In the previous class,
we reviewed the Galilean transformations
for converting from the coordinates and time
measured by one observer to
the coordinates and time measured by another.
Today, we'll look at a different set of transformations,
named for Dutch scientist Hendrik Lorentz.
The **Lorentz transformations**
work properly at relativistic speeds AND at the ordinary
speeds of everyday life.

Once again, imagine two inertial frames of reference: Fred, standing on the ground, and Jane, flying past him at high speed.

We'll denote Fred's measurements (and those of his assistants) with the regular symbols:

while Jane's measurements (and those of her assistants) will be written with "prime" markers:

Jane's spaceship flies past Fred at a speed of **v** in
the positive **x**-direction, to the right.

I will not derive the Lorentz transformations here.
If you wish, you can read the derivation
in Taylor and Wheeler,
or in Professor Lindberg's notes
(see
pages 40-42 in particular).
The bottom line is that if Jane moves in the
**x**-direction
relative to Fred with velocity **v**,
then we can convert Fred's measurements
to Jane's measurements like so:

If you happen to be writing velocities
in terms of the speed of light,
so that someone moving at half the speed
of light is given a velocity **v = 0.5,**
and a beam of light is given a velocity **v = 1,**
then the final equation simplifies to

Note the BIG difference between
this set of equations and the Galilean transformations:
here, not only does the **position** of an event
depend on the observer, but the **time** of an
event depends on the observer, too.
The measurements of both space and time in the
moving reference frame depend on both the space and time
coordinates of the event in the stationary frame
(and vice versa).
It looks like we can no longer separate space
from time;
instead, events are immersed in a 4-dimensional
matrix of **space-time**.

This mixture of space and time reminds of another situation in which to distinct entities became inextricably combined, with a happy result:Hey, you got chocolate in my peanut butter!

You got peanut butter in my chocolate!

Fred stands on the ground in Rochester, in the middle of a big field. His team of students is spread out all over the field, with clocks synchronized and metersticks at the ready. Fred and his students watch as a series of events unfold.

- A long line of men stand at attention,
spaced exactly 1 meter apart.
At time
**t = 0**, each man raises his left hand. - The man standing at the left end of the line,
at
**x = 0**, has a bad cold. At time**t = 5 meters**, he coughs. At time**t = 10 meters**, he sneezes. - A cute little doggie runs across the
field at a speed of
**0.2c**to the left. At time**t = 0**, the doggie is at**x = 8 meters**. The doggie barks at time**t = 5 meters**and**t = 10 meters**. - A bird flies just above the ground,
looking for insects.
It moves at speed
**0.9c**to the right. At time**t = 0,**when the bird is at**x = -3 meters**, it chirps: "TWEET!"

Q: Make a space-time diagram which shows all these events, as measured by Fred and his team. (Your diagram should cover at least the regionx = -4tox = +11meters andt = -1tot = 16meters) (You may consider just a few moments --t = 5andt = 10meters, for example)

You can look at my graph if you wish.

Now, Jane and her team are also making careful
measurements of these same events as they
fly past at **v = 0.3c**
to the LEFT.
Use the Lorentz transformations to figure out
the locations and times of these events
in Jane's frame of reference.

Q: Make a (new) space-time diagram which shows all these events, as measured by Jane and her team.

You can look at my version of Jane's graph if you wish.

Look at your two diagrams to answer the following questions.

1. The long line of men raising their hands lies along the x-axis in Fred's space-time diagram. Do those events also lie along the x-axis in Jane's diagram? [How does this compare to your answer for the Galilean transformation?] 2. The man with a bad cold lies along the y-axis in Fred's diagram. Does he also lie along the y-axis in Jane's diagram? [How does this compare to your answer for the Galilean transformation?] 3. Consider the cough and the sneeze. What is the time interval between these two events according to Fred? According to Jane? [How does this compare to your answer for the Galilean transformation?] 4. Consider these two events: the bird chirps the bird meets the dog What is the time interval between the events according to each observer? What is the space interval between the events according to each observer? [How does this compare to your answer for the Galilean transformation?] 4a. What is the space-time interval between these two events according to each observer? 5. How fast is the bird flying, according to Jane? [How does this compare to your answer for the Galilean transformation?]

- See Taylor and Wheeler, Spacetime Physics
- Professor Vern Lindberg's notes for this course may act as a textbook for you this quarter. You may also want to see Professor Lindberg's home page for additional materials he has created.

Copyright © Michael Richmond. This work is licensed under a Creative Commons License.