Imaging properties of a photoheliograph with a Lyot plane shutter
Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Györi, L. [verfasserIn] |
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| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1985 |
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| Schlagwörter: |
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| Anmerkung: |
© D. Reidel Publishing Company 1985 |
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| Übergeordnetes Werk: |
Enthalten in: Solar physics - Kluwer Academic Publishers, 1967, 99(1985), 1-2 vom: Sept., Seite 365-369 |
|---|---|
| Übergeordnetes Werk: |
volume:99 ; year:1985 ; number:1-2 ; month:09 ; pages:365-369 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF00157319 |
|---|
| Katalog-ID: |
OLC2033558258 |
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| 520 | |a Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. | ||
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10.1007/BF00157319 doi (DE-627)OLC2033558258 (DE-He213)BF00157319-p DE-627 ger DE-627 rakwb eng 530 VZ 16,12 ssgn Györi, L. verfasserin aut Imaging properties of a photoheliograph with a Lyot plane shutter 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Company 1985 Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. Response Function Frequency Response Constant Velocity Slit Width Frequency Response Function Enthalten in Solar physics Kluwer Academic Publishers, 1967 99(1985), 1-2 vom: Sept., Seite 365-369 (DE-627)129856010 (DE-600)281593-X (DE-576)015160033 0038-0938 nnns volume:99 year:1985 number:1-2 month:09 pages:365-369 https://doi.org/10.1007/BF00157319 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4306 AR 99 1985 1-2 09 365-369 |
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10.1007/BF00157319 doi (DE-627)OLC2033558258 (DE-He213)BF00157319-p DE-627 ger DE-627 rakwb eng 530 VZ 16,12 ssgn Györi, L. verfasserin aut Imaging properties of a photoheliograph with a Lyot plane shutter 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Company 1985 Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. Response Function Frequency Response Constant Velocity Slit Width Frequency Response Function Enthalten in Solar physics Kluwer Academic Publishers, 1967 99(1985), 1-2 vom: Sept., Seite 365-369 (DE-627)129856010 (DE-600)281593-X (DE-576)015160033 0038-0938 nnns volume:99 year:1985 number:1-2 month:09 pages:365-369 https://doi.org/10.1007/BF00157319 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4306 AR 99 1985 1-2 09 365-369 |
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10.1007/BF00157319 doi (DE-627)OLC2033558258 (DE-He213)BF00157319-p DE-627 ger DE-627 rakwb eng 530 VZ 16,12 ssgn Györi, L. verfasserin aut Imaging properties of a photoheliograph with a Lyot plane shutter 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © D. Reidel Publishing Company 1985 Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. Response Function Frequency Response Constant Velocity Slit Width Frequency Response Function Enthalten in Solar physics Kluwer Academic Publishers, 1967 99(1985), 1-2 vom: Sept., Seite 365-369 (DE-627)129856010 (DE-600)281593-X (DE-576)015160033 0038-0938 nnns volume:99 year:1985 number:1-2 month:09 pages:365-369 https://doi.org/10.1007/BF00157319 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY SSG-OLC-AST SSG-OPC-AST GBV_ILN_11 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_70 GBV_ILN_2002 GBV_ILN_2279 GBV_ILN_2286 GBV_ILN_4012 GBV_ILN_4046 GBV_ILN_4306 AR 99 1985 1-2 09 365-369 |
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Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. © D. Reidel Publishing Company 1985 |
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Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. © D. Reidel Publishing Company 1985 |
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Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. Calculated frequency response functions for a ideal objective and various slit widths are presented. © D. Reidel Publishing Company 1985 |
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Reidel Publishing Company 1985</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In a photoheliograph the shutter (a slit moving with constant velocity) may be placed in the Lyot plane, where the image of the objective is formed by the enlarging lens. This degrades the frequency response function of the objective, depending on the width of the slit. 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