Table 3: Assumed binary parameter of WX Ceti and model parameter. In the EMT scenario $f_{\rm ill}$ defines the strength of enhanced mass transfer and $\langle\mbox{$R_{\rm out}$ }\rangle$ the mean outer radius which is assumed to be given by the average of r₁, r₂, and $r_{\rm max}$ in Table 1 of Paczynsky (1977). We arbitrarily assumed a rather low value of the viscosity parameter during quiescence ( $\alpha _c$ ) to reproduce the long lasting low-states.
$P_{\rm orb}$ /h 1.4

$T_{\rm sec}$ 2750 K

$\mbox{$M_{\rm wd}$ }/\mbox{$M_{\odot}$ }$ 1.0

$\mbox{$M_{\rm sec}$ }/\mbox{$M_{\odot}$ }$ 0.1

$R_{\rm wd}$ /10⁸ cm 5.6

i/ $~^{\circ}$ 60

d/pc 100

$\alpha_{\rm c}$ 0.008

$\alpha_{\rm h}$ 0.12

$\langle R_{{\rm out}}\rangle/10^{10}$ cm 2.1

$f_{\rm ill}$ 0.15

**Table 3:** Assumed binary parameter of WX Ceti and model parameter. In the EMT scenario $f_{\rm ill}$ defines the strength of enhanced mass transfer and $\langle\mbox{$R_{\rm out}$ }\rangle$ the mean outer radius which is assumed to be given by the average of r₁, r₂, and $r_{\rm max}$ in Table 1 of Paczynsky (1977). We arbitrarily assumed a rather low value of the viscosity parameter during quiescence ( $\alpha _c$ ) to reproduce the long lasting low-states.
$P_{\rm orb}$ /h	1.4
$T_{\rm sec}$	2750 K
$\mbox{$M_{\rm wd}$ }/\mbox{$M_{\odot}$ }$	1.0
$\mbox{$M_{\rm sec}$ }/\mbox{$M_{\odot}$ }$	0.1
$R_{\rm wd}$ /10⁸ cm	5.6
i/ $~^{\circ}$	60
d/pc	100
$\alpha_{\rm c}$	0.008
$\alpha_{\rm h}$	0.12
$\langle R_{{\rm out}}\rangle/10^{10}$ cm	2.1
$f_{\rm ill}$	0.15

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