
Paul L. answered 03/23/19
4 Years of Teaching and 12 years of Tutoring Experience
This is a classic Dynamics problem. 1st step is to draw a free body diagram of the brick showing all forces. Vertically there are two forces, the normal force N pointing up and weight mg pointing down.
Using Newton's 2nd Law Fnet = ma, Vertically: Fnet = N-mg = ma (taking up to be positive). There is no movement vertically therefore no acceleration vertically so N-mg = 0 or N=mg.
Horizontally there are two forces, Tension T and friction f. Let's assume the brick is being pulled to the right. Friction always opposes motion so f points to the left.
Using Newton's 2nd Law Fnet = ma again, Horizontally: Fnet = T- f = ma (taking right to be positive). There is movement horizontally so there will be acceleration horizontally unless we are moving at constant velocity.
Solving for a and substituting µN for f we get a = (T-µN)/m = (T-µmg)/m = (50N-.32×10kg×9.8m/s2)/10kg = +1.864 m/s2 where the positive sign means to the right or in the same direction as T