Statics p. 97 prints F ≤ μs N and calls the largest value the limiting friction. Equality is impending slip, not the force at rest. Dynamics p. 110 adds F < μs N (no slip), F = μs N (impending), and F = μk N (sliding). Belt friction F1 = F2 e^{μθ} (θ in radians) and the square-thread screw are on Statics p. 98; they are not the dry-friction inequality tested as the Civil statics bullet. On a slope, impending motion is the derived condition tan α = μs.
μs
Static friction coefficient
μk
Kinetic friction coefficient
N(N)
Normal force
Step-by-step solved example
A 200 kg crate rests on a horizontal floor, μ_s = 0.35. What horizontal force starts motion? g = 9.81 m/s².
Horizontal 200 kg crate: N = mg and impending slip at P = μs N.
1. Normal force
N = mg = 200×9.81 = 1962 N.
2. Impending friction
Impending motion: F = μ_s N = 0.35×1962 = 686.7 N → 687 N. At rest with a smaller push, F would be less than μs N.
F=687N
Answer: 687 N
10 practice questions
0/10 correct
1.If μ_s = 0.4 and N = 500 N, max static friction is
2.A block on a rough horizontal surface with no applied load has friction
3.Angle of repose is
4.Typically μ_k compared with μ_s is
5.Wedge of angle θ, μ = 0, self-locking never occurs because
6.A 50 lb block, μ_s = 0.25, just moves under P. P is
7.On a 20° slope, μ_s = 0.5, a block
Block on a 20° incline. Weight acts straight down. Normal is perpendicular to the surface. Friction acts up the plane. μs = 0.5.
8.Belt friction (no slip impending) uses
9.Normal force on a horizontal floor under a 10 kN crate is
10.If applied force is 30 N and μ_s N = 50 N, friction is