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Chapter 21 Magnetic Force.

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Presentation on theme: "Chapter 21 Magnetic Force."— Presentation transcript:

1 Chapter 21 Magnetic Force

2 Magnetic Field of a Moving Charge
The Biot-Savart law for a moving charge The Biot-Savart law for a short piece of wire: How magnetic field affects other charges?

3 Magnetic Force on a Moving Charge
TV and CRT monitors: Direction of the magnetic force depends on: the direction of B the direction of v of the moving charge the sign of the moving charge Electrons are accelerated and deflected vertically by a magnetic field q – charge of the particle v – speed of the particle B – magnetic field

4 Right Hand Rule for Magnetic Force
Electron charge = -e: The magnetic force on a moving electron is in opposite direction to the direction of the cross product

5 Effect of B on the Speed of the Charge
What is the effect on the magnitude of speed? Kinetic energy does not change Magnetic field cannot change a particle’s energy! Magnetic field cannot change a particle’s speed! Magnetic force can only change the direction of velocity but not its magnitude

6 Magnitude of the Magnetic Force
Move charged tape close to a magnet: can you detect the magnetic force? Single electron in television tube: (v<<c) e/me = C/kg Magnetic forces on rubbed objects – always tiny! q/m for charged tape: (10-8 C)/(10-4 kg)  10-4 C/kg

7 Exercise Net charge on invisible tape is ~ 10-8 C
Magnetic field near your bar magnet is ~0.1 T What is the force on tape if the tape is moved in the direction perpendicular to the field with a speed of 10 m/s ? Electric force between two charged tapes 10 cm apart:

8 Motion in a Magnetic Field
Confined area: deflection What if we have large (infinite) area with constant Bv No work is done on the charged particle

9 Circular Motion at any Speed
Any rotating vector: …angular speed Cyclotron Frequency

10 Circular Motion at Low Speed
if v<<c: independent of v! Alternative derivation: Circular motion: Period T: Non-Relativistic

11 Determining the Momentum of a Particle
Position vector r: Circular motion Position r is a rotating vector! valid even for relativistic speeds Used to measure momentum in high-energy particle experiments

12 1st Event at STAR Experiment
Looking along collision direction Looking at right Angle to collision direction Au

13 Determining e/m of an Electron

14 Joseph John Thomson (1856-1940)
1897: m/e >1000 times smaller than H atom

15 Clicker Question

16 Clicker Question

17 Exercise What if v is not perpendicular to B? Direction? Magnitude?
𝐹 𝑚𝑎𝑔𝑛𝑒𝑡𝑖𝑐 =𝑞 𝑣 ⊥ + 𝑣 ∥ × 𝐵 𝑣 ∥ 𝑢𝑛𝑐ℎ𝑎𝑛𝑔𝑒𝑑; Trajectory: helix

18 Exercise: Circular Motion
Which direction an electron would go? Clockwise or anti-clockwise? Clockwise: -ev x B points inward

19 Exercise: B in TV set How big is the magnetic field in a TV created by the electron beam deflection coil? B Acceleration voltage: 15000V Solution: 1. Electron speed: v= m/s Gamma = 1.03. 2. Are we justified in using the nonrelativistic KE?

20 The Lorentz Force Can combine electric and magnetic forces:
Coulomb law and Biot-Savart law have coefficients 1/(40) and 0/(4) to make the field and force equations consistent with each other

21 A Velocity Selector Is it possible to arrange E and B fields so that the total force on a moving charge is zero? E FE What if v changes? If velocity is less than E/B, magnetic force is less than electric force, leading (for a positive charge) to a greater deflection in +y direction. If velocity is greater than E/B, greater magnetic force (-y deflection). B FB

22 A negative charge is placed at rest in a magnetic field as shown below
A negative charge is placed at rest in a magnetic field as shown below. What is the direction of the magnetic force on the charge? B Up Down Into the page Out of the page No force at all. 73 of 140

23 A negatively charged particle is moving horizontally to the right in a uniform magnetic field that is pointing in the same direction as the velocity. What is the direction of the magnetic force on the charge? 𝒗 B Up Down Into the page Out of the page No force at all. 72 of 140

24 Now, another negatively charged particle is moving upward and to the right in a uniform magnetic field that points in the horizontal direction. What is the direction of the magnetic force on the charge? 𝒗 B Left Up Down Into the page Out of the page Up out of page. v X B is into page but negative particle. 70 of 140

25 A Cyclotron Vequivalent ~ 108 V  v~c : need to adjust B or 
Used to study nucleus – accelerate particles (protons) and shoot at nucleus to observe nuclear reactions Also create new particles – collide particles Synchrotron – source of synchrotron radiation D-shaped boxes (Dees)

26 Particle Accelerator Fermilab: Tevatron CERN: Large Hadron Collider
Final stage: circle radius ~ km Proton speed up to c To keep R constant B is increased up to 3 T (superconducting coils)

27 Magnetic Force on a Current-carrying Wire
Current: many charges are moving Superposition: add up forces on individual charges Number of moving charges in short wire: I Total force: 𝐹 𝑚 = 𝑛𝐴∆𝑙 𝑞 𝑣 × 𝐵 = 𝑛𝑞𝐴 𝑣 ∆𝑙 × 𝐵 Electrons drift in a direction OPPOSITE to the conventional current. The term qv has 2 minus which cancel Force of a short wire: In metals: charges q are negative. Will this equation still work?

28 Hall Effect When does it reach equilibrium? E h v 𝐸 𝑒⊥ = 𝑣 𝐵 B
𝐸 𝑒⊥ = 𝑣 𝐵 B Electrons will be deflected toward the bottom surface ???? + - V>0 ∆𝑉= 𝐸 𝑒⊥ ℎ= 𝑣 𝐵 ℎ

29 Hall Effect for Opposite Charges
v B E >0 + - V>0 ???? + - E v B V<0

30 Hall Effect By measuring the Hall effect for a particular material,
we can determine the sign of the moving particles that make up the current Edwin Herbert Hall ( )

31 Hall Effect in a Metal What is the magnitude of the Hall effect in a metal? 𝑣 = 𝐼 𝑞 𝑛𝐴 𝐼= 𝑞 𝑛𝐴 𝑣 ∆𝑉= 𝐼𝐵ℎ 𝑞 𝑛𝐴 ~5×1 0 −6 V Measure ∆𝑉, know the charge (e) Then we can find n Sodium, copper Last shown Monovalent metals: n is the same as # of atoms per m3 Some metals: n is larger than # of atoms per m3

32 Exercise What is VHall for the shown copper ribbon? 0.1mm
B=1T 5mm 0.1mm I=20A What is VHall for the shown copper ribbon? nCu= m3 What is potential difference along 5 mm of copper ribbon to sustain current 20 A? Cu = (A/m2)/(V/m2) Must be carefull connecting voltmeter exactly across the strip! The potential difference along the I direction is much greater than that resulting from the Hall effect in the transverse direction.

33 Clicker Question Voltmeter 1 reading is POSITIVE
Mobile charges are: A) Positive (holes) B) Negative (electrons) C) Not enough information Must be electrons traveling to right. E points from right to left <---, making right end of bar higher potential than left. Electrons will be forced to top surface by B field, making top surface lower potential than bottom surface.


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