28.9 Zeros28.11 Expansions in Series of Mathieu Functions

§28.10 Integral Equations

Contents

§28.10(i) Equations with Elementary Kernels

With the notation of §28.4 for Fourier coefficients,

28.10.4 \frac{2}{\pi}\int _{{0}}^{{\ifrac{\pi}{2}}}\mathop{\cos\/}\nolimits z\mathop{\cos\/}\nolimits t\mathop{\cosh\/}\nolimits\!\left(2h\mathop{\sin\/}\nolimits z\mathop{\sin\/}\nolimits t\right)\mathop{\mathrm{ce}_{{2n+1}}\/}\nolimits\!\left(t,h^{2}\right)dt=\frac{A_{1}^{{2n+1}}(h^{2})}{2\mathop{\mathrm{ce}_{{2n+1}}\/}\nolimits\!\left(0,h^{2}\right)}\mathop{\mathrm{ce}_{{2n+1}}\/}\nolimits\!\left(z,h^{2}\right),
28.10.5 \frac{2}{\pi}\int _{{0}}^{{\ifrac{\pi}{2}}}\mathop{\sinh\/}\nolimits\!\left(2h\mathop{\sin\/}\nolimits z\mathop{\sin\/}\nolimits t\right)\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits\!\left(t,h^{2}\right)dt=\frac{hB_{1}^{{2n+1}}(h^{2})}{{\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits^{{\prime}}}\!\left(0,h^{2}\right)}\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits\!\left(z,h^{2}\right),
28.10.6 \frac{2}{\pi}\int _{{0}}^{{\ifrac{\pi}{2}}}\mathop{\sin\/}\nolimits z\mathop{\sin\/}\nolimits t\mathop{\cos\/}\nolimits\!\left(2h\mathop{\cos\/}\nolimits z\mathop{\cos\/}\nolimits t\right)\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits\!\left(t,h^{2}\right)dt=\frac{B_{1}^{{2n+1}}(h^{2})}{2\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits\!\left(\frac{1}{2}\pi,h^{2}\right)}\mathop{\mathrm{se}_{{2n+1}}\/}\nolimits\!\left(z,h^{2}\right),
28.10.7 \frac{2}{\pi}\int _{{0}}^{{\ifrac{\pi}{2}}}\mathop{\sin\/}\nolimits z\mathop{\sin\/}\nolimits t\mathop{\sin\/}\nolimits\!\left(2h\mathop{\cos\/}\nolimits z\mathop{\cos\/}\nolimits t\right)\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits\!\left(t,h^{2}\right)dt=-\frac{hB_{2}^{{2n+2}}(h^{2})}{2{\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits^{{\prime}}}\!\left(\frac{1}{2}\pi,h^{2}\right)}\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits\!\left(z,h^{2}\right),
28.10.8 \frac{2}{\pi}\int _{{0}}^{{\ifrac{\pi}{2}}}\mathop{\cos\/}\nolimits z\mathop{\cos\/}\nolimits t\mathop{\sinh\/}\nolimits\!\left(2h\mathop{\sin\/}\nolimits z\mathop{\sin\/}\nolimits t\right)\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits\!\left(t,h^{2}\right)dt=\frac{hB_{2}^{{2n+2}}(h^{2})}{2{\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits^{{\prime}}}\!\left(0,h^{2}\right)}\mathop{\mathrm{se}_{{2n+2}}\/}\nolimits\!\left(z,h^{2}\right).

§28.10(iii) Further Equations

See §28.28. See also Prudnikov et al. (1990, pp. 359–368), Erdélyi et al. (1955, p. 115), and Gradshteyn and Ryzhik (2000, pp. 755–759). For relations with variable boundaries see Volkmer (1983).