LNF ICTS

TJ-II

Stellarator (confinamiento magnético) para investigación en física de plasmas de fusión

TJ-II

¿Qué es TJ-II y para qué se usa?

TJ-II es un dispositivo experimental de tipo stellarator (confinamiento magnético) utilizado para generar y estudiar plasmas en condiciones controladas. Su propósito es apoyar investigación de fusión mediante el desarrollo, validación y explotación de procedimientos experimentales y técnicas de diagnóstico.

Objetivos principales de la campaña
  • Cualificar procedimientos experimentales y técnicas de diagnóstico.
  • Validar modelos de física de stellarators.
  • Dar soporte a la explotación científica de W7-X.
En esta campaña (Spring 2024), TJ-II ofrece
  • Campo magnético: 0.5–1.0 T (en eje)
  • Pulso: ≤ 300 ms (flat-top)
  • Repetición: 1 pulso / 10 min (≈ 35 pulsos / sesión)
  • Calentamiento ECRH: 500 kW / 250 ms (modo X2, 53.2 GHz; on/off-axis; ECCD)
  • Calentamiento NBI: 1000 kW / 100 ms (energía 20–30 keV; potencia 200–500 kW)
  • Acondicionamiento de pared: Boronization + Lithiumization
  • Extra: dynamic magnetic configuration scan en un solo disparo

La operación se organiza en campañas con disparos (pulsos) repetitivos. Esta página resume la información esencial de la campaña y el conjunto de diagnósticos disponibles.

Enlaces

Si necesitas acceso o detalles operativos (planificación, propuestas, condiciones de uso), consulta la documentación oficial o contacta con el equipo responsable.

Essential Campaign Information Sheet

General

Campaign Spring 2024
From 12 Feb 24
To 30 May 24
Main goal(s) Qualify experimental procedures and diagnostic techniques. Validate stellarator physics models. Support the scientific exploitation of W7-X.
Proposal submission by
(Enlace indicativo: ajusta aquí la URL del formulario si es diferente)

Operación

B on-axis 0.5 – 1.0 Tesla
Max. flat-top length ≤ 300 ms
Pulse repetition one every 10 minutes (35 pulses/session on average)
ECRH heating
500 kW / 250 ms
Remarks: X2 mode (53.2 GHz). Higher power can be achieved in shorter pulses. On-axis/off-axis as well as ECCD capabilities.
NBI heating
1000 kW / 100 ms
Remarks: NBI#1 Co / NBI#2 Counter. Beam energy can be varied between 20 keV and 30 keV. Corresponding beam power between 200 kW and 500 kW.
Wall conditioning Boronization and Lithiumization
Others Capability for dynamic magnetic configuration scan in a single shot

Diagnostics

Tabla filtrable. Usa el buscador para localizar un diagnóstico y, si lo necesitas, activa “Solo operativos” para ver únicamente los sistemas disponibles.

System R.O. Status Capabilities
Thomson Scattering I. Pastor Operational 1 shot per discharge, medium-to-high spatial resolution Te and ne profiles along plasma chord. Best in NBI phase (due to increased density). Not very reliable @ densities below ≈ 0.5 × 1019 m-3. As of 30/10/2023 both ICCD cameras are in operation. Please request TS measurements whenever necessary, but only if necessary.
Microwave Interferometer T. Estrada Operational Time trace of the central line-integrated electron density. Less reliable for high densities (above 3–4e19 m-3) due to spurious phase jumps. Fundamental for machine operation.
Mirnov coil arrays A. Cappa
P. Pons
Operational Four sets of magnetic coils digitised at 1 Ms/s:
  • 2 “vertical” arrays located at sectors B5 and C4 (four triaxial coils each)
  • A poloidal array at sector D5 (less than 15 coils remain useful)
  • 2 helical arrays covering sector D (32 triaxial coils each)
Diamagnetic loop A. Cappa
F. Lapayese
A. Pereira
Operational Time trace roughly proportional to plasma energy content. Strongly perturbed by plasma current. Correction acceptable for small currents (|Ip| ≤ 1 kA), not for high plasma currents.
Rogowski coil A. Cappa
F. Lapayese
A. Pereira
Operational Time trace proportional to the plasma current.
AM Reflectometer T. Estrada Operational Edge density profiles with temporal resolution of 2 ms. Reconstructed profiles often have large uncertainties; raw data commonly used in Bayesian approaches (with interferometry and Thomson scattering) to reconstruct density profiles.
Doppler Reflectometer T. Estrada Operational Density turbulence and perpendicular rotation velocity (E×B velocity) with good temporal, spatial and spectral resolution. Radial range ~ ρ = 0.5–0.9; k⊥ selectable between 3 and 15 cm-1.
ECE T. Estrada Operational Electron temperature profiles using a 12-channel heterodyne radiometer (50–60 GHz), corresponding to second harmonic ECE in X-mode at B = 0.95 T on-axis. Most channels receive radiation from the HFS.
Heavy Ion Beam Probe J. L. de Pablos Operational Two HIBP systems measuring plasma electrostatic potential and electron density (HIBP1 and HIBP2a; 2 and 5 simultaneous sample volumes respectively, poloidally separated). Signal bandwidth: 1 MHz (density), 250 kHz (potential). Full in-out radial scan. Beam attenuation tolerable until 2e19 m-3 line-averaged density.
H pellet and TESPEL injection K. J. McCarthy Operational 4 pellets or 3 pellets & TESPEL per discharge.
Langmuir probes M. Ochando
I. Voldiner
Operational Two systems of reciprocating multi-pin LP provide radial profiles of Vf, Isat, Te, Er, Ep and their fluctuations in the plasma periphery.
Charge exchange spectroscopy J. Hernández
K. McCarthy
Non operational Vi, Ti and Er from ρ = 0 to 0.7 once per discharge.
Bolometry F. Medina Operational Three 20-channel arrays for tomographic reconstruction of plasma emissivity (2 eV to 5 keV) plus three 16-channel arrays to detect toroidal asymmetries of global plasma radiation.
Motional Stark Effect K. J. McCarthy
J. Hernández
Non operational Bz & Bphi & pitch, from ρ = 0 to 0.7, once per discharge.
Soft X-rays Tomography F. Medina Operational Four 16-channel arrays for tomographic reconstruction of soft X-ray (SXR) emissions (0.7–5 keV). Fifth camera (thinner Al/C filter) at same toroidal position monitors fast events up to 1 MHz.
SXR Multifilter diagnostic F. Medina Operational Two twin sets of four SXR detectors, each with a different Be filter, to obtain coarse spectral information. Te and Zeff can be estimated for NBI plasmas.
SXR Spectroscopy F. Medina Non operational Being upgraded / not operative. PHA technique with Silicon Drift detector. Several collimators and Be filters. System can be tilted vertically for radial scans shot-to-shot.
Supersonic He beam D. Tafalla Operational ne & Te profiles from ρ = 1.0 to 0.8. Number of profiles is limited.
Fast cameras E. de la Cal
N. Panadero
Operational APX-RS in sector B2 (pellet injector): single or double bundle for TOP, SIDE and/or TANG view, or in sector A1 (LBO): single bundle for TOP view. Speed: 3 kpfs @ 1024×1024, 10 kfps @ 512×512, 250 kfs @ 128×16. Min. exposure time: 1 μs.
Fast Ion Loss detector B. López-Miranda
A. Baciero
D. Jiménez Rey
Operational Energy (Ti) and pitch angle of fast ion loss from plasma edge under NBI co-injection (and ECRH). PMT (sampling up to MHz) for integrated light trend and CCD fast camera for phase-space study. Typical integration time 5–10 ms up to 200 ms.
Scanner system B. López-Miranda
A. Baciero
Operational Selects a wavelength with a 1/2 m spectrometer and rotating mirror to obtain spatial profile for Zeff. Mirror can be bypassed with optical fibre to measure at central chord (A1).
CCD + 1/2 m spectrometer B. López-Miranda
A. Baciero
Operational 1/2 m spectrometer to measure one spectrum in selected wavelength with the CCD (A1).
PMA12 B. López-Miranda
A. Baciero
Operational Low spectral resolution but wide spectral band (200 to 900 nm) every 20 ms (A1).
Laser Blow-Off & LIBS B. López-Miranda
A. Baciero
Operational Nd:YAG IR laser (1064 nm, up to 800 mJ, 10 Hz) used for blow-off experiments (e.g., Fe injection) and LIBS studies (LiLA-TOF) (A1).
CV monitor B. López-Miranda
A. Baciero
Operational With a monochromator, the 227.1 nm wavelength (CV) is selected and measured with a photomultiplier (B5).
CCD + 1 m spectrometer B. López-Miranda
A. Baciero
Operational Measures selected wavelength with spatial resolution. Usually measures Halpha, CV or CIII (B5).
D1461 B. López-Miranda
A. Baciero
Operational Linear array + high resolution spectrometer to measure Halpha/Dalpha spectrum, typically every 15 ms (B5).
Neutral Particle Analyzers J. Hernández
A. Ros
J. M. Fontdecaba
Operational Ti along 2 radial lines-of-sight with 1 ms resolution. Usually scans neutrals in the 200–1200 eV range (12 energy channels per LOS) for Ti calculation. Can change energy range up to 20 keV. LOS can be changed from centre to edge.
Spectroscopic Gas Puff Imaging E. de la Cal
I. Voldiner
Operational 2D imaging of edge plasma ne and Te. Helium injection is mandatory.
Compact Neutral Particle Analyzers J. Hernández Non operational Tangential line-of-sight. Scans 1–40 keV neutrals in 16 energy channels from NBI #1.