PCS 130 Lab report 1 Charge to Mass Ratio

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Toronto Metropolitan University *

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130

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Apr 3, 2024

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Lab 1: Charge to Mass ratio of an Electron Nayalash Iqbal (501156321), Muskaan Bajwa (501255858) Toronto Metropolitan University PCS 130 - 091 Dr Vladislav Toronov Date of Laboratory: January 31st 2024 Date of submission: February 7th 2024
Introduction In the 1800s, a physicist by the name of Sir J.J Thomas worked at the Cavendish laboratory in Cambridge England. One day, while working on his experiments, he came across a fascinating discovery, the electron. Thomas’s discovery was prodigious. His work has become a truly important part of modern day science. Sir J.J. Thomas performed an experiment that involved the use of a cathode ray discharge tube containing electrodes at each end. The electrode is connected to a negative terminal of a battery, the cathode. The other is connected to the positive terminal of the battery, the anode. To control the pressure of gas inside the tube, it is connected to a vacuum pump. When electricity is passed through the tube, rays are emitted from the cathode towards the anode. When rays hit the walls of the discharge tube, fluorescence is produced. Thomas realized that the charge to mass ratio of the cathode rays were the same as for an electron. Therefore, the negatively charged particles in an atom are electrons. This lab is a replication of Sir J.J Thomas’s experiment in modern day. Theory When a charged particle moves through a uniform magnetic field, the velocity then travels in a circular path. The circular motion can be described by using the force exerted by a magnetic field and Newton’s second law of motion which can be expressed in terms of: Where “F” represents the force on the charged particle which is measured in newtons, “q” is known for the charge measured in coulombs, ”B” is the magnetic field strength measured in teslas, “m” refers to the mass which is measured
in kilograms or grams, “v” is the velocity of the particle measured in meters per second, and “r” represents the radius which is measured in centimeters or meters. The velocity of the charged particle depends on its kinetic energy. The kinetic energy of the charged particle and the conservation of energy can be reduced to its electric potential energy which has been expressed by this equation below: By examining the relationship between the kinematics energy and its particle, an equation can be found to calculate the charge to mass ratio of the particle. Materials Meter Stick Wooden Cover to block out light Banana Cables Set of Helmholtz Coils Low Voltage Variable Power Supply for Helmholtz Coils High Voltage Power Supply for accelerating Voltage Tube Procedure Before touching any equipment, be sure that the power supply is shut off to keep out of danger. The radius of the coils was given in the lab manual to prevent any damage to the apparatus in a potential attempt of recording this value yourself. Turn on the power supply, begin with a low current to check if the apparatus is in function. Increase the voltage until a beam is visible in the apparatus, this is the electron accelerating. Once everything is set and ready, proceed to change the current, doing this alters the radius of the electron beam. Change the current 10 times while recording the diameter of each trial.
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Once the trials are complete, lower the voltage and current, carefully shut off the power supply, and leave the apparatus as it was at the beginning of the experiment. Results and Calculations Table 1: Results from the experiment
Figure 1: Graph displaying “1/B^2 vs r^2” r 2 = 0.99 Given: u 0 = 4 π × 10 7 N = 2 × 130 = 260 turns the coil I = 1.85 A a = 0.1525 B = 8 u 0 ¿ a ¿ B = 8 ( 4 π × 10 7 )( 260 )( 1.85 ) ( 0.1525 ) ¿¿ ¿ 4.84 × 10 3 1.71 ¿ 2.84 × 10 3 T Figure 2: Sample calculation of the magnetic field from trial 1
Given: B = 2.84 × 10 3 T e = 1.60 × 10 19 C m = 9.12 × 10 31 Kg ΔV = 250 volts r 2 = 2 ( e m ) ΔV ( 1 B 2 ) r 2 = 2 ( 1.60 × 10 19 9.12 × 10 31 ) 250 ( 1 ( 2.84 × 10 3 ) 2 ) r 2 = 1.08 × 10 19 Figure 3: Sample calculation of r^2 value from trial 1 Charge to mass ratio (e/m) of an electron: The slope of the graph in “figure 1” should represent the mass to charge ratio of an electron, therefore, to get the charge to mass ratio of an electron we can simply take the reciprocal of the slope value. slope = m e = 1.18 × 10 10 e m = 1 1.18 × 10 10 = 8.47 × 10 9 C Kg Percent error: % error = | Theoreticalvalue Experimentalvalue | Theoreticalvalue × 100 % error = | 1.76 × 10 11 8.47 × 10 9 | 1.76 × 10 11 × 100 % error = ¿ 95% Therefore, this experiment was extremely inaccurate. Some errors that may have occurred during the lab could be incorrect values of diameter. Another error that could have occurred can be the equipment, there may have been potential dysfunctions in the apparatus that was used to conduct the experiment. The voltage may have been too low while doing the experiment, this could have resulted in errors as well.
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There may have been some human error considering the graph was manually made, if the graph was created via matlab, it may have come out more accurate. Discussion 1) The direction of the magnetic field in the experiment can be easily determined using the “right- hand rule”. This rule consists of using your right hand to predict the direction of a magnetic field. To successfully execute the right-hand rule, the index finger should point in the same direction as the velocity of the particle, the thumb should be 90° from the index finger, the thumb represents the direction of the current. The middle finger shall be 90° from the index finger as well, the middle finger represents the direction of the magnetic field. By pointing the index finger counter clockwise in the direction of the velocity, the middle finger points toward the screen meaning the magnetic field should be into the page. Considering pre lab question one, where the particle in motion was a proton going counterclockwise into the page, an electron should do the opposite. With this information at hand, it can be said that the direction of the magnetic field of the experiment is out of the page. 2) Given the values of a protons charge ( 1.602 × 10 19 C ), and a protons mass ( 1.67 × 10 27 Kg ), the charge to mass ratio can be determined as 9.59 × 10 47 C / Kg . If we are to analyze this value and compare it to the value found in our experiment, the charge to mass ratio of a proton is much smaller than that of an electron. The possibility of a new particle can also be considered if the charge to mass ratio is not close to that of an electron or proton. Another way we can determine what particle is present during the experiment is the direction of the velocity and magnetic field. For instance, if the particle has a similar direction of velocity and magnetic field to that of the
protons, the particle must be a proton. However there is a possibility that the directions can oppose that of the proton, in this case, a new particle may have been discovered. 3) If the voltage is kept constant, certainly the electron with the smaller radius will accelerate faster than the electron with the larger radius. We must take into account the equation for centripetal acceleration, a c = v 2 / r . As the radius becomes larger, acceleration becomes smaller, vice versa Acceleration is inversely related to the radius therefore it is known that as one value increases, the other will inevitably decrease. Another variable to consider is the force acting on the electrons. This requires Newton's second law to be looked at, F = m∙a . Both electrons have the same mass, therefore the force is dependent on the acceleration of the electrons. The electron with the smaller radius will tend to accelerate faster than the electron with the larger radius, therefore it is safe to assume that the electron with the smaller radius will have greater force acting on it. Of course if both electrons are accelerating at the same speed, the force acting on them will be the same. This is indeed accurate to the results of this experiment. As the current was increased, the radius decreased, this is because a higher current creates a faster acceleration. In trials where the current was lower, the radius of the beam was larger compared to trials where the current was higher. Conclusion Overall, The findings of our lab seem to be inaccurate despite the correct execution of the experiment. Human error and equipment error could have been factors to our inaccurate findings. Sir J.J. Thomson’s experiment certainly requires extreme precision and very accurate measurements. A lesson to be learned following this experiment is to double check each and every value recorded throughout the lab. The completion of this experiment has heightened our understanding of magnetic fields and particle acceleration, skills obtained from this lab will surely be applied throughout the remainder of the course.
References 1. Randall Dewey Knight. (2017). Physics for scientists and engineers a strategic approach 4th edition Pearson 2. Lab 1 - Charge to mass ratio of the electron
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