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Experiment:
Measurement of Charge to Mass (e/m) ratio for Electron
Assigned By:
Dr. Kamran SB
Assigned To:
Muhammad Shahzad Rafiq
BS-PHY-18-26
Department Of Physics
Ghazi University
DGK
Calculations and Analysis
Data Acquisition
Acceptable Power Supplies
Apparatus Safety
Safety
Equipment Needed
History
Objectives
Outline
12/8/2020
2
Objectives:
Measure the ratio of the electron charge-to-mass ratio e/m by
studying the electron trajectories in a uniform magnetic field.
History:
J.J. Thomson first measured the charge-to-mass ratio of the
fundamental particle of charge in a cathode ray tube in 1897. The
charge-to-mass (e/m) ratio of the particles can be measured by
observing their motion in an applied magnetic field. Thomson repeated
his measurement of e/m many times with different metals for cathodes
and also different gases. Having reached the same value for e/m every
time, it was concluded that a fundamental particle having a negative
charge e and a mass 2000 times less than the lightest atom existed in
all atoms. Thomson named these particles “corpuscles” but we now
know them as electrons.
Formula:
12/8/2020
3
Equipment Needed:
• Pasco e/m apparatus (SE-9638)
• Pasco high voltage power supply for accelerating
voltage and filament heater.
• GW power supply for Helmholtz coils
• Two digital multi-meters
 Safety:
You will be working with high voltage make all
connections when power is off. Turn power off before
changing connections.
12/8/2020
4
 Apparatus Setup
12/8/2020
5
 Acceptable Power supplies setting:
• Electron gun / Filament heater: 6 V AC
• Electrodes: 150 to 400 V DC
• Helmholtz Coils: 6-9 V DC
 Data Acquisition:
a) Slowly turn the current adjust knob for the Helmholtz coils clockwise.
Watch the ammeter and take care that the current is less than 2 A.
b) Wait several minutes for the cathode to heat up. When it does, you
will see the electron beam emerge from the electron gun. Its
trajectory be curved by the magnetic field.
c) Rotate the tube slightly if you see any spiraling of the beam. Check
that the electron beam is parallel to the Helmholtz coils. If it is not,
turn the tube until it is. Don’t take it out of its socket. As you rotate
the tube, the socket will turn.
12/8/2020
6
d) Measurement procedure for the radius of the electron beam r:
For each measurement record:
Accelerating voltage Va
Current through the Helmholtz coils Ihc
Look through the tube at the electron beam. To avoid parallax
errors, move your head to align one side the electron beam ring with
its reflflection that you can see on the mirrored scale. Measure the
radius of the beam as you see it, then repeat the measurement on
the other side, then average the results. Record your result below.
To minimize human errors each lab partner should repeat this
measurement, then calculate the average value of the radius and its
uncertainty.
e) Repeat the radius measurements for at least 4 values of Va and
for each Va for 5-6 different values of the magnetic field.
12/8/2020
7
 Observation and Calculations:
1. Calculate e/m for each of the readings using Eq.
Use MKS units for calculations.
2. For each of the four Va settings calculate the mean < e/m >, the standard
deviation σ and the
standard error in the mean σm. Are these means consistent with one another
sufficiently that you
can combine them ? [Put quantitatively, are they within 2σ of each other ?]
Calculate the grand mean for all e/m readings, its standard deviation σ and the
standard error in the grand mean σm.
4. Specify how this grand mean compares to the accepted value.
5. Finally, plot the data in the following way which should, ( according to Eq. 5),
reveal a linear relationship: plot Va on the ordinate [y-axis] versus r2B2/2 on the
abscissa [x-axis]. The optimal slope of
this configuration of data should be < e/m >. Determine the slope from your plot
and its error. Do
6. Comment on which procedure gives a better value of < e/m > (averaging or
linear plot).
12/8/2020
8

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Determination of charge to mass ratio of an electron

  • 1. Experiment: Measurement of Charge to Mass (e/m) ratio for Electron Assigned By: Dr. Kamran SB Assigned To: Muhammad Shahzad Rafiq BS-PHY-18-26 Department Of Physics Ghazi University DGK
  • 2. Calculations and Analysis Data Acquisition Acceptable Power Supplies Apparatus Safety Safety Equipment Needed History Objectives Outline 12/8/2020 2
  • 3. Objectives: Measure the ratio of the electron charge-to-mass ratio e/m by studying the electron trajectories in a uniform magnetic field. History: J.J. Thomson first measured the charge-to-mass ratio of the fundamental particle of charge in a cathode ray tube in 1897. The charge-to-mass (e/m) ratio of the particles can be measured by observing their motion in an applied magnetic field. Thomson repeated his measurement of e/m many times with different metals for cathodes and also different gases. Having reached the same value for e/m every time, it was concluded that a fundamental particle having a negative charge e and a mass 2000 times less than the lightest atom existed in all atoms. Thomson named these particles “corpuscles” but we now know them as electrons. Formula: 12/8/2020 3
  • 4. Equipment Needed: • Pasco e/m apparatus (SE-9638) • Pasco high voltage power supply for accelerating voltage and filament heater. • GW power supply for Helmholtz coils • Two digital multi-meters  Safety: You will be working with high voltage make all connections when power is off. Turn power off before changing connections. 12/8/2020 4
  • 6.  Acceptable Power supplies setting: • Electron gun / Filament heater: 6 V AC • Electrodes: 150 to 400 V DC • Helmholtz Coils: 6-9 V DC  Data Acquisition: a) Slowly turn the current adjust knob for the Helmholtz coils clockwise. Watch the ammeter and take care that the current is less than 2 A. b) Wait several minutes for the cathode to heat up. When it does, you will see the electron beam emerge from the electron gun. Its trajectory be curved by the magnetic field. c) Rotate the tube slightly if you see any spiraling of the beam. Check that the electron beam is parallel to the Helmholtz coils. If it is not, turn the tube until it is. Don’t take it out of its socket. As you rotate the tube, the socket will turn. 12/8/2020 6
  • 7. d) Measurement procedure for the radius of the electron beam r: For each measurement record: Accelerating voltage Va Current through the Helmholtz coils Ihc Look through the tube at the electron beam. To avoid parallax errors, move your head to align one side the electron beam ring with its reflflection that you can see on the mirrored scale. Measure the radius of the beam as you see it, then repeat the measurement on the other side, then average the results. Record your result below. To minimize human errors each lab partner should repeat this measurement, then calculate the average value of the radius and its uncertainty. e) Repeat the radius measurements for at least 4 values of Va and for each Va for 5-6 different values of the magnetic field. 12/8/2020 7
  • 8.  Observation and Calculations: 1. Calculate e/m for each of the readings using Eq. Use MKS units for calculations. 2. For each of the four Va settings calculate the mean < e/m >, the standard deviation σ and the standard error in the mean σm. Are these means consistent with one another sufficiently that you can combine them ? [Put quantitatively, are they within 2σ of each other ?] Calculate the grand mean for all e/m readings, its standard deviation σ and the standard error in the grand mean σm. 4. Specify how this grand mean compares to the accepted value. 5. Finally, plot the data in the following way which should, ( according to Eq. 5), reveal a linear relationship: plot Va on the ordinate [y-axis] versus r2B2/2 on the abscissa [x-axis]. The optimal slope of this configuration of data should be < e/m >. Determine the slope from your plot and its error. Do 6. Comment on which procedure gives a better value of < e/m > (averaging or linear plot). 12/8/2020 8