( Thompson’s Experiment )

Slides:



Advertisements
Similar presentations
Advanced Higher Physics Unit 2
Advertisements

PT UNIT 1 Subunit 3.
The Structure of the Atom. Demonstrate the Think Tube.
An atom is made of a nucleus containing protons and neutrons; electrons move around the nucleus. Section 2: Defining the Atom K What I Know W What I Want.
The specific charge of the electron
Magnetism The Magnetic Force x x x v F B q  v F B q   v F = 0 B q.
Purpose Determine the charge to mass ratio (e/m) of an electron.
2/xx/07184 Lecture 221 PHY 184 Week 6 Spring 2007 Lecture 22 Title: The Lorentz Force = q v x B.
Lecture 20 Discussion. [1] A rectangular coil of 150 loops forms a closed circuit with a resistance of 5 and measures 0.2 m wide by 0.1 m deep, as shown.
Magnetic Force. Moving Charge  A charge in an electric field is subject to a force. Charge at rest or in motion In the direction of field  A charge.
24-1 Physics I Class 24 e/m Ratio for the Electron.
Reflection & Refraction,Reflected Images Lecture 24 Monday: 12 April 2004.
Refracted Images Lecture 25 Thursday: 15 April 2004.
The History of the Atom.
Lecture 49/7/05 Homework concerns Atomic Structure.
More than One Way to Skin a Cat? The Charge-to-Mass Ratio of the Electron.
Magnetic Fields Magnetic fields emerge from the North pole of a magnet and go into the South pole. The direction of the field lines show the direction.
Experimental Measurement of the Charge to Mass Ratio of the Electron Stephen Luzader Physics Department Frostburg State University Frostburg, MD.
Electrons Thermionic Emission
Comprehension Check 1. An electron is moving at right angles to uniform magnetic field; if the electron is moving at.010c, determine the magnitude of the.
Centripetal force on charges in magnetic fields
to Atomic and Nuclear Physics
Chapter 19 Magnetism 1. Magnets 2. Earth’s Magnetic Field 3. Magnetic Force 4. Magnetic Torque 5. Motion of Charged Particles 6. Amperes Law 7. Parallel.
standards: 1e, 1h terms: 92 mastering concept: 112 (34-46) Homework Cornell notes: 4.2 sec. assessment: 97(6-8) 1.
The History of the Atom…. went against, Aristotle, who believed that matter was composed of four qualities: earth, fire, air and water all matter is composed.
Topic 25: Charged Particles 25.1 Electrons 25.2 Beams of charged particles.
Physics 2170 – Spring OUR FRIEND THE ATOM First midterm is 7:30pm on 2/17/09 Problem solving sessions M3-5.
Magnetic Forces. * Current-carrying wires have magnetic fields and… * Magnets exert forces on other magnets. Therefore… Magnets exert forces on current-carrying.
Lecture 5 R 2R2R Yesterday we introduced electric field lines Today we will cover some extra topics on Electric Fields before going on to Electric Flux.
The Structure of the Atom 3.2. Experiments  Atom – the smallest part of an element that retains the chemical properties of that element.  Subatomic.
Properties of cathode rays
Deflections We have already done programs on Gravitational Deflection (trajectories - PHYS 201, Vol. 1, #6) and Electric Deflection (cathode ray tube,
The History of the Atom Part 2 – The discovery of subatomic particles When we last left the atom, it looked like this:
When charged particles move through magnetic fields, they experience a force, which deflects them Examples of such particles are electrons, protons, and.
Late 1800s/ Early 1900s Experiments were conducted using electricity and matter Use a cathode-ray Tube At each end of the cathode -ray tube electrodes.
Chapter 25 Electromagnetic Induction. Do Now (2/8/12): True or False 1.Magnetic force is maximum when v and B are perpendicular to each other. 2.A charge.
26.1 Action of Electric and Magnetic Fields on Matter Chapter 26.
How Are Electric And Magnetic Fields Used To Steer Particles In The Large Hadron Collider?
Book Reference : Pages To understand that the path of a charged particle in a magnetic field is circular 2.To equate the force due to the magnetic.
Chapter 21 Magnetic Force.
7.3 Magnetic Fields and the Electron p. 284 Electron Behaviour (part 1) J.J. Thomson (1856 – 1940) made meticulous measurements of cathode rays and measured.
Models of the Atom Day 1. What is an atom? Why do we care about older models?
Mass Spectrograph Physics Chapter 27 B. Mass spectrograph Adapted CRT/Thomson tube used to form and accelerate charged particles and measure their deflection.
Magnetic Forces. The Force on a Moving Charge in a Magnetic Field Just as current-carrying wires (a stream of moving charges) experience a force in a.
Chapter 26 Electromagnetism. Mass of Electron Determined by J.J. Thomson Determined by the deflection of the electron in a cathode ray tube.
1 Motion in Electric Fields SACE Stage 2 Physics.
Chapter 21 Magnetic Force. Clicker A)1.7 V B)3.4 V C)5.1 V D)6.8 V E)12 V What is the potential difference across the clams when I take bulb out of circuit?
Think Harder…you can do it! Do the units of N/C equal V/m ? Prove this to be true or false !
ELECTRIC FIELDS. CREATING AND MEASURING ELECTRIC FIELDS Michael Faraday developed the concept of an electrical field where electrical charges exert forces.
Atomic Structure.
We know spinning electrons make a magnetic field…
ELECTRONIC DEVICES AND CIRCUITS
Section 2: Defining the Atom
Discovery of the Electron
3.1: Discovery of the X Ray and the Electron
Measurement of electron’s E/M
Section 2: Defining the Atom
The Millikan Oil Drop Experiment
A proton is accelerated from rest through a potential difference of V
PARTS OF THE ATOM electrons protons neutrons.
Charged Particles Moving in Simultaneous Electric and Magnetic Fields
Electrons Thermionic Emission
Textbook: 8.2 Homework: pg. 396 # 3 – 5 pg. 402 # 1 – 3 , 10
Discovery of the Electron
e/m Ratio for the Electron
An atom is made of a nucleus containing protons and neutrons; electrons move around the nucleus. Section 2: Defining the Atom K What I Know W What I Want.
Today 5-6 pm is a LAST chance
The Electron – Learning Outcomes
Fundamental Particles of Matter
Presentation transcript:

( Thompson’s Experiment ) Measurement of Charge to Mass Ratio For an Electron ( Thompson’s Experiment ) Carleton University

The scale of the subatomic world You and me Insect 1 m Virus on an insect 10-3 m Atom of a virus 10-6 m Proton 10-9 m + electron 10-12 m Quark Carleton University 10-15 m

The Electron: is an elementary particle: smallest speck of matter is normally found in the immediate vicinity of a nucleus, forming an atom Mass (me): 9.11 x 10-31 kg Charge (e): 1.6 x 10-19 C (C = Coulombs) Charge is found by Millikan’s Oil Drop experiment So, if we can find e/me, we can determine me In 1897, J.J. Thompson found this value Ratio (e/me): -1.76 x 1011 C/kg Your Job: try to repeat that measurement today Carleton University

Forces affecting the electron: 1. The electric field: e- E the electric field, E, produces a force FE = q·E (q = e, the charge of the electron) The electric field, E, always points in the direction that a +ve charge would move if it were within the field. Carleton University

Forces affecting the electron: 2. The magnetic field: e- Bout The magnetic field (Bout) produces a force: FB = Bout·e·v (v is the velocity of the electron) This force is perpendicular to both Bout and v. Into the page Out of Carleton University

Finding e/m: Electrons move in circles in magnetic fields This motion produces a centripetal force We can equate this to FB: Re-arranging: Thus, to find e/m we need to know 3 things: the magnetic field, B, the radius of curvature, R, and the velocity of the electrons, v. v e- Bout R Carleton University

Finding the magnetic field, B: “Helmholtz” coil arrangement delivers uniform magnetic field B depends on current, and is calibrated to be: B = I x 4.23 x 10-3 Wb m-2 (I measured in Amps) D.C. “Lambda” Power Supply Beckman I B Carleton University

Determine the radius, R: 4 3 2 1 R x y Measure y - deflection at a distance, x, from the exit of the electron Given (x,y) - find R To prove this, try Pythagoras: (x,y) = (4,-2) y R b = R - y x Carleton University

Determine the velocity, v: Now switch on the Electric Field Use it to cancel the effects of the B field +ve 2 1 -1 -2 8 7 6 5 4 3 2 1 d E Use the Electric field to cancel the deflection at the x value where the magnetic deflection was measured -ve CENCO Power Supply D.C. Voltage (5kV) Carleton University

Procedure: Plug in transformer for cathode heater supply Switch on CENCO D.C. supply to accelerate electrons down the tube and onto the screen set to ~ 2400 V There should now be a blue trace on the screen Switch on Beckman meter and Lambda power supply unit connected to coils set to ~ 0.2 A Determine B Carleton University

Procedure: Measure (x,y): determine R Switch on second CENCO DC supply connected to electrodes on top of mica screen set to ~ 1.5 kV Adjust to cancel deflection: determine v Fill in worksheet and calculate e/m Switch off all power supplies Carleton University

Carleton University