The modern viewpoint (though not favoured by everyone) is this.
A body's mass m (used to be called $rest\ mass, m_0$) is an intrinsic property of the body, independent of its motion. But it is not simply a sum of masses of its constituent particles. It increases with the body's internal energy (including vibrational energy of particles) according to $\Delta U = c^2 \Delta m$.
A body's total energy, E is given by $E=\gamma m c^2$, in which $\gamma$ has its usual meaning. $\gamma m$ (which does, of course, increase with the body's speed) used to be called the body's relativistic mass, but this usage has largely fallen out of favour, partly because, except for the 'mere' constant, $c^2$, $\gamma m$ is telling us the body's total energy. Why confuse the issue by giving it another name?
If the body is at rest, $\gamma=1$, so the energy of the body at rest is $E=m c^2$. [The relationship, $\Delta U = c^2 \Delta m$, given in the first paragraph follows from $E=m c^2$, applied to an ordinary body.]
The body's KE when moving is therefore $E_k=\gamma m c{^2}-m c^2$.
In SR, a body's momentum is given by $\vec{p}= \gamma m \vec{v}$. Part of the motivation for calling $\gamma m$ "relativistic mass" was that we then preserve in SR the Newtonian momentum formula, with relativistic mass instead of rest mass. But this is now generally considered to be not worth the conceptual disadvantages described above. And, what's more, it doesn't help to preserve other Newtonian formulae, such as that for KE!