Table 1: Total wave energy fluxes $F_{\rm tors}$ (erg/ cm² s) generated as torsional waves in a single magnetic flux tube embedded in the solar convection zone are compared to the fluxes for transverse tube waves, $F_{\rm trans}$ and longitudinal tube waves, $F_{\rm long}$ ; note that the factor 4 (see discussion below Eq. (23)) was included in the computation of the wave energy fluxes for transverse tube waves. All presented fluxes were computed by using analytical methods only.
$\alpha$ $B_{\rm o}/B_{\rm eq}$ $F_{\rm tors}$ $F_{\rm trans}$ $F_{\rm long}$

1.0 0.85 $6.0\times 10^7$ $1.2\times 10^8$ $6.3\times 10^6$

1.5 0.85 $1.4\times 10^8$ $2.9\times 10^8$ $1.4\times 10^7$

2.0 0.85 $2.6\times 10^8$ $5.6\times 10^8$ $2.4\times 10^7$

2.0 0.75 $4.4\times 10^8$ $8.8\times 10^8$ $5.5\times 10^7$

2.0 0.95 $1.3\times 10^8$ $3.6\times 10^8$ $5.9\times 10^6$

**Table 1:** Total wave energy fluxes $F_{\rm tors}$ (erg/ cm² s) generated as torsional waves in a single magnetic flux tube embedded in the solar convection zone are compared to the fluxes for transverse tube waves, $F_{\rm trans}$ and longitudinal tube waves, $F_{\rm long}$ ; note that the factor 4 (see discussion below Eq. (23)) was included in the computation of the wave energy fluxes for transverse tube waves. All presented fluxes were computed by using analytical methods only.
$\alpha$	$B_{\rm o}/B_{\rm eq}$	$F_{\rm tors}$	$F_{\rm trans}$	$F_{\rm long}$
1.0	0.85	$6.0\times 10^7$	$1.2\times 10^8$	$6.3\times 10^6$
1.5	0.85	$1.4\times 10^8$	$2.9\times 10^8$	$1.4\times 10^7$
2.0	0.85	$2.6\times 10^8$	$5.6\times 10^8$	$2.4\times 10^7$
2.0	0.75	$4.4\times 10^8$	$8.8\times 10^8$	$5.5\times 10^7$
2.0	0.95	$1.3\times 10^8$	$3.6\times 10^8$	$5.9\times 10^6$

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