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Bhupal Nobles' University, Udaipur Convocation | भूपाल नोबल्स विश्वविद्यालय, उदयपुर दीक्षांत समारोह

भूपाल नोबल्स विश्वविद्यालय दीक्षांत समारोह महाराणा प्रताप स्टेशन रोड, सेवाश्रम सर्कल, उदयपुर। भूपाल नोबल्स विश्वविद्यालय उदयपुर द्वारा वर्ष 2018 से 2024 तक की स्नातक एवं स्नातकोत्तर परीक्षा में उत्तीर्ण एवं विद्यावाचस्पति (Ph.D.) उपाधिधारियों के लिए दीक्षान्त समारोह 27 मार्च 2025 गुरूवार को प्रातः 10:30 बजे आयोजित करने का निश्चित हुआ है। दीक्षान्त समारोह में 2020 से 2025 तक की विद्यावाचस्पति की उपाधियों तथा स्नातक एवं स्नातकोत्तर परीक्षाओं में वर्ष 2024 तक प्रथम स्थान प्राप्त करने वाले छात्रों को उपाधि एवं स्वर्ण पदक प्रदान किए जायेंगे। अतः जो उपाधिधारी उक्त समारोह में उपाधि प्राप्त करने के इच्छुक हों, वे समारोह में उपस्थित होने की लिखित सूचना के साथ स्नातक एवं स्नातकोत्तर प्रथम वरीयता प्राप्त छात्रों हेतु, पंजीकरण शुल्क ₹500 व उपाधि शुल्क ₹5000 (कुल ₹5500) एवं विद्यावाचस्पति (Ph.D.), शोधार्थी पंजीकरण शुल्क ₹500 व उपाधि शुल्क ₹5000 (कुल ₹5500) नकद अथवा डिमाण्ड ड्राफ्ट भूपाल नोबल्स विश्वविद्यालय, उदयपुर के नाम बनाकर कुलसचिव, भूपाल नोबल्स विश्वविद्यालय, उदयपुर को दिनांक 17.03.2025 तक ...
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Thick lens and its cardinal points | Optics | General theory of image formation

Thick lens and its cardinal points

Thick lens

  • The combination of two spherical surfaces, is known as thick lens, if the distance between their poles can not be neglected in comparison to their radii.
  • It can be treated as the combination of thin lenses.
  • The thickness of these lenses are comparable to their focal lengths.

Cardinal points of thick lens

  • Let µ = refractive index of material of lens
  • t = thickness of lens
  • R1 and R2 = Radii of curvature of first and second curved surface of the given thick lens.
  • F1 and F2 = First and second focal points respectively.
  • H1 and H2 = First and second principal points respectively.
  • f1 and f2 = First and second focal length of thick lens respectively.

Cardinal points of thick lens

Equivalent focal length

  • If there is same medium on either side of thick lens
  • H1F1 = f1 = - f , and H2F2 = f2 = f

Refraction from surface PP1


Refraction from surface QP2

  • This time I works as an object and forms final image is obtained at F2



  • For thin lens t → 0, and f → f0

Power of thick lens


Position of second focal point (P2F2 = β2)

  • The distance of second focal point will be measured from pole of second refracting surface.

Position of second principal point (P2H2 = α2)

 
  • The distance of second principal point will be measured from pole of second refracting surface

  • Above result is obtained using sign convention.

Position of first focal point (P2F1 = β1)

 
  • For obtaining it we consider that the ray is incident on lens system from right i.e., O՛Q, this time image will be formed on F1. So in β2, R1 is replaced by -R2 and f is replaced by -f.


Position of first principal point (P1H1 = α1)

 
  • For it we use R1 → –R2 and  f → – f in second principal point α2 

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