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-Magnetic Force on a Charged Particle -Magnetic Force on a Current-Carrying Wire -Torque on a Current-Carrying Loop Fermi Lab, Chicago Illinois Circumference.

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Presentation on theme: "-Magnetic Force on a Charged Particle -Magnetic Force on a Current-Carrying Wire -Torque on a Current-Carrying Loop Fermi Lab, Chicago Illinois Circumference."— Presentation transcript:

1 -Magnetic Force on a Charged Particle -Magnetic Force on a Current-Carrying Wire -Torque on a Current-Carrying Loop Fermi Lab, Chicago Illinois Circumference 6.3km Mass Spectrometer DC Motor AP Physics C Mrs. Coyle

2 A magnetic field can exert a force on a charged particle that moves in it.

3 Three ways we talk about “magnetic field”.
Magnetic Field: Regions surrounding a magnet where another magnet or a moving electric charge will feel a force of attraction or repulsion. Magnetic Field Lines: exit the north pole and enter the south. Magnetic Field Strength, B Vector, Unit: Tesla, T Named after Nikola Tesla

4 Poles Law of Poles: Like poles repel, unlike poles attract.
The force between two poles varies as the inverse square of the distance between them. A single pole (monopole) has not been isolated.

5 Force on a Charged Particle Moving in a Magnetic Field
-Magnetic fields only exert forces on moving charged particles or other magnets.  F = |q|(v x B) = |q|vB sin q vector cross-product q is the angle between v and B F=0 for q =0 or 1800

6 Remember: Cross Product Using Determinants
or

7 Remember: Properties of Cross Products of Unit Vectors
ixi=0 jxj=0 kxk=0 ixj=k jxk=i kxi=j

8 To find the direction of the force use the Right Hand Rule
For a positive test charge: Thumb v Fingers B Out of palm F The force is always perpendicular to the vB plane

9 For a negative particle the F is opposite to what it would be for a positive particle (use left hand)

10 Alternate Rule: Right Hand Curl Rule
Curl fingers from v to B F = q(v x B) F is in the direction of the thumb Similarly used for the direction of torque (t=r x F)

11 Graphical Representation of the Magnetic Field Vector (Strength), B
x field lines pointing into the page ● field lines pointing out of the page

12 Question Find the direction of the magnetic force acting on the +charged particle entering the magnetic field with a velocity v perpendicular to B. x x x x x V x x x x x Answer: Upwards

13 What motion will the particle in the previous example undergo (particle entered the B-field in a direction perpendicular to B? Circular Motion Magnetic force will represent the centripetal force

14 Examples:

15 Does the magnetic force do work?
F is always perpendicular to the displacement F can change the direction of v not the magnitude F cannot do work, cannot change KE

16 Mass Spectrometer U.S. Department of Energy

17 Motion of Alpha- Beta-Gamma Particles in a Magnetic Field
1) Alpha particles, positive helium nuclei, charge +2e 2) Gamma rays, (no charge) electromagnetic radiation 3) Beta particles, electrons charge -1e

18 Problem 1 A proton is accelerated through a constant electric field
(parallel plates) and acquires kinetic energy of 4eV. It enters perpendicularly to the 2T field of a detector as shown. Charge of a proton=1.6x10-19 C, mass of proton=1.67x10-27 kg, ignore gravity. a) Draw the path of the positive charge as it enters the magnetic field.

19 Problem 1 cont’d b) Calculate the force acting on the charge due to the magnetic field. Charge of a proton=1.6x10-19 C , mass of proton=1.67x10-27 kg KE= 4eV B= 2T Ans: v= 2.77x104 m/s, F= 8.86x10-15 N

20 Problem 1 cont’d c) Calculate the distance on the detector where the particle will land (radius of the circular path). Ignore gravity. Charge of a proton=1.6x10-19 C, mass of proton=1.67x10-27 kg KE= 4eV B= 2T Ans: 1.45x10-4 m

21 Large Hadron Collider CERN (Conseil Européen pour la Recherche Nucléaire) Switzerland- France 2008 Circumference: 27km

22 Particle Accelerators use electric and magnetic fields to accelerate charged particles.
Cyclotron Applet

23 Magnetic Force on a Current Carrying Wire
F = I (L x B) = I L B sinq I is the current L is a vector of magnitude of the length of the wire and direction that of the current q is the angle formed between I and B What is the direction of the magnetic force acting on this wire? F

24 The force acting on a wire of arbitrary shape is the same as if it were a straight wire with the same ends The total force is:

25 What is the net force acting on this current-carrying loop?

26 Which way will a loop turn?

27 Forces on a Current-Carrying Loop
For B as shown: F 1 = F3 = 0 F 2 = F4 = IaB Electric DC Motor (Fendt Applet)

28 F 2 = F4 = IaB Top View Torque Acting on the Current-Carrying Loop
Torque acting on the loop:

29 Torque Acting on the Current-Carrying Loop

30 Magnetic Force on a Current Carrying Wire
Lorentz Force- Magnetic Force on a Current Carrying Wire (Fendt Applet)

31 DC Motor

32 DC Motor

33 Problem #9 A proton moves with a velocity of v=(2i-4j+k)m/s in a region in which the magnetic field is B=(i+2j-3k)T. What is the magnitude of the magnetic force this charge experiences? Ans: 2.34x10-18 N

34 Problem #13 A wire 2.80 m in length carries a current of 5.00 A in a region where a uniform magnetic field has a magnitude of T. Calculate the magnitude of the magnetic force on the wire assuming the angle between the magnetic field and the current is (a) 60.0°, (b) 90.0°, (c) 120°. Ans: a)4.73N, b)5.46N, c)4.73N

35 Problem # 21 A small bar magnet is suspended in a uniform T magnetic field. The maximum torque experienced by the bar magnet is 4.60 × 10–3 N · m. Calculate the magnetic moment of the bar magnet. Ans: 18.4mA m2

36 Problem #54 A kg metal rod carrying a current of 10.0 A glides on two horizontal rails m apart. What vertical magnetic field is required to keep the rod moving at a constant speed if the coefficient of kinetic friction between the rod and rails is 0.100? Ans: F=0.196N, B=0.039T


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