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PHY 4822L (Advanced Laboratory):
Analysis of a bubble chamber picture
Introduction
In this experiment you will study a reaction between
“elementary particles” by analyzing their
tracks in a bubble chamber. Such particles are everywhere
around us [1,2]. Apart from the standard
matter particles proton, neutron and electron, hundreds of other
particles have been found [3,4],
produced in cosmic ray interactions in the atmosphere or by
accelerators. Hundreds of charged
particles traverse our bodies per second, and some will damage
our DNA, one of the reasons for the
necessity of a sophisticated DNA repair mechanism in the cell.
2
Figure 1: Photograph of the interaction between a high-energy
π--meson from the Berkeley
Bevatron accelerator and a proton in a liquid hydrogen bubble
chamber, which produces two neutral
short-lived particles Λ0 and K0 which decay into charged
particles a bit further.
Figure 2: illustration of the interaction, and identification of
bubble trails and variables to be
measured in the photograph in Figures 3 and 4.
The data for this experiment is in the form of a bubble chamber
photograph which shows bubble
tracks made by elementary particles as they traverse liquid
hydrogen. In the experiment under
study, a beam of low-energy negative pions (π- beam) hits a
hydrogen target in a bubble chamber.
A bubble chamber [5] is essentially a container with a liquid
kept just below its boiling point (T=20
K for hydrogen). A piston allows expanding the inside volume,
thus lowering the pressure inside
the bubblechamber. When the beam particles enter the
detector a piston slightly decompresses the
liquid so it becomes "super-critical'' and starts boiling, and
bubbles form, first at the ionization
trails left by the charged particles traversing the liquid.
The reaction shown in Figure 1 shows the production of a pair
of neutral particles (that do not leave
a ionized trail in their wake), which after a short while decay
into pairs of charged particles:
π - + p → Λo + Ko,
3
where the neutral particles Λo and Ko decay as follows:
Λo → p + π-, Ko → π+ + π-.
In this experiment, we assume the masses of the proton (mp =
938.3 MeV/c2) and the pions (mπ+ =
mπ- = 139.4 MeV/c2) to be known precisely, and we will
determine the masses of the Λ0 and the K0,
also in these mass energy units.
Momentum measurement
In order to “reconstruct” the interaction completely, one uses
the conservation laws of (relativistic)
momentum and energy, plus the knowledge of the initial pion
beam parameters (mass and
momentum). In order to measure momenta of the produced
charged particles, the bubble chamber is
located inside a magnet that bends the charged particles in
helical paths. The 1.5 T magnetic field is
directed up out of the photograph. The momentum p of each
particle is directly proportional to the
radius of curvature R, which in turn can be calculated from a
measurement of the “chord length” L
and sagitta s as:
r = [L2/(8s)] + [s/2] ,
Note that the above is strictly true only if all momenta are
perfectly in the plane of the photograph;
in actual experiments stereo photographs of the interaction are
taken so that a reconstruction in all
three dimensions can be done. The interaction in this
photograph was specially selected for its
planarity.
In the reproduced photograph the actual radius of curvature R of
the track in the bubble chamber is
multiplied by the magnification factor g, r = gR. For the
reproduction in Figure 3, g = height of
photograph (in mm) divided by 173 mm.
The momentum p of the particles is proportional to their radius
of curvature R in the chamber. To
derive this relationship for relativistic particles we begin with
Newton's law in the form:
F = dp/dt = e v×B (Lorentz force).
Here the momentum (p) is the relativistic momentum m v γ,
where the relativistic γ-factor is defined
in the usual way
γ = [√(1- v 2/c2)]-1.
Thus, because the speed v is constant:
F = dp/dt = d(mvγ)/dt = mγ dv/dt = mγ (v2/R)(-r) = e v B (-r) ,
where r is the unit vector in the radial direction. Division by v
on both sides of the last equality
finally yields:
mγv /R = p /R = e B ,
identical to the non-relativistic result! In “particle physics
units” we find:
p c (in eV) = c R B , (1)
4
thus p (in MeV/c) = 2.998•108 R B •10-6 = 300 R (in m) B
(in T)
Measurement of angles
Draw straight lines from the point of primary interaction to the
points where the Λ0 and the K0
decay. Extend the lines beyond the decay vertices. Draw
tangents to the four decay product tracks at
the two vertices. (Take care drawing these tangents, as doing it
carelessly is a source of large
errors.) Use a protractor to measure the angles of the decay
product tracks relative to the parent
directions (use Fig. 3 or 4 for measurements and Fig. 2 for
definitions).
Note: You can achieve much better precision if you use graphics
software to make the
measurements, rather than ruler and protractor on paper.
Examples of suitable programs are
GIMP or GoogleSketchUp, both of which can be obtained for
free.
Analysis
The laws of relativistic kinematics relevant to this calculation
are written below. We use the
subscripts zero, plus, and minus to refer to the charges of the
decaying particles and the decay
products.
p+sinθ+ = p-sinθ-
(2)
p0 = p+cosθ+ + p-cosθ-
(3)
E0 = E+ + E-,
where E+ = √(p+2c2 + m+2c4) , and E- = √(p-2c2 + m-
2c4)
m0c2 = √(E02 - p02c2)
Note that there is a redundancy here. That is, if p+, p-, θ+, and
θ- are all known, equation (2) is not
needed to find m0. In our two-dimensional case we have two
equations (2 and 3), and only one
unknown quantity m0, and the system is over-determined. This
is fortunate, because sometimes (as
here) one of the four measured quantities will have a large
experimental error. When this is the case,
it is usually advantageous to use only three of the variables and
to use equation (2) to calculate the
fourth. Alternatively, one may use the over-determination to
"fit'' m0, which allows to determine it
more precisely.
A. K0 decay
1. Measure three of the quantities r+, r-, θ+, and θ-. Omit the
one which you believe would
introduce the largest experimental error if used to determine
mK. Estimate the uncertainty of
your measurements.
2. Use the magnification factor g to calculate the actual radii R
and equation (1) to calculate the
momenta (in MeV/c) of one or both pions.
3. Use the equations above to determine the rest mass (in
MeV/c2) of the Ko.
4. Estimate the error in your result from the errors in the
measured quantities.
5.
5
Β. Λo decay:
1. The proton track is too straight to be well measured in
curvature. Note that θ+ is small and
difficult to measure, and the value of mΛ is quite sensitive to
this measurement. Measure θ+, r-
and θ-. Estimate the uncertainty on your measurements.
2. Calculate mΛ and its error the same way as for the Ko.
3. Estimate the error in your result from the errors in the
measured quantities.
4. Finally, compare your values with the accepted mass values
(the world average) [3], and
discuss.
C. Lifetimes:
Measure the distance traveled by both neutral particles and
calculate their speed from their
momenta, and hence determine the lifetimes, both in the
laboratory, and in their own rest-frames.
Compare the latter with the accepted values [3]. Estimate the
probability of finding a lifetime value
equal or larger than the one you found.
References:
[1] G.D. Coughlan and J.E. Dodd: “The ideas of particle
physics”, Cambridge Univ. Press,
Cambridge 1991
[2] “The Particle Adventure”, http://particleadventure.org/
[3] Review of Particle Physics, by the Particle Data Group,
Physics Letters B 592, 1-1109
(2004) (latest edition available on WWW: http://pdg.lbl.gov )
[4] Kenneth Krane: Modern Physics, 2nd ed.; John Wiley &
Sons, New York 1996
[5] see, e.g. K. Kleinknecht: “Detectors for Particle Radiation”,
Cambridge University Press,
Cambridge 1986;
R. Fernow: “Introduction to Experimental Particle Physics”,
Cambridge University Press,
Cambridge 1986;
W. Leo: Techniques for Nuclear and Particle Physics
Experiments :
A How-To Approach; Springer Verlag, New York
1994 (2nd ed.)
Note: Experiment adapted from PHY 251 lab at SUNY at Stony
Brook (Michael Rijssenbeek)
6
Figure 3 : Photograph of the interaction between a high-energy
π--meson from the Berkeley
Bevatron accelerator and a proton in a liquid hydrogen bubble
chamber. The interaction produces
two neutral particles Λ0 and K0, which are short-lived and
decay into charged particles a bit further.
The photo covers an area (H•W) of 173 mm • 138 mm of the
bubble chamber. In this enlargement,
the magnification factor g = (height (in mm) of the photograph
)/173 mm.
7
Fig. 4: Negative of picture shown in Fig. 3
HIGHER COLLEGE OF TECHNOLOGY
DEPARTMENT: BUSINESS STUDIES
Final Examination:
Assignment Based Assessment
Semester: II A. Y.: 2019 / 2020
Diploma I and II Year
Start Date: 16-5-2020 Time: 9:00AM
Due Date: 18-5-2020 Time: 9:00AM
Student Name
Student ID
Specialization
Section
Level Diploma I –Year
Course Name Principles of Microeconomics
Course Code BAEC1203
For official Use Only
Question No. Max. Marks
Obtained
Marks
Question No.
Max.
Marks
Obtained
Marks
1 5 1 5
2 5 2 5
3 5 3 5
4 5 4 5
5 5 5 5
6 5 6 5
7 5 7 5
8 5 8 5
9 5 9 5
10 5 10 5
Grand Total
Marks 50 50
First Marker: Second Marker:
Date: Date:
Guidelines for Students to Submit the Assignment:
1) The final assessment for semester 2, 2019-20 will be done
through comprehensive
assignment for a maximum of 50 marks. The schedule of the
final assessment is
available in the college website.
https://www.hct.edu.om/about/the-
college/announcements/final-assessment-timetable-041620
2) All the students are expected to have only one assignment at
one time. In case, if the
students have more than one assignment on the same day, please
report to the exam
committee through the following mail id. [email protected] as
soon as possible.
3) All students are given 48 hours to complete and submit each
assignment from the day,
date and time the assignment is uploaded. Students are advised
not to wait till the last
moment of the deadline to submit the assignment.
4) The students can check the assignment anytime and any
number of times from the
opening of the assignment. The answer to the assignment need
to be uploaded in e-
learning within 48 hours.
5) The answer to the assignment can be uploaded only one time.
No requests for
resubmission of the assignment will be entertained.
6) In case students face any difficulties while uploading the
assignment in e-learning,
they can contact ETC helpdesk.
For Academic related support :
Business Courses
For Technical Writing 1
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cted][email protected]
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7) Student may contact their respective lecturer through email
(within the 48-hour period
given) if they have any doubts and clarifications on the
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independent assessment. Students
are not allowed to get help from any other person during the
assessment period.
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investigated in case of plagiarism as per the College policy and
procedures.
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submission of assignment,
the answer to the assignment can be mailed to the concerned
lecturer within the 48-
hour period.
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evaluation.
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format is acceptable at all (e.g. pictures, JPEG, PDF, etc.)
13) The students need to answer the assignment in the
prescribed number of words as
mentioned in the assignment.
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preparing the assignment :
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Font Size: 12 point for body and 14 point for Headings
Line Spacing: 1.5
Margin: 2.54cm (One inch) on all the sides
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15) Students who will fail to submit their assignment as per the
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required to make an online appeal along with the valid excuses
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Main Instructions:
16) At the time of answer papers submission in the E-Learning,
Students have to follow
the two things importantly:
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learning, Students have
to delete all instructions points from the answer sheet (1-16)
(Guidelines
for Students to Submit the Assignment):
ii) When you are submitting the answer sheet, delete questions
from the answer
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These are the above two instructions, students have to be
followed strictly. Then
only it will show less plagiarism percentage, if students are not
followed, it shown
more plagiarism, due to that you marks may be low.
All the Best
CASE STUDIES
(Suggested time: 48 hours)
Answer all the questions given below the case studies. For
every question
given, it should be answered with minimum fifty hundred (50)
words and
maximum hundred (100) words per question.
Part-I
Food delivery is the present trend nowadays especially that
most people are required to stay
home. In the case of Patsy restaurant, the company has
effectively operated in Oman for
many years catering to non-Omani and Omani foods. With the
required take-out and home
delivery only, the restaurant has to reduce the workforce. Some
of the Cooks were separated
and one of them is Zara’s father. The family has stayed in
Oman living comfortably. Her
family enjoys their wealth by spending on different luxury
products. Now that the father
loses his job, the family started to live on their remaining
limited resources.
Q1 What concept/s can best describe the situation and how can
the family survive their
present condition. (5 Marks)
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Part-II
Zara’s family did not lose hope. The father can either look for
another restaurant for
employment or partner with other friends to start a homemade
cooked food delivery. But
before they decided on this business, the group conducted a
study to finally make a choice of
a new venture. Now their problem is to choose which business
will continue to support their
families.
Q2 Explain the five problems that must be faced (or) dealt with
before attempting to
start the business. (5 Marks)
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Q3 Describe the opportunity cost of each choice whether to
apply for another job or put
up a business. Defining Opportunity cost 2.5 Marks+ answer
related to case 2.5 Marks)
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Part-III
In order to assure success, the new business has to consider the
demand and supply situations
in Oman. The new delivery business may face competition with
similar business but offering
other type of food (Asian, Indian, Arabic dishes). Now that
there is a lockdown, the supply
of some of the materials needed may not be available in the
market. Further, some homes are
also extra careful in ordering food and would rather cook their
own in their kitchen. The new
business will also have to prove that they are practicing safety
measures to assure customers
that their food is safe. They found out that the present virus
situation has led to shortage of
protective items like masks and gloves.
Q4 Explain five factors that can specifically affect the increase
and decrease in the
demand for the homemade food delivery. (5 Marks)
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Q5 Explain five factors that can specifically affect the supply
of these items that are
needed by the new business. (5 Marks)
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Part-IV
When the business was launched, initially they offered eight (8)
types of meat dishes,
vegetable dishes and seafood. There are also desserts and
sandwiches. Knowing that they
have competition with another homemade food delivery
company, the business lowered its
price from 5 RO to 3 RO per dish. Likewise, the number of
dishes was increased to ten (10).
Q6 What kind of elasticity is being shown here? Calculate the
elasticity. (5 Marks)
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Part-V
In order to minimize costs, the business uses a vacant room in
one of the partners’ house to
store the products. The business is also being run by members
of the family like their wives
and Zara and the other children. They deliver the products to
the different shops using their
own van. They deliver the products to the different shops using
their own van. Power and
Wi-Fi per month cost the business 400 RO. Raw materials
which are the ingredients for the
food costs 250 RO per week. Petrol is about 60 RO per month.
Repairs and maintenance of
the van costs 30 per month. Salaries in the form of allowances
to the two Helpers cost 35 RO
each per month. Profit for the first month was 3000 RO and
during the second month it
increased to 5,000 RO.
Q7 Solve for the firm’s: 1) fixed cost; 2) average fixed cost; 3)
average variable cost; 4)
average total cost and 5) marginal revenue for the first and
second month. (5 Marks)
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Q8 Describe the explicit and implicit costs in this situation.
(5 Marks)
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Part- VI
Putting in mind the situational demands for their homemade
foods, the business relates with
their customers on a daily basis. The business keep tract of the
market prices and the news
related to the operation of the business. Zara being a college
graduate is a big help to the
business. She gives feedback and suggest strategies to her
father and the partners. Now they
are concentrating only on specific dishes per day but since she
is aware of the competition,
the business will try to keep operating. There may be seasons
that the business may just break
even and they are expecting this.
Q9 What kind of market structure is being described here and
what other
characteristics does this market structure show. (5
Marks)
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Q10 What will the business do in the following situation
1) When the prices in the market is higher than equilibrium
price. (2.5 Marks)
2) When there is shortage of demand.
(2.5 Marks)
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…
Measurement
of
the
angle
θ
For
better
understanding
I
am
showing
you
a
different
particle
track
diagram
bellow.
Where
at
point
C
particle
�! ��� Σ!
are
created
and
the
Σ!
decays
into
�∓ ��� K!
particles
The
angle
θ
between
the
π−
and
Σ−
momentum
vectors
can
be
determined
by
drawing
tangents
to
the
π−
and
Σ−
tracks
at
the
point
of
the
Σ−
decay.
We
can
then
measure
the
angle
between
the
tangents
using
a
protractor.
Alternative
method
which
does
not
require
a
protractor
is
also
possible.
Let
AC
and
BC
be
the
tangents
to
the
π−
and
Σ−
tracks
respectively.
Drop
a
perpendicular
(AB)
and
measure
the
distances
AB
and
BC.
The
ratio
AB/BC
gives
the
tangent
of
the
angle180◦−θ.
It
should
be
noted
that
only
some
of
the
time
will
the
angle
θ
exceed
90◦
as
shown
here.
Determining
the
uncertainty
of
Measurements
In
part
B,
It
is
asked
to
estimate
the
uncertainty
of
your
measurements
of
�
and
r.
Uncertainty
of
measurement
is
the
doubt
that
exists
about
the
result
of
any
measurement.
You
might
think
that
well-­‐made
rulers,
clocks
and
thermometers
should
be
trustworthy,
and
give
the
right
answers.
But
for
every
measurement
-­‐
even
the
most
careful
-­‐
there
is
always
a
margin
of
doubt.
It
is
important
not
to
confuse
the
terms
‘error’
and
‘uncertainty’.
Error
is
the
difference
between
the
measured
value
and
the
‘true
value’
of
the
thing
being
measured.
Uncertainty
is
a
quantification
of
the
doubt
about
the
measurement
result
Since
there
is
always
a
margin
of
doubt
about
any
measurement,
we
need
to
ask
‘How
big
is
the
margin?’
and
‘How
bad
is
the
doubt?’
Thus,
two
numbers
are
really
needed
in
order
to
quantify
an
uncertainty.
One
is
the
width
of
the
margin,
or
interval.
The
other
is
a
confidence
level,
and
states
how
sure
we
are
that
the
‘true
value’
is
within
that
margin.
You
can
increase
the
amount
of
information
you
get
from
your
measurements
by
taking
a
number
of
readings
and
carrying
out
some
basic
statistical
calculations.
The
two
most
important
statistical
calculations
are
to
find
the
average
or
arithmetic
mean,
and
the
standard
deviation
for
a
set
of
numbers.
The
‘true’
value
for
the
standard
deviation
can
only
be
found
from
a
very
large
(infinite)
set
of
readings.
From
a
moderate
number
of
values,
only
an
estimate
of
the
standard
deviation
can
be
found.
The
symbol
s
is
usually
used
for
the
estimated
standard
deviation.
Suppose
you
have
a
set
of
n
readings.
Start
by
finding
the
average:
For
the
set
of
readings
x={16,
19,
18,
16,
17,
19,
20,
15,
17
and
13},
the
average
is
� = !!
!
=
17.
Next
find
(�! − �)!
Then
� =
(!!!!)!
!
!!!
!!!
= 2.21
To
calculating
standard
uncertainty
u
when
a
set
of
several
repeated
readings
has
been
taken,
use
� =
�
�
(The
standard
uncertainty
of
the
mean
has
historically
also
been
called
the
standard
deviation
of
the
mean,
or
the
standard
error
of
the
mean)
Lifetime
calculation
In
part
C
you
are
asked
to
determine
the
life
time
of
the
neutral
particles
from
their
momentums.
The
Σ−
lifetime
can
be
approximately
determined
using
the
measured
values
of
the
Σ−
track
lengths.
The
average
momentum
of
the
Σ−
particle
can
be
found
from
its
initial
and
final
values:
�! =
1
2
(�!! + �!!)
Where
�!! ��� �!!
are
initial
and
final
momentums
of
Σ
particle.
And
can
be
found
using
the
measured
track
length
�!.
The
length
of
time
that
the
Σ−lives(the
time
between
its
creation
and
decay)
is
� =
�!
�
���������� ������ �� ���� �� �ℎ� ���
� =
�!
�
1 −
�!
�!
���������� ������ ������ ���ℎ
��������
� =
�!�!
�!�
1PHY 4822L (Advanced Laboratory)  Analysis of a bu.docx

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