# CW1-RELATIVITY ```RELATIVITY – MTH6132
PROBLEM SET 1
1. Suppose a river flows at a constant rate v and consider the motion of a boat
crossing this river with velocity u0 . Suppose two observers are monitoring the boat:
the first observer is on a raft floating down the river (reference frame F 0 ) and the
second observer is standing on the river bank (reference frame F ). To the observer
in the raft, the boat appears to to travel at right angles to the river bank when
crossing. On the other hand, to the observe on the bank the boat moves at an angle
θ with respect to the bank. Draw a diagram of this scenario and identify any relevant
quantities such as angles and velocities. How are the coordinates in the two reference
frames related?
2. In this problem, you may assume the speed of light c = 1. Is length ∆x = x2 − x1
an invariant under either the Galilean or Lorentz Transformations (or both)? Is the
interval −c2 t2 + x2 invariant under the Galilean or Lorentz Transformations? Recall
that for two frames in standard configuration, the Galilean Transformations (GT) are
given by t0 = t,
x0 = x − vt and the Lorentz Transformations (LT) are given by
1
.
t0 = γ(t − vx/c2 ),
x0 = γ(x − vt), where γ = q
1 − v 2 /c2
∂ 2φ
1 ∂ 2φ
3. Show that the wave equation
=
does not remain invariant under the
∂x2
c2 ∂t2
1–dimensional Galilean transformations. but that it does remain invariant under the
Lorentz transformations
Hint: Recall that the chain rule for partial derivatives gives
∂t0 ∂
∂x0 ∂
∂
=
+
,
∂t
∂t ∂t0
∂t ∂x0
Use these expressions twice to compute
∂
∂t0 ∂
∂x0 ∂
=
+
.
∂x
∂x ∂t0
∂x ∂x0
∂ 2φ ∂ 2φ
,
.
∂x2 ∂t2
4. (Extension of Problem 1) Starting from the Galilean transformation in the form
r0 = r − vt, v = (vx , vy , vz ), show that the scalar wave equation
∇2 φ =
∂ 2φ ∂ 2φ ∂ 2φ
1 ∂ 2φ
+
+
=
∂x2 ∂y 2
∂z 2
c2 ∂t2
does not remain invariant under these transformations.
Hint: recall that t = t(t0 , x0 , y 0 , z 0 ) and x = x(t0 , x0 , y 0 , z 0 ). Use the chain rule of
partial differentiation to show that
∂
∂
∂
∂
∂
∂
= 0 − vx 0 − vy 0 − vz 0 = 0 − v &middot; ∇0
∂t
∂t
∂x
∂y
∂z
∂t
and similar formulae for
∂
∂x
etc.
5. Starting from the Lorentz transformations between two frames F and F 0 in standard configuration (with F 0 moving with velocity of magnitude v relative to F ) show
ct0 − x0 = (ct − x),
r
where =
1+v/c
.
1−v/c
ct0 + x0 =
1
(ct + x)
Hence show that the combination of two LTs is a LT.
6. Consider F and F 0 in standard configuration. Let a standard clock be at rest in
F 0 and consider two events in this clock at times t01 and t02 so that ∆t0 = t02 − t01 . What
is the time interval as measured by F ? Draw and explain a spacetime diagram to
7. Consider F and F 0 in standard configuration. Let a rod of length ∆x0 be at rest
along the x0 axis in F 0 . What is the length of this rod as measured by F ? Draw and
explain a spacetime diagram to accompany your calculations.
8. Charged pions are produced in an accelerator and emerge from the machine at a
speed of .996c. Such unstable particles decay with a half-life of 1.8 &times; 10−8 seconds.
According to an observer in the laboratory, how far can such particles travel before
half of them decay? Perform a similar calculation without time dilation and compare
9. A train travels along the x-axis past a platform at a speed v. A passenger at rest
in the train holds a measuring ruler of length L parallel to the x-axis. Determine
the speed at which the train must be travelling in order for the length of the ruler as
measured by the observer at the platform to be L/3.
10. Consider two inertial systems of reference Joe and Moe. Moe moves with velocity
v with respect to Joe. In Joe’s frame of reference a ray of light is shot at t = 0 from
x = L towards the origin where a mirror reflects it back. The ray reaches x = 2L at
time t1 . Draw a spacetime of the situation as seen by Joe. Draw also the situation
as seen by Moe who is moving with positive velocity v &lt; c along Joe’s x-axis.
Further Exploration. Here are some more challenging and diverse problems to