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11: 16.14 Partial Differential Equations
x ( 1 - x ) 2 F 1 x 2 + y ( 1 - x ) 2 F 1 x y + ( γ - ( α + β + 1 ) x ) F 1 x - β y F 1 y - α β F 1 = 0 ,
y ( 1 - y ) 2 F 1 y 2 + x ( 1 - y ) 2 F 1 x y + ( γ - ( α + β + 1 ) y ) F 1 y - β x F 1 x - α β F 1 = 0 ,
x ( 1 - x ) 2 F 2 x 2 - x y 2 F 2 x y + ( γ - ( α + β + 1 ) x ) F 2 x - β y F 2 y - α β F 2 = 0 ,
x ( 1 - x ) 2 F 4 x 2 - 2 x y 2 F 4 x y - y 2 2 F 4 y 2 + ( γ - ( α + β + 1 ) x ) F 4 x - ( α + β + 1 ) y F 4 y - α β F 4 = 0 ,
y ( 1 - y ) 2 F 4 y 2 - 2 x y 2 F 4 x y - x 2 2 F 4 x 2 + ( γ - ( α + β + 1 ) y ) F 4 y - ( α + β + 1 ) x F 4 x - α β F 4 = 0 .
12: 10.15 Derivatives with Respect to Order
§10.15 Derivatives with Respect to Order
10.15.2 Y ν ( z ) ν = cot ( ν π ) ( J ν ( z ) ν - π Y ν ( z ) ) - csc ( ν π ) J - ν ( z ) ν - π J ν ( z ) .
For J ν ( z ) / ν at ν = - n combine (10.2.4) and (10.15.3). …
10.15.5 J ν ( z ) ν | ν = 0 = π 2 Y 0 ( z ) , Y ν ( z ) ν | ν = 0 = - π 2 J 0 ( z ) .
13: 19.4 Derivatives and Differential Equations
§19.4 Derivatives and Differential Equations
§19.4(i) Derivatives
19.4.3 d 2 E ( k ) d k 2 = - 1 k d K ( k ) d k = k 2 K ( k ) - E ( k ) k 2 k 2 ,
Let D k = / k . …
14: 10.73 Physical Applications
10.73.1 2 V = 1 r r ( r V r ) + 1 r 2 2 V ϕ 2 + 2 V z 2 = 0 ,
10.73.2 2 ψ = 1 c 2 2 ψ t 2 ,
10.73.3 4 W + λ 2 2 W t 2 = 0 .
10.73.4 ( 2 + k 2 ) f = 1 ρ 2 ρ ( ρ 2 f ρ ) + 1 ρ 2 sin θ θ ( sin θ f θ ) + 1 ρ 2 sin 2 θ 2 f ϕ 2 + k 2 f .
15: 1.13 Differential Equations
A solution becomes unique, for example, when w and d w / d z are prescribed at a point in D . … Then at each z D , w , w / z and 2 w / z 2 are analytic functions of u . …
Elimination of First Derivative by Change of Dependent Variable
Elimination of First Derivative by Change of Independent Variable
Cayley’s Identity
16: 30.12 Generalized and Coulomb Spheroidal Functions
30.12.1 d d z ( ( 1 - z 2 ) d w d z ) + ( λ + α z + γ 2 ( 1 - z 2 ) - μ 2 1 - z 2 ) w = 0 ,
30.12.2 d d z ( ( 1 - z 2 ) d w d z ) + ( λ + γ 2 ( 1 - z 2 ) - α ( α + 1 ) z 2 - μ 2 1 - z 2 ) w = 0 ,
17: 14.29 Generalizations
14.29.1 ( 1 - z 2 ) d 2 w d z 2 - 2 z d w d z + ( ν ( ν + 1 ) - μ 1 2 2 ( 1 - z ) - μ 2 2 2 ( 1 + z ) ) w = 0
18: 31.12 Confluent Forms of Heun’s Equation
31.12.1 d 2 w d z 2 + ( γ z + δ z - 1 + ϵ ) d w d z + α z - q z ( z - 1 ) w = 0 .
31.12.2 d 2 w d z 2 + ( δ z 2 + γ z + 1 ) d w d z + α z - q z 2 w = 0 .
31.12.3 d 2 w d z 2 - ( γ z + δ + z ) d w d z + α z - q z w = 0 .
31.12.4 d 2 w d z 2 + ( γ + z ) z d w d z + ( α z - q ) w = 0 .
19: 28.32 Mathematical Applications
28.32.2 2 V x 2 + 2 V y 2 + k 2 V = 0
28.32.3 2 V ξ 2 + 2 V η 2 + 1 2 c 2 k 2 ( cosh ( 2 ξ ) - cos ( 2 η ) ) V = 0 .
28.32.4 2 K z 2 - 2 K ζ 2 = 2 q ( cos ( 2 z ) - cos ( 2 ζ ) ) K .
28.32.5 K ( z , ζ ) d u ( ζ ) d ζ - u ( ζ ) K ( z , ζ ) ζ
20: 30.13 Wave Equation in Prolate Spheroidal Coordinates
30.13.3 h ξ 2 = ( x ξ ) 2 + ( y ξ ) 2 + ( z ξ ) 2 = c 2 ( ξ 2 - η 2 ) ξ 2 - 1 ,
30.13.4 h η 2 = ( x η ) 2 + ( y η ) 2 + ( z η ) 2 = c 2 ( ξ 2 - η 2 ) 1 - η 2 ,
30.13.6 2 = 1 h ξ h η h ϕ ( ξ ( h η h ϕ h ξ ξ ) + η ( h ξ h ϕ h η η ) + ϕ ( h ξ h η h ϕ ϕ ) ) = 1 c 2 ( ξ 2 - η 2 ) ( ξ ( ( ξ 2 - 1 ) ξ ) + η ( ( 1 - η 2 ) η ) + ξ 2 - η 2 ( ξ 2 - 1 ) ( 1 - η 2 ) 2 ϕ 2 ) .
30.13.11 d 2 w 3 d ϕ 2 + μ 2 w 3 = 0 ,