1. notice
  2. English
  3. logic_topic
  4. 1. logic
  5. 2. basic
  6. 3. map
  7. 4. order
  8. 5. combinatorics
  9. calculus
  10. 6. real_numbers
  11. 7. limit_sequence
  12. 8. division_algebra
  13. 9. Euclidean_space
  14. 10. Minkowski_space
  15. 11. polynomial
  16. 12. analytic_Euclidean
  17. 13. analytic_struct_operation
  18. 14. ordinary_differential_equation
  19. 15. convex_hull
  20. 16. volume
  21. 17. integral
  22. 18. divergence
  23. 19. limit_net
  24. 20. topology
  25. 21. compact
  26. 22. connected
  27. 23. topology_struct_operation
  28. 24. exponential
  29. 25. angle
  30. geometry
  31. 26. manifold
  32. 27. metric
  33. 28. metric_connection
  34. 29. geodesic_derivative
  35. 30. curvature_of_metric
  36. 31. Einstein_metric
  37. 32. constant_sectional_curvature
  38. 33. simple_symmetric_space
  39. 34. principal_bundle
  40. 35. group
  41. 36. stereographic_projection
  42. 37. Hopf_bundle
  43. field_theory
  44. 38. point_particle_non_relativity
  45. 39. point_particle_relativity
  46. 40. scalar_field
  47. 41. scalar_field_current
  48. 42. scalar_field_non_relativity
  49. 43. projective_lightcone
  50. 44. spacetime_momentum_spinor_representation
  51. 45. Lorentz_group
  52. 46. spinor_field
  53. 47. spinor_field_current
  54. 48. electromagnetic_field
  55. 49. Laplacian_of_tensor_field
  56. 50. Einstein_metric
  57. 51. interaction
  58. 52. harmonic_oscillator_quantization
  59. 53. spinor_field_misc
  60. 54. reference
  61. ไธญๆ–‡
  62. 55. notice
  63. ้€ป่พ‘
  64. 56. ้€ป่พ‘
  65. 57. ๅŸบ็ก€
  66. 58. ๆ˜ ๅฐ„
  67. 59. ๅบ
  68. 60. ็ป„ๅˆ
  69. ๅพฎ็งฏๅˆ†
  70. 61. ๅฎžๆ•ฐ
  71. 62. ๆ•ฐๅˆ—ๆž้™
  72. 63. ๅฏ้™คไปฃๆ•ฐ
  73. 64. Euclidean ็ฉบ้—ด
  74. 65. Minkowski ็ฉบ้—ด
  75. 66. ๅคš้กนๅผ
  76. 67. ่งฃๆž (Euclidean)
  77. 68. ่งฃๆž struct ็š„ๆ“ไฝœ
  78. 69. ๅธธๅพฎๅˆ†ๆ–น็จ‹
  79. 70. convex_hull
  80. 71. ไฝ“็งฏ
  81. 72. ็งฏๅˆ†
  82. 73. ๆ•ฃๅบฆ
  83. 74. ็ฝ‘ๆž้™
  84. 75. ๆ‹“ๆ‰‘
  85. 76. ็ดง่‡ด
  86. 77. ่ฟž้€š
  87. 78. ๆ‹“ๆ‰‘ struct ็š„ๆ“ไฝœ
  88. 79. ๆŒ‡ๆ•ฐๅ‡ฝๆ•ฐ
  89. 80. ่ง’ๅบฆ
  90. ๅ‡ ไฝ•
  91. 81. ๆตๅฝข
  92. 82. ๅบฆ่ง„
  93. 83. ๅบฆ่ง„็š„่”็ปœ
  94. 84. Levi_Civita ๅฏผๆ•ฐ
  95. 85. ๅบฆ่ง„็š„ๆ›ฒ็އ
  96. 86. Einstein ๅบฆ่ง„
  97. 87. ๅธธๆˆช้ขๆ›ฒ็އ
  98. 88. simple_symmetric_space
  99. 89. ไธปไธ›
  100. 90. ็พค
  101. 91. ็ƒๆžๆŠ•ๅฝฑ
  102. 92. Hopf ไธ›
  103. ๅœบ่ฎบ
  104. 93. ้ž็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  105. 94. ็›ธๅฏน่ฎบ็‚น็ฒ’ๅญ
  106. 95. ็บฏ้‡ๅœบ
  107. 96. ็บฏ้‡ๅœบ็š„ๅฎˆๆ’ๆต
  108. 97. ้ž็›ธๅฏน่ฎบ็บฏ้‡ๅœบ
  109. 98. ๅ…‰้”ฅๅฐ„ๅฝฑ
  110. 99. ๆ—ถ็ฉบๅŠจ้‡็š„่‡ชๆ—‹่กจ็คบ
  111. 100. Lorentz ็พค
  112. 101. ๆ—‹้‡ๅœบ
  113. 102. ๆ—‹้‡ๅœบ็š„ๅฎˆๆ’ๆต
  114. 103. ็”ต็ฃๅœบ
  115. 104. ๅผ ้‡ๅœบ็š„ Laplacian
  116. 105. Einstein ๅบฆ่ง„
  117. 106. ็›ธไบ’ไฝœ็”จ
  118. 107. ่ฐๆŒฏๅญ้‡ๅญๅŒ–
  119. 108. ๆ—‹้‡ๅœบๆ‚้กน
  120. 109. ๅ‚่€ƒ

note-math

The problem of defining the derivative of a vector field in the direction

For a vector field near , in the direction, try to calculate the derivative in coordinates

However, the difference operation is not linearly compatible with coordinate changes of general diffeomorphisms.

But in a metric-manifold, there are special coordinates โ€” geodesic coordinates. The transformation method for different geodesic coordinates at is , which is linear.

[geodesic_derivative] Geodesic derivative alias [Levi_Civita_derivative] Levi-Civita derivative :=

In geodesic coordinates at point , the derivative at point ,

It is also possible to take the derivative of a tensor field . According to the scalar multiplication associated with the tensor structure, calculations can be performed using the product-rule Example

Prop . Proof In geodesic coordinates

Prop or

Prop The covariant derivative is compatible with the metric-dual e.g. since

Other coordinates may be needed to compute geodesic coordinates, and thus other coordinates may also be needed to express the geodesic derivative.

[geodesic_derivative_in_general_coordinate]

Compute geodesic coordinates using general coordinates , then in coordinates , the geodesic derivative is

Using connection transformation

==>

Use . Substitute into the calculation of

The tangent space linearly transforms to by , but keeps in coordinate , but keep in coordinate

Or written as, in general coordinates, geodesic derivative

For coordinate-frame

Is there a more intuitive explanation, rather than directly using the transformation of connection?

If we only consider linear compatibility, then there are many linear connections, and the one that coincides with the geodesic-derivative is the metric-connection

[geodesic_derivative_of_co_vector] Prop For co-vector field

Proof

Question Similar to the case of vector fields. Use the transformation and the product-rule

For co-vector coordinate-frame

[parallel_transport_metric_connection]

Parallel transport as โ€œzero rate of change along the curveโ€ or where

is an ODE

According to calculation (?), covariant derivative can be recovered from parallel transport + difference quotient

[orthonormal_frame]

Parallel transport of metric-connection preserves the metric

Can be used to construct orthonormal frames

It can be proven that a manifold metric uniquely corresponds to an principal-bundle structure on the manifold

But are there more specific and operational calculation results? Regarding calculating orthonormal frames using parallel transport in geodesic coordinates

A canonical orthonormal frame may be used for simplified some of calculations of spinors on curved manifolds, e.g. Pauli-matrix