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"Spherical triangle" redirects here. For triangles in the Euclidean plane with circular-arc sides, see Reuleaux triangle.

**Spherical trigonometry** is the branch of spherical geometry that deals with the relationships between trigonometric functions of the sides and angles of the spherical polygons (especially **spherical triangles**) defined by a number of intersecting great circles on the sphere. Spherical trigonometry is of great importance for calculations in astronomy, geodesy and navigation.

The origins of spherical trigonometry in Greek mathematics and the major developments in Islamic mathematics are discussed fully in History of trigonometry and Mathematics in medieval Islam. The subject came to fruition in Early Modern times with important developments by John Napier, Delambre and others, and attained an essentially complete form by the end of the nineteenth century with the publication of Todhunter's textbook *Spherical trigonometry for the use of colleges and Schools*. This book is now readily available on the web.^{[1]}
The only significant developments since then have been the application of vector methods for the derivation of the theorems and the use of computers to carry through lengthy calculations.

A *spherical polygon* is a polygon on the surface of the sphere defined by a number of great-circle arcs, which are the intersection of the surface with planes through the centre of the sphere. Such polygons may have any number of sides. Two planes define a lune, also called a "digon" or bi-angle, the two-sided analogue of the triangle: a familiar example is the curved surface of a segment of an orange.
Three planes define a spherical triangle, the principal subject of this article. Four planes define a spherical quadrilateral: such a figure, and higher sided polygons, can always be treated as a number of spherical triangles.

From this point the article will be restricted to spherical triangles, denoted simply as *triangles*.

- Both vertices and angles at the vertices are denoted by the same upper case letters
*A, B*and*C*. - The angles
*A*,*B*,*C*of the triangle are equal to the angles between the planes that intersect the surface of the sphere or, equivalently, the angles between the tangent vectors of the great circle arcs where they meet at the vertices. Angles are in radians. The angles of*proper*spherical triangles are (by convention) less than π so that*π*<*A*+*B*+*C*< 3π. (Todhunter,^{[1]}Art.22,32). - The sides are denoted by lower-case letters
*a*,*b*,*c*. On the unit sphere their lengths are numerically equal to the radian measure of the angles that the great circle arcs subtend at the centre. The sides of*proper*spherical triangles are (by convention) less than π so that 0 <*a*+*b*+*c*< 3π. (Todhunter,^{[1]}Art.22,32). - The radius of the sphere is taken as unity. For specific practical problems on a sphere of radius
*R*the measured lengths of the sides must be divided by*R*before using the identities given below. Likewise, after a calculation on the unit sphere the sides*a*,*b*,*c*must be multiplied by*R*.

The polar triangle associated with a triangle ABC is defined as follows. Consider the great circle that contains the side BC. This great circle is defined by the intersection of a diametral plane with the surface. Draw the normal to that plane at the centre: it intersects the surface at two points and the point that is on the same side of the plane as A is (conventionally) termed the pole of A and it is denoted by A'. The points B' and C' are defined similarly.

The triangle A'B'C' is the polar triangle corresponding to triangle ABC. A very important theorem (Todhunter,^{[1]} Art.27) proves that the angles and sides of the polar triangle are
given by

- ${\begin{alignedat}{3}A'&=\pi -a,&\qquad B'&=\pi -b,&\qquad C'&=\pi -c,\\a'&=\pi -A,&b'&=\pi -B,&c'&=\pi -C.\end{alignedat}}$

Therefore, if any identity is proved for the triangle ABC then we can immediately derive a second identity by applying the first identity to the polar triangle by making the above substitutions. This is how the supplemental cosine equations are derived from the cosine equations. Similarly, the identities for a quadrantal triangle can be derived from those for a right-angled triangle. The polar triangle of a polar triangle is the original triangle.

Main article: Spherical law of cosines

The cosine rule is the fundamental identity of spherical trigonometry: all other identities, including the sine rule, may be derived from the cosine rule.

- $\cos a=\cos b\cos c+\sin b\sin c\cos A,\!$
- $\cos b=\cos c\cos a+\sin c\sin a\cos B,\!$
- $\cos c=\cos a\cos b+\sin a\sin b\cos C,\!$

These identities approximate the cosine rule of plane trigonometry if the sides are much smaller than the radius of the sphere. (On the unit sphere, if *a, b, c << 1*: set $\sin a\approx a$ and $\cos a\approx 1-a^{2}/2$ etc.; see Spherical law of cosines.)

Main article: Spherical law of sines

The spherical law of sines is given by the formula

- ${\frac {\sin A}{\sin a}}={\frac {\sin B}{\sin b}}={\frac {\sin C}{\sin c}}.$

These identities approximate the sine rule of plane trigonometry when the sides are much smaller than the radius of the sphere.

Main article: Spherical law of cosines

The spherical cosine formulae were originally proved by elementary geometry and the planar cosine rule (Todhunter,^{[1]} Art.37). He also gives a derivation using simple coordinate geometry and the planar cosine rule (Art.60). The approach outlined here uses simpler vector methods. (These methods are also discussed at Spherical law of cosines.)

Consider three unit vectors **OA**, **OB** and **OC** drawn from the origin to the vertices of the triangle (on the unit sphere). The arc BC subtends an angle of magnitude *a* at the centre and therefore **OB·OC**=cos *a*. Introduce a Cartesian basis with **OA** along the *z*-axis and **OB** in the *xz*-plane making an angle *c* with the *z*-axis. The vector **OC** projects to ON in the *xy*-plane and the angle between ON and the *x*-axis is *A*. Therefore, the three vectors have components:

**OA**$(0,\,0,\,1)$**OB**$(\sin c,\,0,\,\cos c)$**OC**$(\sin b\cos A,\,\sin b\sin A,\,\cos b)$.

The scalar product **OB·OC** in terms of the components is

**OB·OC**= $\sin c\,\sin b\,\cos A+\cos c\,\cos b$.

Equating the two expressions for the scalar product gives

- $\cos a=\cos b\,\cos c+\sin b\,\sin c\,\cos A.$

This equation can be re-arranged to give explicit expressions for the angle in terms of the sides:

- $\cos A={\frac {\cos a\,-\,\cos b\,\cos c}{\sin b\,\sin c}}.$

The other cosine rules are obtained by cyclic permutations.

Main article: Spherical law of sines

This derivation is given in Todhunter,^{[1]} (Art.40). From the identity $\sin ^{2}A=1-\cos ^{2}A$ and the explicit expression for $\cos A$ given immediately above

- ${\begin{aligned}\sin ^{2}\!A&=1-\left({\frac {\cos a-\cos b\,\cos c}{\sin b\,\sin c}}\right)^{2}\\&={\frac {(1-\cos ^{2}\!b)(1-\cos ^{2}\!c)-(\cos a-\cos b\,\cos c)^{2}}{\sin ^{2}\!b\,\sin ^{2}\!c}}\\{\frac {\sin A}{\sin a}}&={\frac {[1-\cos ^{2}\!a-\cos ^{2}\!b-\cos ^{2}\!c+2\cos a\cos b\cos c]^{1/2}}{\sin a\sin b\sin c}}.\end{aligned}}$

Since the right hand side is invariant under a cyclic permutation of $a,\;b,\;c$ the spherical sine rule follows immediately.

There are many ways of deriving the fundamental cosine and sine rules and the other rules developed in the following sections. For example Todhunter^{[1]} gives two proofs of the cosine rule (Articles 37 and 60) and two proofs of the sine rule (Articles 40 and 42). The page on Spherical law of cosines gives four different proofs of the cosine rule. Text books on geodesy (such as Clarke^{[2]}) and spherical astronomy (such as Smart^{[3]}) give different proofs and the online resources of MathWorld provide yet more.^{[4]} There are even more exotic derivations, such as that of Banerjee^{[5]} who derives the formulae using the linear algebra of projection matrices and also quotes methods in differential geometry and the group theory of rotations.

The derivation of the cosine rule presented above has the merits of simplicity and directness and the derivation of the sine rule emphasises the fact that no separate proof is required other than the cosine rule. However, the above geometry may be used to give an independent proof of the sine rule. The scalar triple product, **OA·(OB×OC)** evaluates to $\sin b\sin c\sin A$ in the basis shown. Similarly, in a basis oriented with the *z*-axis along **OB**, the triple product **OB·(OC×OA)** evaluates to $\sin c\sin a\sin B$. Therefore the invariance of the triple product under cyclic permutations gives $\sin b\sin A=\sin a\sin B$ which is the first of the sine rules.

Applying the cosine rules to the polar triangle gives (Todhunter,^{[1]} Art.47), *i.e.* replacing *A* by π–*a*, *a* by π–*A* etc.,

- ${\begin{aligned}\cos A&=-\cos B\,\cos C+\sin B\,\sin C\,\cos a,\\\cos B&=-\cos C\,\cos A+\sin C\,\sin A\,\cos b,\\\cos C&=-\cos A\,\cos B+\sin A\,\sin B\,\cos c.\end{aligned}}$

The six parts of a triangle may be written in cyclic order as (*aCbAcB*). The cotangent, or four-part, formulae relate two sides and two angles forming four *consecutive* parts around the triangle, for example (*aCbA*) or (*BaCb*). In such a set there are inner and outer parts: for example in the set (*BaCb*) the inner angle is *C*, the inner side is *a*, the outer angle is *B*, the outer side is *b*. The cotangent rule may be written as (Todhunter,^{[1]} Art.44)

- $\cos({\text{inner side}})\cos({\text{inner angle}})=\cot({\text{outer side}})\sin({\text{inner side}})\ -\ \cot({\text{outer angle}})\sin({\text{inner angle}}),$

and the six possible equations are (with the relevant set shown at right):

- ${\begin{array}{lll}{\text{(CT1)}}\quad &\cos b\,\cos C=\cot a\,\sin b-\cot A\,\sin C,\qquad &(aCbA)\\[0ex]{\text{(CT2)}}&\cos b\,\cos A=\cot c\,\sin b-\cot C\,\sin A,&(CbAc)\\[0ex]{\text{(CT3)}}&\cos c\,\cos A=\cot b\,\sin c-\cot B\,\sin A,&(bAcB)\\[0ex]{\text{(CT4)}}&\cos c\,\cos B=\cot a\,\sin c-\cot A\,\sin B,&(AcBa)\\[0ex]{\text{(CT5)}}&\cos a\,\cos B=\cot c\,\sin a-\cot C\,\sin B,&(cBaC)\\[0ex]{\text{(CT6)}}&\cos a\,\cos C=\cot b\,\sin a-\cot B\,\sin C,&(BaCb).\end{array}}$

To prove the first formula start from the first cosine rule and on the right-hand side substitute for $\cos c$ from the third cosine rule:

- ${\begin{aligned}\cos a&=\cos b\cos c+\sin b\sin c\cos A\\&=\cos b\ (\cos a\cos b+\sin a\sin b\cos C)+\sin b\sin C\sin a\cot A\\\cos a\sin ^{2}b&=\cos b\sin a\sin b\cos C+\sin b\sin C\sin a\cot A.\end{aligned}}$

The result follows on dividing by $\sin a\sin b$. Similar techniques with the other two cosine rules give CT3 and CT5. The other three equations follow by applying rules 1, 3 and 5 to the polar triangle.

With $2s=(a+b+c)$ and $2S=(A+B+C)$,

- ${\begin{aligned}&\sin {\textstyle {\frac {1}{2}}}A=\left[{\frac {\sin(s{-}b)\sin(s{-}c)}{\sin b\sin c}}\right]^{1/2}&\qquad &\sin {\textstyle {\frac {1}{2}}}a=\left[{\frac {-\cos S\cos(S{-}A)}{\sin B\sin C}}\right]^{1/2}\\[2ex]&\cos {\textstyle {\frac {1}{2}}}A=\left[{\frac {\sin s\sin(s{-}a)}{\sin b\sin c}}\right]^{1/2}&\qquad &\cos {\textstyle {\frac {1}{2}}}a=\left[{\frac {\cos(S{-}B)\cos(S{-}C)}{\sin B\sin C}}\right]^{1/2}\\[2ex]&\tan {\textstyle {\frac {1}{2}}}A=\left[{\frac {\sin(s{-}b)\sin(s{-}c)}{\sin s\sin(s{-}a)}}\right]^{1/2}&\qquad &\tan {\textstyle {\frac {1}{2}}}a=\left[{\frac {-\cos S\cos(S{-}A)}{\cos(S{-}B)\cos(S{-}C)}}\right]^{1/2}\end{aligned}}$

Another twelve identities follow by cyclic permutation.

The proof (Todhunter,^{[1]} Art.49) of the first formula starts from the identity 2sin^{2}(*A*/2) = 1–cos*A*, using the cosine rule to express *A* in terms of the sides and replacing the sum of two cosines by a product. (See sum-to-product identities.) The second formula starts from the identity 2cos^{2}(*A*/2) = 1+cos*A*, the third is a quotient and the remainder follow by applying the results to the polar triangle.

- ${\begin{aligned}&\\{\frac {\sin {\textstyle {\frac {1}{2}}}(A{+}B)}{\cos {\textstyle {\frac {1}{2}}}C}}={\frac {\cos {\textstyle {\frac {1}{2}}}(a{-}b)}{\cos {\textstyle {\frac {1}{2}}}c}}&\qquad \qquad &{\frac {\sin {\textstyle {\frac {1}{2}}}(A{-}B)}{\cos {\textstyle {\frac {1}{2}}}C}}={\frac {\sin {\textstyle {\frac {1}{2}}}(a{-}b)}{\sin {\textstyle {\frac {1}{2}}}c}}\\[2ex]{\frac {\cos {\textstyle {\frac {1}{2}}}(A{+}B)}{\sin {\textstyle {\frac {1}{2}}}C}}={\frac {\cos {\textstyle {\frac {1}{2}}}(a{+}b)}{\cos {\textstyle {\frac {1}{2}}}c}}&\qquad &{\frac {\cos {\textstyle {\frac {1}{2}}}(A{-}B)}{\sin {\textstyle {\frac {1}{2}}}C}}={\frac {\sin {\textstyle {\frac {1}{2}}}(a{+}b)}{\sin {\textstyle {\frac {1}{2}}}c}}\end{aligned}}$

Another eight identities follow by cyclic permutation.

Proved by expanding the numerators and using the half angle formulae. (Todhunter,^{[1]} Art.54 and Delambre^{[6]})

- ${\begin{aligned}&&\\[-2ex]\displaystyle {\tan {\textstyle {\frac {1}{2}}}(A{+}B)}={\frac {\cos {\textstyle {\frac {1}{2}}}(a{-}b)}{\cos {\textstyle {\frac {1}{2}}}(a{+}b)}}\cot {\textstyle {\frac {1}{2}}C}&\qquad &{\tan {\textstyle {\frac {1}{2}}}(a{+}b)}={\frac {\cos {\textstyle {\frac {1}{2}}}(A{-}B)}{\cos {\textstyle {\frac {1}{2}}}(A{+}B)}}\tan {\textstyle {\frac {1}{2}}c}\\[2ex]{\tan {\textstyle {\frac {1}{2}}}(A{-}B)}={\frac {\sin {\textstyle {\frac {1}{2}}}(a{-}b)}{\sin {\textstyle {\frac {1}{2}}}(a{+}b)}}\cot {\textstyle {\frac {1}{2}}C}&\qquad &{\tan {\textstyle {\frac {1}{2}}}(a{-}b)}={\frac {\sin {\textstyle {\frac {1}{2}}}(A{-}B)}{\sin {\textstyle {\frac {1}{2}}}(A{+}B)}}\tan {\textstyle {\frac {1}{2}}c}\end{aligned}}$

Another eight identities follow by cyclic permutation.

These identities follow by division of the Delambre formulae. (Todhunter,^{[1]} Art.52)

When one of the angles, say *C*, of a spherical triangle is equal to π/2 the various identities given above are considerably simplified. There are ten identities relating three elements chosen from the set *a, b, c, A, B*.

Napier^{[7]} provided an elegant mnemonic aid for the ten independent equations: the mnemonic is called Napier's circle or Napier's pentagon (when the circle in the above figure, right, is replaced by a pentagon).

First write in a circle the six parts of the triangle (three vertex angles, three arc angles for the sides): for the triangle shown above left this gives *aCbAcB*. Next replace the parts that are not adjacent to C (that is *A, c, B*) by their complements and then delete the angle C from the list. The remaining parts are as shown in the above figure (right). For any choice of three contiguous parts, one (the *middle* part) will be adjacent to two parts and opposite the other two parts. The ten Napier's Rules are given by

- sine of the middle part = the product of the tangents of the adjacent parts
- sine of the middle part = the product of the cosines of the opposite parts

For an example, starting with the sector containing $a$ we have:

- $\sin a=\tan(\pi /2{-}B)\,\tan b=\cos(\pi /2{-}c)\,\cos(\pi /2{-}A)=\cot B\,\tan b=\sin c\,\sin A.$

The full set of rules for the right spherical triangle is (Todhunter,^{[1]} Art.62)

- ${\begin{alignedat}{4}&{\text{(R1)}}&\qquad \cos c&=\cos a\,\cos b,&\qquad \qquad &{\text{(R6)}}&\qquad \tan b&=\cos A\,\tan c,\\&{\text{(R2)}}&\sin a&=\sin A\,\sin c,&&{\text{(R7)}}&\tan a&=\cos B\,\tan c,\\&{\text{(R3)}}&\sin b&=\sin B\,\sin c,&&{\text{(R8)}}&\cos A&=\sin B\,\cos a,\\&{\text{(R4)}}&\tan a&=\tan A\,\sin b,&&{\text{(R9)}}&\cos B&=\sin A\,\cos b,\\&{\text{(R5)}}&\tan b&=\tan B\,\sin a,&&{\text{(R10)}}&\cos c&=\cot A\,\cot B.\end{alignedat}}$

A quadrantal spherical triangle is defined to be a spherical triangle in which one of the sides subtends an angle of *π*/2 radians at the centre of the sphere: on the unit sphere the side has length *π*/2. In the case that the side *c* has length *π*/2 on the unit sphere the equations governing the remaining sides and angles may be obtained by applying the rules for the right spherical triangle of the previous section to the polar triangle *A'B'C' * with sides *a',b',c' * such that *A' *= *π*−*a*, *a' * = *π*−*A* etc. The results are:

- ${\begin{alignedat}{4}&{\text{(Q1)}}&\qquad \cos C&=-\cos A\,\cos B,&\qquad \qquad &{\text{(Q6)}}&\qquad \tan B&=-\cos a\,\tan C,\\&{\text{(Q2)}}&\sin A&=\sin a\,\sin C,&&{\text{(Q7)}}&\tan A&=-\cos b\,\tan C,\\&{\text{(Q3)}}&\sin B&=\sin b\,\sin C,&&{\text{(Q8)}}&\cos a&=\sin b\,\cos A,\\&{\text{(Q4)}}&\tan A&=\tan a\,\sin B,&&{\text{(Q9)}}&\cos b&=\sin a\,\cos B,\\&{\text{(Q5)}}&\tan B&=\tan b\,\sin A,&&{\text{(Q10)}}&\cos C&=-\cot a\,\cot b.\end{alignedat}}$

Substituting the second cosine rule into the first and simplifying gives:

- $\cos a=(\cos a\,\cos c+\sin a\,\sin c\,\cos B)\cos c+\sin b\,\sin c\,\cos A$
- $\cos a\,\sin ^{2}c=\sin a\,\cos c\,\sin c\,\cos B+\sin b\,\sin c\,\cos A$

Cancelling the factor of $\sin c$ gives

- $\cos a\sin c=\sin a\,\cos c\,\cos B+\sin b\,\cos A$

Similar substitutions in the other cosine and supplementary cosine formulae give a large variety of 5-part rules. They are rarely used.

- Main article: Solution of triangles § Solving spherical triangles

The solution of triangles is the principal purpose of spherical trigonometry: given three, four or five elements of the triangle determine the remainder. The case of five given elements is trivial, requiring only a single application of the sine rule. For four given elements there is one non-trivial case, which is discussed below. For three given elements there are six cases: three sides, two sides and an included or opposite angle, two angles and an included or opposite side, or three angles. (The last case has no analogue in planar trigonometry.) No single method solves all cases. The figure below shows the seven non-trivial cases: in each case the given sides are marked with a cross-bar and the given angles with an arc. (The given elements are also listed below the triangle). There is a full discussion of the solution of oblique triangles in Todhunter^{[1]} (ChapterVI).

**Case 1: three sides given.**The cosine rule may be used to give the angles*A*,*B*, and*C*but, to avoid ambiguities, the half angle formulae are preferred.**Case 2: two sides and an included angle given.**The cosine rule gives*a*and then we are back to Case 1.**Case 3: two sides and an opposite angle given.**The sine rule gives*C*and then we have Case 7. There are either one or two solutions.**Case 4: two angles and an included side given.**The four-part cotangent formulae for sets (*cBaC*) and (*BaCb*) give*c*and*b*, then*A*follows from the sine rule.**Case 5: two angles and an opposite side given.**The sine rule gives*b*and then we have Case 7 (rotated). There are either one or two solutions.**Case 6: three angles given.**The supplemental cosine rule may be used to give the sides*a*,*b*, and*c*but, to avoid ambiguities, the half-side formulae are preferred.**Case 7: two angles and two sides given.**Use Napier's analogies for*a*and*A*.

The solution methods listed here are not the only possible choices: many others are possible. In general it is better to choose methods that avoid taking an inverse sine because of the possible ambiguity between an angle and its supplement. The use of half-angle formulae is often advisable because half-angles will be less than π/2 and therefore free from ambiguity. There is a full discussion in Todhunter. The solution of triangles article presents variants on these methods with a slightly different notation.

Another approach is to split the triangle into two right-angled triangles. For example, take the Case 3 example where *b, c, B* are given. Construct the great circle from *A* that is normal to the side *BC* at the point *D*. Use Napier's rules to solve the triangle *ABD*: use *c* and *B* to find the sides *AD*, *BD* and the angle *BAD*. Then use Napier's rules to solve the triangle *ACD*: that is use *AD* and *b* to find the side *DC* and the angles *C* and *DAC*. The angle *A* and side *a* follow by addition.

Not all of the rules obtained are numerically robust in extreme examples, for example when an angle approaches zero or π. Problems and solutions may have to be examined carefully, particularly when writing code to solve an arbitrary triangle.

See also: Solid angle

Consider an *N*-sided spherical polygon and let A_{n} denote the *n*-th interior angle. The area of such a polygon is given by (Todhunter,^{[1]} Art.99)

- ${\text{Area of polygon (on the unit sphere)}}\equiv E_{N}=\left(\sum _{n=1}^{N}A_{n}\right)-(N-2)\pi .$

For the case of triangle this reduces to

- ${\text{Area of triangle (on the unit sphere)}}\equiv E=E_{3}=A+B+C-\pi ,$

where *E* is the amount by which the sum of the angles exceeds π radians. The quantity *E* is called the **spherical excess** of the triangle. This theorem is named after its author, Albert Girard.^{[8]} An earlier proof was derived, but not published, by the English mathematician Thomas Harriot. On a sphere of radius *R* both of the above area expressions are multiplied by *R*^{2}. The definition of the excess is independent of the radius of the sphere.

The converse result may be written as

- $\displaystyle A+B+C=\pi +{\frac {4\pi \times {\text{Area of triangle}}}{\text{Area of the sphere}}}.$

Since the area of a triangle cannot be negative the spherical excess is always positive. Note that it is not necessarily small since the sum of the angles may attain 3π. For example,
an octant of a sphere is a spherical triangle with three right angles, so that the excess is π/2. In practical applications it *is* often small: for example the triangles of geodetic survey typically have a spherical excess much less than 1' of arc. (Rapp^{[9]}
Clarke,^{[10]} Legendre's theorem on spherical triangles).
On the Earth the excess of an equilateral triangle with sides 21.3 km (and area 393 km^{2}) is approximately 1 arc second.

There are many formulae for the excess. For example, Todhunter,^{[1]} (Art.101—103) gives ten examples including that of L'Huilier:

- $\tan {\tfrac {1}{4}}E={\sqrt {\tan {\tfrac {1}{2}}s\,\tan {\tfrac {1}{2}}(s{-}a)\,\tan {\tfrac {1}{2}}(s{-}b)\,\tan {\tfrac {1}{2}}(s{-}c)}}$

where $s=(a+b+c)/2$. Because some triangles are badly characterized by their edges (e.g., if $a=b\approx {\frac {1}{2}}c$), it is often better to use the formula for the excess in terms of two edges and their included angle

- $\tan {\frac {E}{2}}={\frac {\tan {\frac {1}{2}}a\tan {\frac {1}{2}}b\sin C}{1+\tan {\frac {1}{2}}a\tan {\frac {1}{2}}b\cos C}}.$

An example for a spherical quadrangle bounded by a segment of a great circle, two meridians, and the equator is

- $\tan {\frac {E_{4}}{2}}={\frac {\sin {\frac {1}{2}}(\phi _{2}+\phi _{1})}{\cos {\frac {1}{2}}(\phi _{2}-\phi _{1})}}\tan {\frac {\lambda _{2}-\lambda _{1}}{2}}.$

where $\phi ,\lambda$ denote latitude and longitude. This result is obtained from one of Napier's analogies. In the limit where $\phi _{1},\phi _{2},\lambda _{2}-\lambda _{1}$ are all small, this reduces to the familiar trapezoidal area, $E_{4}\approx {\frac {1}{2}}(\phi _{2}+\phi _{1})(\lambda _{2}-\lambda _{1})$.

Angle deficit is defined similarly for hyperbolic geometry.

This article uses material from the Wikipedia article "Spherical trigonometry", which is released under the Creative Commons Attribution-Share-Alike License 3.0. There is a list of all authors in Wikipedia

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