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22 Jacobian Elliptic FunctionsProperties

§22.13 Derivatives and Differential Equations

Contents
  1. §22.13(i) Derivatives
  2. §22.13(ii) First-Order Differential Equations
  3. §22.13(iii) Second-Order Differential Equations

§22.13(i) Derivatives

Table 22.13.1: Derivatives of Jacobian elliptic functions with respect to variable.
ddz⁡(sn⁡z)= cn⁡z⁢dn⁡z ddz⁡(dc⁡z) = k′2⁢sc⁡z⁢nc⁡z
ddz⁡(cn⁡z)= −sn⁡z⁢dn⁡z ddz⁡(nc⁡z) = sc⁡z⁢dc⁡z
ddz⁡(dn⁡z)= −k2⁢sn⁡z⁢cn⁡z ddz⁡(sc⁡z) = dc⁡z⁢nc⁡z
ddz⁡(cd⁡z)= −k′2⁢sd⁡z⁢nd⁡z ddz⁡(ns⁡z) = −ds⁡z⁢cs⁡z
ddz⁡(sd⁡z)= cd⁡z⁢nd⁡z ddz⁡(ds⁡z) = −cs⁡z⁢ns⁡z
ddz⁡(nd⁡z)= k2⁢sd⁡z⁢cd⁡z ddz⁡(cs⁡z) = −ns⁡z⁢ds⁡z

Note that each derivative in Table 22.13.1 is a constant multiple of the product of the corresponding copolar functions. (The modulus k is suppressed throughout the table.)

For alternative, and symmetric, formulations of these results see Carlson (2004, 2006a).

§22.13(ii) First-Order Differential Equations

22.13.1 (ddz⁡sn⁡(z,k))2 =(1−sn2⁡(z,k))⁢(1−k2⁢sn2⁡(z,k)),
22.13.2 (ddz⁡cn⁡(z,k))2 =(1−cn2⁡(z,k))⁢(k′2+k2⁢cn2⁡(z,k)),
22.13.3 (ddz⁡dn⁡(z,k))2 =(1−dn2⁡(z,k))⁢(dn2⁡(z,k)−k′2).
22.13.4 (ddz⁡cd⁡(z,k))2 =(1−cd2⁡(z,k))⁢(1−k2⁢cd2⁡(z,k)),
22.13.5 (ddz⁡sd⁡(z,k))2 =(1−k′2⁢sd2⁡(z,k))⁢(1+k2⁢sd2⁡(z,k)),
22.13.6 (ddz⁡nd⁡(z,k))2 =(nd2⁡(z,k)−1)⁢(1−k′2⁢nd2⁡(z,k)),
22.13.7 (ddz⁡dc⁡(z,k))2 =(dc2⁡(z,k)−1)⁢(dc2⁡(z,k)−k2),
22.13.8 (ddz⁡nc⁡(z,k))2 =(k2+k′2⁢nc2⁡(z,k))⁢(nc2⁡(z,k)−1),
22.13.9 (ddz⁡sc⁡(z,k))2 =(1+sc2⁡(z,k))⁢(1+k′2⁢sc2⁡(z,k)),
22.13.10 (ddz⁡ns⁡(z,k))2 =(ns2⁡(z,k)−k2)⁢(ns2⁡(z,k)−1),
22.13.11 (ddz⁡ds⁡(z,k))2 =(ds2⁡(z,k)−k′2)⁢(k2+ds2⁡(z,k)),
22.13.12 (ddz⁡cs⁡(z,k))2 =(1+cs2⁡(z,k))⁢(k′2+cs2⁡(z,k)).

For alternative, and symmetric, formulations of these results see Carlson (2006a).

§22.13(iii) Second-Order Differential Equations

22.13.13 d2dz2⁡sn⁡(z,k) =−(1+k2)⁢sn⁡(z,k)+2⁢k2⁢sn3⁡(z,k),
22.13.14 d2dz2⁡cn⁡(z,k) =−(k′2−k2)⁢cn⁡(z,k)−2⁢k2⁢cn3⁡(z,k),
22.13.15 d2dz2⁡dn⁡(z,k) =(1+k′2)⁢dn⁡(z,k)−2⁢dn3⁡(z,k).
22.13.16 d2dz2⁡cd⁡(z,k) =−(1+k2)⁢cd⁡(z,k)+2⁢k2⁢cd3⁡(z,k),
22.13.17 d2dz2⁡sd⁡(z,k) =(k2−k′2)⁢sd⁡(z,k)−2⁢k2⁢k′2⁢sd3⁡(z,k),
22.13.18 d2dz2⁡nd⁡(z,k) =(1+k′2)⁢nd⁡(z,k)−2⁢k′2⁢nd3⁡(z,k),
22.13.19 d2dz2⁡dc⁡(z,k) =−(1+k2)⁢dc⁡(z,k)+2⁢dc3⁡(z,k),
22.13.20 d2dz2⁡nc⁡(z,k) =(k2−k′2)⁢nc⁡(z,k)+2⁢k′2⁢nc3⁡(z,k),
22.13.21 d2dz2⁡sc⁡(z,k) =(1+k′2)⁢sc⁡(z,k)+2⁢k′2⁢sc3⁡(z,k),
22.13.22 d2dz2⁡ns⁡(z,k) =−(1+k2)⁢ns⁡(z,k)+2⁢ns3⁡(z,k),
22.13.23 d2dz2⁡ds⁡(z,k) =(k2−k′2)⁢ds⁡(z,k)+2⁢ds3⁡(z,k),
22.13.24 d2dz2⁡cs⁡(z,k) =(1+k′2)⁢cs⁡(z,k)+2⁢cs3⁡(z,k).

For alternative, and symmetric, formulations of these results see Carlson (2006a).