Law of Radioactivity defines that the number of Nuclei undergoing number of Nuclei present in the sample at that Instant.
Since from the graph; we have
$$N=N_{ - }e^{-\lambda t }$$ ....1
where $$\lambda $$=Disintegration constant
For $$\therefore $$ For $$T_{1/2}$$ is the time at $$N-\frac{1}{2}N_D$$
$$\Rightarrow$$ $$t=T_{1/2}$$
$$\frac{N_0}{2}$$=$$N_0e^{-\lambda\frac{T}{2}}$$
$$\Rightarrow$$ $$\boxed { T_{ 1/2 }=\frac { Ln2 }{ \lambda } =\frac { 0.693 }{ \lambda } } $$
And for Mean life -we have to sum it over the whole Range for
$$N(t)=N_0e^{-\lambda t}$$
for number of nuclei which decay in time t to t t $$\triangle$$;
$$N(t)\triangle t=\lambda N_{ 0 }e^{ -\lambda \, t}\triangle t$$
For Integration it over the Range $$T=0\, to\,\infty$$
$$\tau$$=$$\frac { \lambda N_{ 0 }\iint _{ 0 }^{ \infty }{ te^{ -\lambda t }dt } }{ N_ 0 }$$
$$=\lambda \int ^{ \infty }_0{ t } e^{ \lambda t }dt$$
$$\boxed { \tau =\frac { 1 }{ \lambda } } $$
Mean-life