It sounds like your question is about the nature of normal forces.
A massive object is subject to gravity. If you drop it, the only force acting on it is gravity, and so it accelerates downward.
The same object sitting on a table is motionless. The acceleration is $0$, so the total force is $0$. The table exerts an upward force just as strong as the downward force of gravity.
If you stack another mass on top, now the downward force on the object is twice as big. The table makes its upward force twice as big to cancel it.
On the other hand, if you pick up the mass, the table does nothing to prevent you. It reduces its force to $0$, but does not reverse it to pull the object downward.
This illustrates the nature of reaction forces. Without the reaction force the mass would penetrate into the table. The reaction force is just strong enough to prevent this.
It is a little more intuitive with a spring. If you compress a spring, the spring pushes back. The harder you push, the more the spring is compressed, and the more it pushes back. If you lift your hand off, the spring does not hold onto you.
The origin of the tabletop and spring forces is the same. Atomic bonds are stiff. If you deform them, the push back to try to keep their shape.
A spring has a shape that is makes it easier to bend than a solid block of steel. The spring is made of thin coils. A small bend in each piece of the coil adds up to a big compression. The block of steel would bend a microscopic amount. And so does the table.
So for your example, two blocks sit side by side with nothing pressing them together. The force of one block pressing against the other is $0$. So the reaction force from the other block is $0$. The blocks do not push each other apart.
Suppose you squeeze them together. Then the blocks push each other apart just hard enough to keep from penetrating into each other. They stay still. If you stop pushing them together, they stop pushing each other apart.