Fix a value of parameter $t$ and consider the curve with equation $F(t,x,y)=0$. Take then a slightly displaced curve $F(t+\Delta t,x,y)=0$ and suppose this curve meets the other one at some point $P$.
If $\lim_\limits{\Delta t\to0}P$ exists, then we say that this limiting point (which we may call $P(t)$) belongs to the envelope of the pencil of curves.
The coordinates of $P$ satisfy the system
$$
\cases{
F(t,x,y)=0 \\
F(t+\Delta t,x,y)=0 \\
}
$$
But this system is equivalent to the system obtained substituting the second equation with the difference of the two equations, hence equivalent to:
$$
\cases{
F(t,x,y)=0 \\
\\
\displaystyle{F(t+\Delta t,x,y)-F(t,x,y)\over \Delta t}=0 \\
}
$$
We can now take the limit $\Delta t\to0$ in the second equation (provided $F$ is regular enough):
$$
\cases{
F(t,x,y)=0 \\
\\
\displaystyle{\partial F(t,x,y)\over \partial t}=0 \\
}
$$
The solutions $(x(t),y(t))$ of this system will then be the coordinates of limiting point $P(t)$: as $t$ varies, they describe a curve which is the envelope of the pencil of curves.
If you want a cartesian equation for the envelope, you can instead eliminate $t$ to obtain a single equation in $(x,y)$.