On the nonextensivity contributions in collisional plasma damping waves

Figures & data

Figure 1. Change of the amplitude ${\varphi }_1(\tau )$ with $Q$and q for ${\mu }_e=0.4,\sigma =1.1,{\mu }_p=0.6,\alpha$ $=1.0,V_0=0.5,{\tilde{\nu }}_0=0.7,L=0.86,{\nu }_{+0}=0.3,{\nu }_{-0}=0.3,$ and $\tau =1.$

Figure 2. Variation of $\mathrm{\Phi }(\chi ,\tau )$ versus χ and for Q = 0.03 (thick lines) and Q = 2.1 (thin lines), with $L=0.86,\sigma =1.1,V_0=0.4,{\mu }_p=0.7,{\mu }_e=0.4,\alpha =1.0,{\nu }_{+0}=0.3,{\tilde{\nu }}_0=0.7,{\nu }_{-0}=0.3,$ and q = 1.5.

Figure 3. Change of ${\varphi }_1(\tau )$ with ${\nu }_{+0}$ for different q when $\alpha =1.0,\sigma =1.1,L=0.86,V_0=0.5,{\mu }_e=0.5,{\mu }_p=0.7,{\tilde{\nu }}_0=0.7,{\nu }_{-0}=0.3$, $\tau =1,$ and q = 1.0 with (a) Q = 0.03; (b) Q = 2.1.

Figure 4. Change of $W(\tau )$ with ${\nu }_{+0}$ for different q when $\sigma =1.1,L=0.86,\alpha =1.0,V_0=0.5,{\mu }_e=0.5,{\mu }_p=0.7,{\tilde{\nu }}_0=0.7,{\nu }_{-0}=0.3$, $\tau =1,q=1.0,$ and Q = 0.03.

Figure 5. Variation of ${\varphi }_1(\tau )$ with ${\nu }_{-0}$ for different ${\tilde{\nu }}_0$ when $L=0.86,V_0=0.5,\alpha =1.0,\sigma =1.1$, ${\mu }_e=0.5,{\mu }_p=0.7,{\nu }_{+0}=0.3,q=1.0$, and $\tau =1$ with (a) Q = 0.03; (b) Q = 2.1.

Figure 6. Variation of $W(\tau )$ with ${\nu }_{-0}$for different ${\tilde{\nu }}_0$ when $\alpha =1.0,L=0.86,\sigma =1.1,V_0=0.5,{\mu }_e=0.5,{\mu }_p=0.7,{\nu }_{+0}=0.3,q=1.0$, $\tau =1$, and Q = 0.03.