Difference: IntroDip (1 vs. 11)

Revision 11
29 Nov 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short total length (2.5m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
>
>		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1m x 3m) and the comparably short total length (2.5m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
 

The main parameters of the dipole magnet are summarised in the table below.

Revision 10
26 Nov 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short total depth (2.5m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
>
>		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short total length (2.5m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
 

The main parameters of the dipole magnet are summarised in the table below.

Line: 23 to 23
 
Total Inductance 0.87 H
Stored energy 2.03 MJ
Weight 220 t
Changed:
<
<
Dimensions (H × W × D) 3.88 × 5.3 × 2.5 m3
>
>
Dimensions (H × W × L) 3.88 × 5.3 × 2.5 m3
 
Gap opening (H × W ) 0.80 − 1.01 × 3.10 m2

For details of the fields in the target region please refer to the solenoid description.
Revision 9
26 Nov 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short depth (1.64m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
>
>		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short total depth (2.5m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
 

The main parameters of the dipole magnet are summarised in the table below.

Line: 23 to 23
 
Total Inductance 0.87 H
Stored energy 2.03 MJ
Weight 220 t
Changed:
<
<
Dimensions (H × W × D) 3.88 × 5.3 × 1.64 m3
>
>
Dimensions (H × W × D) 3.88 × 5.3 × 2.5 m3
 
Gap opening (H × W ) 0.80 − 1.01 × 3.10 m2

For details of the fields in the target region please refer to the solenoid description.
Revision 8
25 Nov 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 As fixed target experiment PANDA requires excellent momentum reconstruction for particles emitted in forward angles. The forward magnetic spectrometer will allow to reconstruct charged particle tracks from 0° up to 10° (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short depth (1.64m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, such that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
>
>		 As a fixed target experiment, PANDA requires excellent momentum reconstruction for particles emitted at forward angles. The forward magnetic spectrometer will allow the reconstruction of charged particle tracks from 0° up to 10° horizontally (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short depth (1.64m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, so that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).
 

The main parameters of the dipole magnet are summarised in the table below.

Description Value
Field integral 2 Tm
Bending variation ≤ ±15%
Changed:
<
<
Vert. Acceptance ±5°
Horiz. Acceptance ±10°
>
>
Vertical Acceptance ±5°
Horizontal Acceptance ±10°
 
Ramp speed 1.25%/s
Total dissipated power 360 kW
Total Inductance 0.87 H
Stored energy 2.03 MJ
Weight 220 t
Changed:
<
<
Dim. (H × W × D) 3.88 × 5.3 × 1.64 m3
>
>
Dimensions (H × W × D) 3.88 × 5.3 × 1.64 m3
 
Gap opening (H × W ) 0.80 − 1.01 × 3.10 m2

For details of the fields in the target region please refer to the solenoid description.
Revision 7
23 Nov 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part will be a large-aperture dipole magnet which will ensure momentum resolution of ≤ 1% by providing an integral field of 2Tm. Since the dipole magnet will be part of the HESR lattice the magnet is designed to be ramped in sync with the accelerator. Additional field clamps are foreseen to shield stray fields. The main parameters are summarised in the table below.
>
>		 As fixed target experiment PANDA requires excellent momentum reconstruction for particles emitted in forward angles. The forward magnetic spectrometer will allow to reconstruct charged particle tracks from 0° up to 10° (5° vertically) with a momentum resolution of ≤ 1%. The central part of this spectrometer will be the large-aperture dipole magnet which will provide a bending power of 2Tm. Particular challenges are the large opening (about 1 x 3m) and the comparably short depth (1.64m) in conjunction with the requirements on stray fields and the accommodation of detectors within the yoke gap. The lamination of the flux return yoke will ensure the required ramping capabilities, such that the magnet can be operated fully synchronous with the High Energy Storage Ring (HESR).

The main parameters of the dipole magnet are summarised in the table below.
 

Description Value
Field integral 2 Tm
Line: 24 to 26
 
Dim. (H × W × D) 3.88 × 5.3 × 1.64 m3
Gap opening (H × W ) 0.80 − 1.01 × 3.10 m2
Added:
>
>		 For details of the fields in the target region please refer to the solenoid description.
 

Revision 6
28 Oct 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
Changed:
<
<		 Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part will be the dipole magnet which will provide an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%. The main parameters are summarised in the table below.
>
>		 Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part will be a large-aperture dipole magnet which will ensure momentum resolution of ≤ 1% by providing an integral field of 2Tm. Since the dipole magnet will be part of the HESR lattice the magnet is designed to be ramped in sync with the accelerator. Additional field clamps are foreseen to shield stray fields. The main parameters are summarised in the table below.
 

Description
<-- -->
Sorted ascending 		Value
Field integral 2 Tm
Revision 5
20 Oct 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 8 to 8
 
Changed:
<
<
  Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part is the dipole magnet which provides an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%. The main parameters are summarised in the table below.
>
>
Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part will be the dipole magnet which will provide an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%. The main parameters are summarised in the table below.
 

Description Value
Field integral 2 Tm
Revision 4
19 Oct 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 9 to 9
 
 
Changed:
<
<		 Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part is the dipole magnet which provides an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%.
>
>		 Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part is the dipole magnet which provides an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%. The main parameters are summarised in the table below.
 

Description Value
Field integral 2 Tm
Line: 17 to 17
 
Vert. Acceptance ±5°
Horiz. Acceptance ±10°
Ramp speed 1.25%/s
Changed:
<
<
Total length in z ≤ 2.5 m
>
>
Total dissipated power 360 kW
Total Inductance 0.87 H
Stored energy 2.03 MJ
Weight 220 t
Dim. (H × W × D) 3.88 × 5.3 × 1.64 m3
Gap opening (H × W ) 0.80 − 1.01 × 3.10 m2
 


Revision 3
19 Oct 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip

Dipole Magnet Overview

Changed:
<
<		 In preparation...
>
>
  Particles emmitted in forward angles (below 5 or 10° in vertical and horizontal direction, resp.) will be detected in the forward magnetic spectrometer of PANDA. Its central part is the dipole magnet which provides an integral field of 2Tm for those particles, in order to achieve the required momentum resolution of 1%.
 

Description Value
Field integral 2 Tm
Line: 15 to 19
 
Ramp speed 1.25%/s
Total length in z ≤ 2.5 m
Added:
>
>
View of the dipole magnet from the downstream side (field clamps ommitted)
View of the dipole magnet from the downstream side (field clamps ommitted)
 

________________________

-- Created by IntiLehmann - 01 Oct 2009
Changed:
<
<		 You are on: PANDA > Wiki > Magnet > Intro > IntroDip
>
>
META FILEATTACHMENT attr="" comment="View of the dipole magnet from the downstream side (field clamps ommitted)" date="1255956248" name="dipole_view.png" path="dipole_view.png" size="37274" user="IntiLehmann" version="1.1"
Revision 2
14 Oct 2009 - Main.IntiLehmann
Line: 1 to 1
 
META TOPICPARENT name="Intro"
You are on: PANDA > Wiki > Magnet > Intro > IntroDip
Line: 7 to 7
 

In preparation...
Added:
>
>
Description Value
Field integral 2 Tm
Bending variation ≤ ±15%
Vert. Acceptance ±5°
Horiz. Acceptance ±10°
Ramp speed 1.25%/s
Total length in z ≤ 2.5 m
 

________________________

-- Created by IntiLehmann - 01 Oct 2009
View topic | History: r11 < r10 < r9 < r8 | More topic actions...
 
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