Relativistic Electron Mass Experiment John Klumpp.

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Relativistic Electron Mass Experiment John Klumpp

Transcript of Relativistic Electron Mass Experiment John Klumpp.

Page 1: Relativistic Electron Mass Experiment John Klumpp.

Relativistic Electron Mass Experiment

John Klumpp

Page 2: Relativistic Electron Mass Experiment John Klumpp.

Testing Velocity Dependence of the Electron Mass

• Special relativity: A body’s mass increases with velocity according to the equation:

m = m0*[1-(v/c)2]-1/2

• Test by curving electron beam with B field, straightening with E field.

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Setup

-Electron beam from 90Sr source is curved by a B field

-A series of narrow apertures only allow electrons curving with R=15cm to pass by

-Beam then travels through a capacitor. Electrons whose path is not straightened by the E field collide with capacitor plates.

-Scintillator counts electrons which make it through

-Vary E field to find out which one best balances B

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What Does This Tell Us?

• We know E, B, and R• We know the forces from the B field and E

field match• Knowing this, we find:

v = E/Bm= = eRB2/E

• By determining which E field matches a series of B fields, we can find out how mass varies with velocity

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Calibration• To prevent arcing in the capacitor, we put the

whole apparatus in a vacuum chamber• This means we can’t measure B directly while

doing the experiment• Solution: Use Hall probe to find out in advance

what currents lead to what fields:

I (Amps) Average B (Gauss) Uncertainty

0.744 80.04 0.16

0.943 99.98 0.22

1.140 120.36 0.20

1.334 139.93 0.24

1.533 159.73 1.54

1.731 180.36 0.38

1.822 189.69 0.41

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Calibration Results

Magnetic field vs current with linear polynomial overlay.

-Calibration Equation: B = 101.7A + 4.3

-χ2 is 1.79 with 5 degrees of freedom.

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The Experiment

• Remove Hall probe, insert experimental apparatus• Take measurements at 80, 100, 120, 140, 160, 180, and

190 Gauss.• For each B field, Take 13 measurements for 100

seconds each• Measurements are in 50V intervals about theoretical

value• Plot each set of measurements, fit a Gaussian to

determine peak position• This peak is the E field which should perfectly balance

the B field

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Finding the Peak

• E field vs. counts for B = 80.6T with Gaussian overlay• Peak is 2.78kVm-1, in agreement with theory

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• Using this method, we found the electric fields which corresponded to each B field.

• From there we calculated mass and velocity

I (Amps) B(Tessla) Peak (KV) m (kg) dm beta dbeta

0.75 0.0081 2.784 1.14E-30 6.531E-33 0.567 0.017

0.95 0.0101 3.99 1.24E-30 2.3E-32 0.650 0.019

1.14 0.0120 5.17 1.36E-30 8.129E-33 0.708 0.015

1.35 0.0141 6.579 1.48E-30 6.292E-33 0.765 0.013

1.53 0.0160 7.897 1.59E-30 1.105E-32 0.809 0.013

1.73 0.0180 9.117 1.73E-30 3.988E-33 0.832 0.011

1.83 0.0190 9.785 1.8E-30 5.895E-33 0.844 0.011

-Clearly mass varies with velocity, but how?

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Mass vs. Velocity• Relativity predicts mass will vary with velocity as such:

m = mo(1- β2)-1/2

• We plotted m vs β and m vs (1- β2)-1/2 to find out if our results match this shape, and to find the rest mass.

-As expected, these fit lines match the data quite well. The m vs β fit gives m0 = 9.572*10-31. The m vs (1- β2)-1/2 fit gives m0 = 9.48*10-31. The χ2 on the two graphs are 32.6 and 16.5 respectively. Each has 5 degrees of freedom.

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Charge to Mass Ratio• The charge-to-mass ratio of the electron can be

determined by the equatione/mo = e/[m(1- β2)1/2] = U/[RB(D2B2 – U2/e2)1/2]

• Results:

B(Tessla) U (kV) e/mo (C/kg) de/mo

0.00806 2784 1.71E+11 1.24E+10

0.01008 3990 1.7E+11 1.11E+10

0.01199 5170 1.67E+11 9.99E+09

0.01413 6579 1.68E+11 9.74E+09

0.01604 7897 1.71E+11 1.03E+10

0.01800 9117 1.66E+11 9.58E+09

0.01903 9785 1.66E+11 9.64E+09

-Conclusion: e/m0 = (1.68 +/- .04)*1011 C/kg

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Sources of Uncertainty• Tiny uncertainty on E, big uncertainty on B:

-σE/E ≈ .001-σB/B ≈ .025

• B varies within the magnet• Some, but not much, statistical uncertainty from calibration equation• Does the calibration remain stable throughout the experiment?• e/m0 results consistently below accepted value – suggests

systematic uncertainty• On plots to determine E, most points had uncertainty of 5% or

higher (√N statistics) -Could be reduced by taking longer measurements-Uncertainty on location of peak only 0.5%, so not worth it.

• Different results on mo for different plots. Reason?-The uncertainties on the x-values of these fits are different-MatLab does not consider uncertainty on x values when making the plot

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Conclusion

• Mass varies with velocity in accordance with special relativity

• We have two values for m0. Choose the one from the plot with the better fit: m0 = (9.48 +/- 0.506)*10-31kg

• e/m0 = (1.68 +/- .04)*1011 C/kg• Most significant source of uncertainty: B• Uncertainty can be minimized by

-Taking extreme care in calibrating the magnet-Ensuring calibration conditions hold throughout experiment