field and measure the angle θ.
Method 2:
• choose an angle θ
• then set the pd so that the spot from the electron beam is at θ with no magnetic field
• then adjust only the magnetic field until the beam is horizontal.
Discuss both of these methods with reference to the percentage uncertainty in θ that they will produce. In your answer, suggest which method will minimise the percentage uncertainty. No calculations are required.
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