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Transcript of Tutorial: Tutorial examples will be posted at least a day before the tutorial so you can think about...
Tutorial:
Tutorial examples will be posted at least a day before the tutorial so you can think about them to benefit most from the tutorial
Regular Quizzes (every 2-3 weeks, 15-20 min each) during tutorial
Relativity and QuantaPHYS 242Fall 2013
Lecture:
Lecture notes available ahead of time - READ and answer Pre-Lecture Quiz (Moodle)Tell me your questions via Moodle (or in class) – that’s what we’ll discuss
Assignments:
Will be posted Fridays, are due Monday, 10 days later, during the tutorial.
Exam:
Final exam in December (3 h)
Marking scheme:
Lecture Quizzes: 10 %Tutorial Quizzes: 15 %Assignments: 25 %Exam (final): 50 %
concepts, ideas, some derivations of fundamental formulae
application of the concepts, examples (help for assignments)
examples: experience in applying concepts to actual problems, feedback on learning success, practice for exam (assessment)
Motivator for learning, assessment
W. Rau
Books
Relativity and QuantaCustom version of: Serway, Moses, Moyer: Modern Physics ; Brooks/Cole -- Thomson Learning (available at Campus Book Store)
A.P. French: Special Relativity W.W.Norton & Company Inc. New York
R. Eisberg, R. Resnick: QUANTUM PHYSICS of Atoms, Molecules, Solids, Nuclei and Particles John Wiley & Sons, New York, London, Sydney, Toronto
Course Web page:
http://www.physics.queensu.ca/~phys242/ :Lecture Notes, Assignments, Tutorial Questions, Solutions
Moodle: Pre-Lecture Quizzes, YOUR Questions, Grades
Relativity and QuantaPHYS 242Fall 2013
W. Rau
Newton’s laws:1. Inertia: Any object moves with constant velocity as long as no net force acts upon it2. Action: Any object experiences acceleration in presence of a net force: F = ma3. Reaction: If force F acts upon an object, –F acts upon the object where the force originates.
Classical mechanics
Inertial system: Reference frame where Newton’s 1. law applies.
any reference frame that moves with a constant velocity relative to a given inertial system, is also an inertial system and vice versa (any inertial system moves with constant velocity relative to any other inertial system)
Relativity Principle: The evaluation of an observation leads to the same conclusions about the laws of physics in any inertial system
W. Rau
S S '
V
Coordinate transformation:x = x' + Vt' y = y' z = z ' t = t'
Velocity transformation:vx = vx' + V vy = vy' vz = vz'
x = x ' + R
x ' = ( ) x ''
x = ( ) x '' + R
t = t' + Dt
→ → →
cos a sin a-sin a cos a
→ →
cos a sin a-sin a cos a
→ → →
Coordinate Transformation
v = –– = ––––––– = –– + ––– = v ' + V dx d(x '+ R ) dx ' dRdt d(t' + Dt) dt' dt
→→ →
→→→→ →
Choose: x = x‘ = 0 for t = t‘ = 0, V ║ x
Galilean law for the addition of velocities:
v = v ' + V
(V: velocity of S ' w.r.t. S )
→ → →
→
St1
x1
y1
x1''
y1''
S'' t1''
αx1'
y1'
S'
t1'
R = (∆x,∆y)⃑x⃑
x'⃑
W. Rau
Boat
Fog
Fog Reference frame of the boat
W. Rau
Fog
Fog
Wood
Reference frame of the wood
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Wood
Fog
Boat
Fog
Reference frame of the wood(but observer on the boat)
W. Rau
vx = 0vy = 0
v0
vx,ball = 0vy,ball = v0 - gt
S
S'
Reference frame of the boat
W. Rau
S''v0
vx,bqll = vvy,ball = v0 - gt
vvx = vvy = 0
S
S'
Reference frame of the wood
W. Rau
vx,ball = vvy,ball = - gt
v
v0
v
S''
vx = vvy = – v0
S
S'
Reference frame of the elevator
W. Rau
How to Produce Spacetime diagrams
W. Rau
How to produce spacetime diagrams (II)
W. Rau
Spacetime diagram Boat(at rest)
Wood(moving)
Space
Tim
e
W. Rau
Boat
W. Rau
W. Rau
Spacetime diagrams
Boat (center)
Passenger (front)
Passenger (back)
Ball 1
Wood
Ball 2
Boat(center)
Passenger (front)
Passenger (back)
Ball 2
Wood
Ball 1
vB1 = v ; vB2 = – v
vB1 = vB1' + V vB1' = vB1 – V = v – V
vB2 = vB2' + V vB2' = vB2 – V = – v – V
W. Rau
Boat
Reference frame of boat and water
W. Rau
Source at rest with respect to medium
W. Rau
Source moving with respect to medium, frame of medium
W. Rau
Source moving with respect to medium, frame of source
W. Rau
Boat
Reference frame of the boat; water moving
W. Rau
Wood
Reference frame of the wood; boat moving with water
W. Rau
Source at rest with respect to medium;both are moving relative to reference frame
W. Rau
vc
Xs
v
X
Case A:Source and Receiver
at rest
Case B:Source moving with
velocity v
Case C:Receiver moving with velocity – v
W. Rau
SourceReceiver SourceReceiver
Case B
Rest frame of source(and water)
Rest frame of receiver(and water)
Case A Case C
DtR,C
x = v Dt x = 0
t = Dt
t = 0
t1
W. Rau
SourceReceiver
Case B
Rest frame of receiver(and water)
SourceReceiver
Case B
Rest frame of source
Case C
DtR,B
Rest frame of source(and water)
W. Rau
Summary
Newton’s Laws1. Inertia: v constant for F = 02. Action: F = ma3. Reaction: each force is balanced
by counter force
Reference Frames, Coordinate SystemsReference frame: “point of view”Coordinate system / transformation: Specify position / time in different frames
S S '
V
x = x' = 0 for t = t' = 0, V = Vx = const.:x = x' + Vt ; vx = vx' + V ; a = a‘
Inertial frame Reference frame where N.’s 1. law applies
Spacetime DiagramsA way to keep track of the position of objects in time
Propagation of Waves, Doppler Effect- Waves propagate with constant vc relative to medium- Observed frequency n depends on velocity of source
vs and receiver vr relative to medium:Moving source: nr = ns / (1 – v/vc)Moving receiver: nr = ns (1 + v/vc)
- Wavelength depends only on vs
Boat (center)
Passenger (front)
Passenger (back)
Ball 1
Wood
Ball 2
t
x
Galilean velocity transformationv= v'+V
W. Rau