 Please note that this lab notebook page is the combined efforts of Alex Andrego and Anastasia A. Ierides
Purpose
^{SJK 15:41, 14 November 2009 (EST)} 15:41, 14 November 2009 (EST) As usual, excellent primary lab notebook! Really great notes, very easy to follow. My main criticism in this lab would be that you jumped to conclusions on explanation of systematic error, and didn't explore other possibilities at all.
 The purpose of this lab is to measure the charge to mass ratio (e/m) for electrons whilst studying the effects that electric and magnetic fields have on a charged particle. For N coils carrying current I with radius R, the magnetic field along the symmetry axis x is given by:

 You can see a more detailed purpose in Professor Gold's e/m Ratio for Electrons.
Brief Description of e/m
 According to J.J. Thompson if the electron has finite charge e and has mass m it will obey the laws of motion for a charged particle moving through a magnetic/electric field. The e/m ratio is the charge to mass ratio of an electron which can be determined if the energy of the electrons and the magnetic field strength are known. "In this experiment [we will be] observing the behavior of electrons in a magnetic field and determine a value for the electron chargetomass ratio e/m. The apparatus consists of a large vacuum tube supported at the center of a pair of Helmholtz coils,... The vacuum tube contains an electron gun which produces a collimated beam of electrons that is deflected by a magnetic field. An electron gun has two main parts: a filament that produces electrons through thermionic emission, and an anode that is placed at high positive potential so as to accelerate thermal electrons from the filament to the main region of the vacuum tube,... The magnetic field produced by the Helmholtz coils deflects the electrons into circular trajectories and these paths are made visible through collisions by the electrons with a trace amount of mercury vapor present in the vacuum tube." The Electron ChargetoMass Ratio e/m
Equipment
 HewlettPackard DC Power Supply (Model 6384A, 45.5V, 08A)
 SOAR corporation DC Power Supply (Model 7403, 036V, 3A)
 Gelman Instrument Company Deluxe Regulated Power Supply (500 V, 100 mA)
 2 BK PRECISION Digital Multimeter (Model 2831B, (1)SER. NO. 000030618 & (2)SER. NO. 099100357 , 5 WATTS, 8 VA,50~60 Hz)
 e/m Experimental Apparatus (Model TG13)
Safety
 Before we begin, some points of safety must be noted:
 First and foremost your safety comes first and then the equipments'
 Check the cords, cables, and machinery in use for any damage or possible electrocution points on fuses of machinery by making sure the power cords' protective grounding conductor must be connected to ground
 Be careful to ground all power supplies properly before use
 Be careful while handling and working with the mercury tube
 Make sure the areas containing and around the experiment are clear of obstacles
Set Up
(bottom) HewlettPackard DC Power Supply (Model 6384A, 45.5V, 08A) and (top) BK PRECISION Digital Multimeter (Model 2831B, SER. NO. 000030618 , 5 WATTS, 8 VA,50~60 Hz)
e/m Experimental Apparatus (Model TG13)
(left of e/m E. A.) SOAR corporation DC Power Supply (Model 7403, 036V, 3A), (top right) BK PRECISION Digital Multimeter (Model 2831B, SER. NO. 099100357 , 5 WATTS, 8 VA,50~60 Hz), (bottom right) Gelman Instrument Company Deluxe Regulated Power Supply (500 V, 100 mA)
 The procedure we followed was based on the descriptions given in Professor Gold's manual
 Connect a regulated 69 Vdc supply rated at 2 A to the Helmholtz coil jacks using BCN cables
 Connect the ammeter in series between the supply and the coil jacks
 Connect the 6.3 V power supply (rated at 1.5 A0 to the heater jacks of the electron gun
 Connect a high voltage source of 150300 V dc rated at 40 mA to the Electrode jacks of the electron gun
 The value of this voltage determines the average velocity of the electrons in the beam
 Connect the dc voltmeter at the jacks labeled Voltmeter on the base panel
 Turn the Current Adjust control to zero and set the switch on the panel to the e/m position
 Nothing should be connected to the jacks labeled Deflection Plates at this time
 Turn on the Heater supply and allow the electron gun filament to heat up for two minutes
 Apply a 200 Vdc potential from the high voltage supply to the Electrodes
 Turn off the light when ready to begin experimentation
 Use a black cloth hood to mask the tube and to backdrop the beam while witnessing the beam of electrons
 Turn on the coil current and increase the Current Adjust control until the beam forms a complete circle
 Rotate the tube socket until the end of the curving beam strikes between the two wire leads
 Use the scale located behind the bulb to measure the radius of the loop of the beam
Measurements and Data
Calculations and Analysis
^{SJK 15:37, 14 November 2009 (EST)} 15:37, 14 November 2009 (EST) Excellent raw data notebook & nice graphs. Was easy for me to follow your data and check things out. Also, looks like you took nice data, based on looking at your best fit lines.
 In the Helmholtz configuration, from Professor Gold's Manual we are given:
 , , and
 The permeability of free space is given as

 From these values we can calculate:




 We know that:


 So,

 In order to find we need to plot
 vs. , where is constant
 vs. , where is constant
 The current accepted value of is:

 We can plot vs. with this equation:

 treating as a constant which gives us a linear relationship with this as our slope.
 In order to determine the slope we need to plot our data:
 From this graph we have that:

 We also have that the equation of slope is:

 Therefore we can calculate the ratio of by:


 Where,

 So we have:


 Taking into account our slope uncertainty value of the range of our measured ratio is...

^{SJK 12:37, 14 November 2009 (EST)} 12:37, 14 November 2009 (EST) As opposed to below, here I get the same numbers as you do. So, I guess you just made a mistake below? In any case, even here it's important to provide some more information as to how you're calculating the error propagation. You can explicitly say that you're treating any other uncertainties (besides slope) as insignificant, and thus you can use this exact method
 2. We can plot vs. with this equation:

 treating as a constant which gives us a linear relationship with this as our slope.
 In order to determine the slope we need to plot our data:
 Note: Due to the fact that all values of current are negative, we took the absolute value of the current for graphing purposes because the negative sign was purely directional.
 From the above graph we have that:

 We also have that the equation of slope is:

 Therefore we can calculate the ratio of by:


 Where,

 So we have:


 Taking into account our slope uncertainty value of the range of our measured ratio is...

^{SJK 12:29, 14 November 2009 (EST)} 12:29, 14 November 2009 (EST) I get the same mean value you do (3.3E11), but cannot figure out how you get that range. More explanation is needed, especially since many people may think you're using error propagation, whereas you may also be plugging in (slopeuncertainty) and calculating low e/m etc.
Notes about Our Uncertainty
Systematic Error:
 The only way to achieve measurements for the radius of our electron beam was to measure by eye using a fixed ruler in the back of our apparatus. This could cause a huge source of error because we were basically estimating for each measurement. This also caused a lot of rounding error because we were estimating we were not able to give very specific measurements.
 Steve Koch 15:39, 14 November 2009 (EST): As I mentioned on your summary pages, I don't think this is the source of your systematic error. Unfortunately we didn't get to talk about this at all during the lab class, but the experiment is basically forced to have a lot of systematic error, and you can hypothesize on the reasons if you do this lab for your formal report.
Summary
 If you wish to see Alex Andrego's informal summary of this lab follow this link
 If you wish to see Anastasia Ierides's informal summary of this lab follow this link
Acknowledgments
 Prof. Gold's Lab Manual served as a loose guideline for our lab procedure
 The following link was used in our "Brief Description of the e/m ratio" above The Electron ChargetoMass Ratio e/m
 Professor Koch and Pranav for always being of great help to us!
