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GLAST (tokamak)

GLAST (tokamak) is a physics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand GLAST (tokamak) rather than just read about it. In short: The GLAss Spherical Tokamak (or GLAST) is a name given to a set of small spherical tokamaks (i.e. magnetic confinement fusion reactors) located in Islamabad, Pakistan. They were developed by the Pakistan Atomic Energy Commission (PAEC) as part of the National Tokamak Fusion Program (NTFP) in 2008 and are primarily used for teaching and training purposes.

Key takeaways

  • GLAST (tokamak) belongs to physics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect GLAST (tokamak) to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of GLAST (tokamak) from memory before moving on to harder problems.

Reference excerpt

The GLAss Spherical Tokamak (or GLAST) is a name given to a set of small spherical tokamaks (i.e. magnetic confinement fusion reactors) located in Islamabad, Pakistan. They were developed by the Pakistan Atomic Energy Commission (PAEC) as part of the National Tokamak Fusion Program (NTFP) in 2008 and are primarily used for teaching and training purposes.

GLAST-I & GLAST-II

The first two tokamaks developed were named GLAST-I and GLAST-II. Both devices have similar principles of operation and consist of an insulated vacuum vessel made of pyrex glass. However, the central tube of GLAST-I is made of steel, while that of GLAST-II is made of glass. Studies were done in GLAST-II to identify the mechanism responsible for current generation during the start-up phase of tokamak discharge.

Diagnostics Plasma diagnostics including Langmuir triple probes, emissive probes and Optical Emission Spectroscopy systems were developed to measure basic plasma parameters such as electron temperature, electron number density, floating potential and impurity content in the discharge. The triple probe is capable of recording instantaneous plasma characteristics. Plasma current is then enhanced up to 5 kA by applying a small vertical magnetic field that provides additional plasma heating and shaping. The evolution of electron cyclotron heating (ECH)-assisted pre-ionization and subsequent current formation phases in one shot are well envisioned by probe measurements. The probe data seem to correlate with microwave absorption and subsequent light emission. Intense fluctuations in the current formation phase advocate for efficient equilibrium and feedback control systems. Moreover, the emergence of some strong impurity nitrogen lines in the emission spectrum even after few shots propose crucial need for improvement in the base vacuum level. A noticeable change in the profile's shape of floating potential, electron temperature, ion saturation current (Isat) and light emission is observed with changing hydrogen fill pressure and vertical field. The main discharge has been supported by microwave pre-ionization in the presence of optimized resonant toroidal magnetic field (TF). While optimizing the magnetic field, theoretical and experimental results of the TF profile are compared using a combination of fast and slow capacitor banks. The magnetic field produced by poloidal field (PF) coils are compared with theoretically predicted values. It is found that calculated results are in good agreement with experimental measurement. An economical microwave source of 2.45 ± 0.02 GHz is fabricated using a magnetron obtained from a household microwave oven. Pulsed-mode operation of the magnetron is achieved through certain necessary modifications in the circuit. The magnetic field is upgraded to enhance the microwave power, where an additional electromagnet is introduced around the magnetron cavity that confines the fast moving electrons. This modified microwave source is sufficient to achieve the breakdown in GLAST-II with improved plasma current of 5kA.

GLAST-III

GLAST-III is an upgraded version of the GLAST-I and GLAST-II designs which features a larger vessel diameter and a larger central bore for the placement of diagnostic tools such as Rogowski coils and flux loops.

Diagnostics GLAST-III retained most of the diagnostics used in GLAST-I and GLAST-II, but a newly developed spectroscopic system based on linear photodiode array was installed on the upgraded GLAST-III for spatial and temporal characterization of hydrogen discharge through light emission. The spectral range of each silicon photodiode is from 300 nm to 1100 nm with response time of 10 ns and active area of 5 mm2 (circular). The light from the plasma is collected through holes along 4 line-of-sight channels with spatial resolution of about 5 cm passing from entire poloidal cross section. The photodiode's signals located at position of 10 and 14 cm from inboard side show fluctuations in the central plasma region. Moreover, the sequence of plasma lighting shows that plasma instigates from the central resonant field region and then expands outwards. At lower pressure, outboard movement of the plasma is slower suggesting better plasma confinement. In addition to photodiode array, an optical spectrometer (Ocean Optics HR2000+) has been used to record the visible spectrum over the selected range (597–703 nm) with a spectral resolution of 0.15 nm. The studies have been conducted during initial phase of plasma formation for two different hydrogen gas fill pressures. The triple probe is used to get time-resolved information on plasma parameters in the edge region. The time evolution of whole discharge including microwave pre-ionization phase and current formation phase has been demonstrated by temporal profiles of light emission and plasma floating potential.

References

Further reading "Pakistan launches national fusion program". ITER. International Thermonuclear Experimental Reactor. Retrieved 6 January 2013.

Worked examples

Example 1 — a first encounter with GLAST (tokamak)

Start with the simplest possible case. Write down what GLAST (tokamak) claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In physics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to GLAST (tokamak) before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about GLAST (tokamak) ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of GLAST (tokamak)

In research
GLAST (tokamak) appears in physics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses GLAST (tokamak) in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
GLAST (tokamak) is common in secondary-school and first-year university syllabi. It links to neighbouring topics Nuclear technology in Pakistan, Tokamaks, so understanding it makes those chapters shorter.
In everyday life
Look for GLAST (tokamak) outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study GLAST (tokamak) in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what GLAST (tokamak) means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain GLAST (tokamak) out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is GLAST (tokamak) in simple terms?

The GLAss Spherical Tokamak (or GLAST) is a name given to a set of small spherical tokamaks (i.e. magnetic confinement fusion reactors) located in Islamabad, Pakistan. They were developed by the Pakistan Atomic Energy Commission (PAEC) as part of the National Tokamak Fusion Program (NTFP) in 2008 a…

Why does GLAST (tokamak) matter?

Because it connects several physics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study GLAST (tokamak)?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on GLAST (tokamak).

Tags

  • Nuclear technology in Pakistan
  • Tokamaks

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