Requirement Details
Electron Ion Collider
P-HSR-MAG-Q6.10
Requirement details, history, relationships and interfaces associated with requirement P-HSR-MAG-Q6.10
CURRENT RECORD- ARCHIVE RECORDS
- RELATIONSHIPS
- INTERFACES
| Record Date: 02/18/2025 18:26 | |||
| Identifier: | P-HSR-MAG-Q6.10 | WBS: | 6.05.02.01 |
| Date Modified: | TBD: | FALSE | |
| Status Date: | Status: | Not Applicable | |
| Description: | The magnet shall be designed with components capable to withstand a radiation dose of TBD MGy, or be approved by EIC for use in a specific location as shown in the “BNL Materials” List Doc. No. TBD. | ||
| Comments: | |||
| Record Date: 02/13/2025 19:28 | |||
| Identifier: | P-HSR-MAG-Q6.10 | WBS: | 6.05.02.01 |
| Date Modified: | TBD: | FALSE | |
| Status Date: | Status: | In Process | |
| Description: | The magnet shall be designed with components capable to withstand a radiation dose of TBD MGy, or be approved by EIC for use in a specific location as shown in the “BNL Materials” List Doc. No. TBD. | ||
| Comments: | |||
| Record Date: 01/28/2025 17:40 | |||
| Identifier: | P-HSR-MAG-Q6.10 | WBS: | 6.05.02.01 |
| Date Modified: | TBD: | FALSE | |
| Status Date: | Status: | In Process | |
| Description: | The magnet shall be designed with components capable to withstand a radiation dose of TBD MGy, or be approved by EIC for use in a specific location as shown in the BNL Materials List Doc. No. TBD. | ||
| Comments: | |||
| Record Date: 01/27/2025 16:43 | |||
| Identifier: | P-HSR-MAG-Q6.10 | WBS: | 6.05.02.01 |
| Date Modified: | TBD: | FALSE | |
| Status Date: | Status: | In Process | |
| Description: | The magnet shall be designed with components capable to withstand a radiation dose of TBD MGy, or be approved by EIC for use in a specific location as shown in the “BNL Materials” List Doc. No. TBD. | ||
| Comments: | |||
| Parents | |
| F-IR-HSR-LATTICE.2 | The hadron beamline lattice elements through the IR shall have a large enough aperture throughout to accommodate a minimum of 10σ spread in x and y of the incoming hadron beam at all energies without obstruction for all energies set forth in [5.8]. |
| F-IR-HSR-LATTICE.14 | At the IP of the hadron lattice the dispersion, its derivative and alpha shall all be 0 ,and the beta βx βy shall be chosen to deliver the colliding beam parameters set forth in [5.8] |
| F-IR.2 | The IR shall guide the hadron and electron beams to collide at the IP of IR6. |
| F-IR.4 | The IR electron and hadron beam lines shall have the linear lattice functions matched to the incoming and outgoing arcs of the ESR and HSR respectively. |
| F-IR.8 | The IR shall be designed to ensure the hadron and electron beam collisions at the IP meet all the performance requirements set forth in [5.8]. |
| F-IR.9 | The IR shall be designed so that the electron and hadron beams have the same cross-sectional area and maximum overlap to achieve the high luminosities required in [5.8]. |
| F-IR.11 | The IR operational uptime shall match the operational uptime requirements of the EIC. |
| Children | |
| No children. | |
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