Compare the push to the static limit: below it the block stays, above it the block slides and kinetic friction sets the acceleration.
Example
Compare the push to the static limit: below it the block stays, above it the block slides and kinetic friction sets the acceleration. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.
highlighted = computed this step
Push gently: it stays put
Push with 8 newtons. That is less than the 10 newton static limit, so static friction quietly matches it at 8 newtons and the block does not move.
8N<10N⇒stays
Push harder: it breaks free
Push with 12 newtons instead. That beats the 10 newton limit, so the block breaks free and starts sliding.
12N>10N⇒slides
The sign of the excess decides the verdict
Compare the push to the static limit. Negative excess means the limit can still hold, zero is just at the edge, and positive excess means the block breaks free.
P8N10N12Nfsmax10N10N10NP−fsmax−2N0N2N
Now kinetic friction sets the acceleration
While sliding, friction is the kinetic 6 newtons. The net force is the push minus friction, 12 minus 6, which is 6 newtons. Divide by the mass: 6 over 2 is 3 metres per second squared. The drag dropped from the 10 newton limit to 6 newtons the moment it broke free, which is why a heavy box lurches as it starts to slide.
a=2kg12−6=2kg6=3m/s2
More sliding push gives more acceleration
Once it is sliding, kinetic friction is the fixed drag for this block and surface. More push leaves more net force, so acceleration grows.
P12N14N16NFnet6N8N10Na3m/s24m/s25m/s2
mechanicsPushing 8 N then 12 N against a 10 N static limit makes the stay-or-slide verdict concrete, with a clean 3 m/s^2 once it slides.