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This is lab report for Advanced Physics Course. It was submitted to Prof. Dhirendra Kapoor at Alliance University. Its main points are: State, Nuclear, Solid, Detector, Track, Etched, Hours, Radiation, Damage, Direction, Dent, Cosmic, Ray
Typology: Exercises
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Abstract
The characteristics of Solid State Nuclear Track Detectors (SSNTDs) and their detection mechanism of heavy nuclear charge particles, such as alpha particles and fission fragments, were studied. The strips of CR-39 (Columbia Resin-39), irradiated by Am-241 (alpha source) and Cf-252 (spontaneous fission source) and after being etched in NaOH 6M solution, were analyzed under optical microscope and diameters of the spots (tracks) left by alpha particles and fission fragments were measured. The relationship between track diameter and etching time was studied and critical angle of incidence of the particle on the strip required for the track formation was also determined.
Introduction
A solid-state nuclear track detector or SSNTD (also known as an etched track detector or a dielectric track detector, DTD) is a section of a solid material (photographic emulsion, crystal, glass or plastic) exposed to nuclear radiation (neutrons or charged particles, intermittently as well gamma rays), etched, and inspected microscopically. The pathway of nuclear particles are imprinted quicker than the body substance, in addition to the range and form of these trails acquiesce knowledge regarding the charge, mass, direction of motion of the particles as well as the energy. The benefits over other radiation detectors include the thorough knowledge accessible on distinctive particles, the perseverance of the passageways permitting measurements to be made over extended periods of time, and the easy, inexpensive and hearty construction of the detector.
The foundation of SSNTDs is that charged particles break the detector within nanometers down the path in such a way that the path can be imprinted persistently more rapidly than the unspoiled substance. Engraving, characteristically for some hours, extends the dent to tapering depths of micrometer dimensions, which can be seen with a microscope. For a known particle, the span of the pathway shows the energy of the particle. The charge can be acquired from the carve rate of the pathway in contrast to that of the main part. If the particles go through the exterior at normal incidence, the depths are circular; or else the ellipticity and direction of the elliptical pit mouth suggests the direction of incidence.
SSNTDs are frequently used to learn more about cosmic rays, long-standing radioactive elements, radon concentration in houses, and the age of geological samples.
A substance frequently used in SSNTDs is polyallyl diglycol carbonate (PADC), also known as Tastrak, CR-39. It is a transparent, colorless, inflexible plastic with the chemical formula C 12 H 18 O 7. Etching to expose radiation damage is typically performed using solutions of caustic alkalis such as sodium hydroxide, regularly at high temperatures for a number of hours.
Procedure
Where,
Vb = bulk etching rate
Vt = track etching rate
Where,
Dff = Diameter of fission fragments
Dα = Diameter of alpha particles
t = Etching time
Then, critical angel was determined as:
For etching time, t = 10.5 hrs
Dff Dα 23 9 24 8 27 8 23 8 22 8 25 7 24 8 23 8 24 7 22 9 Average = 23.7 μm Average = 8 μm
Average Dff = 23.7 μm
Average Dα = 8 μm
Discussion
The spots produce by fission-fragments was having larger diameter than that of alpha-particles. The reason is that fission fragments have a wide spectrum from lighter (A: 60-120) and heavier (A: 120-160) fragments. The lightest fragments produced is even heavier that alpha-particle. Thatās the reason that F.F caused more damaged than alpha-particle.
The curve between etching-time and diameter is an increasing curve. The etchant doesnāt get enough time to dissolve the damaged area for smaller etching-time. In case of large etching time the revere is prominent.
This detector cannot be used for neutron and gamma-rays because they are not directly ionizing particles. Beta rays also donāt produce tracks or spots. This method of detection is suitable for particles heavier than proton.
Conclusion
By taking into account the results of the experiment, it can be concluded that this technique can be implemented in prospecting the radon and ultimately uranium. Efficiency is comparatively poor may be because of our inefficiency in noting dimension of different spots of fission fragments and alpha particles.
Since a CR-39 chip cannot be used again therefore the information is permanent and canāt be erased, as compared with TLDās. This technique gives the accumulated dose in a given interval of time.
References