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Apparent Weight – Downward Acceleration Alternative View The elevator is accelerated downward. !a y !w !FN Net force in the new y direction (downward) acting on the person: Fnet = w − FN = ma So apparent weight is: FN = w − ma = 400 N 53 Static Friction The static friction force between dry, unlubricated surfaces is: • independent of area of contact for hard surfaces – not true for deformable surfaces, such as tire rubber. 54 A cup of coffee sits on a table in a plane (µs = 0.30). The plane accelerates. What is the maximum acceleration before the cup starts to slide? For the cup not to slide: fs = ma (second law) fsmax = µsFN = µs mg and fsmax = mamax FN fs mg a So, mamax = µs mg → amax = µs g = 0.3g amax = 2.94 m/s2 55 Kinetic Friction Occurs when surfaces slide. Friction force opposes the relative motion of the surfaces. The magnitude of the kinetic friction force is: fk = µk FN µk = coefficient of kinetic friction The kinetic friction force is: • independent of area of contact between the surfaces • independent of relative speed of the surfaces for small speeds – high speed of sliding may cause heating and a change in the properties of the surfaces. 56 Serway, Physics for Scientists and Engineers 57 Yahoo search – The end of two bones which meet to form the joint are covered with articular cartilage, a surface material much like a tread of a tire. Its strength comes from tough fibers called collagen. The joint surface cartilage is well lubricated - more slippery than well-manufactured ball bearings... Its living cells are nourished by joint fluid, called synovial fluid which is also extremely good lubrication. 58 A block of weight 45 N rests on a horizontal table. Will the block move and, if so, what is its acceleration? FN µs = 0.650, µk = 0.420 As there are only two forces with vertical components: P = 36 N FN = w = 45 N The maximum static friction force is: m Ff Fs = µsFN = 0.65 × 45 = 29.25 N w = 45 N w = mg This is less than the force applied, so the block starts sliding. The kinetic friction force is: Fk = µk FN = 0.42 × 45 = 18.9 N The acceleration is: a = Fnet /m = (36 − 18.9 N)/(45/g kg) = 3.72 m/s2 59 A 20 kg sled is pulled across a horizontal surface at constant speed. FN Fk F = 80 N y 30o x mg What is the coefficient of kinetic friction? Speed is constant, so net force on sled = 0. x direction: F cos 30◦ = Fk = µk FN y direction: F sin 30◦ + FN = mg so, FN = F cos 30◦/µk and, FN = mg − F sin 30◦ Therefore, FN = F cos 30◦/µk = mg − F sin 30◦ 60 Therefore, FN = F cos 30◦/µk = mg − F sin 30◦ F cos 30◦ µk = mg − F sin 30◦ Substitute F = 80 N, m = 20 kg 80 cos 30◦ µk = = 0.444 ◦ 20 × 9.8 − 80 sin 30 61 A crate is being pushed across the floor at constant velocity by applying a downward force at an angle θ to the horizontal. Show that θ if is greater than a certain value, then it is impossible to push the crate, no matter how large the force. F Friction force: Fk = µk FN FN θ How large is FN? µk = 0.41 Forces in vertical direction: F k mg FN − F sin q − mg = 0 So FN = F sin q + mg The kinetic friction force is then Fk = µk FN = µk (F sin q + mg) The force pushing the crate sideways is F cos q 62 The kinetic friction force is then Fk = µk FN = µk (F sin q + mg) The force pushing the crate sideways is F cos q If the friction force is greater than the sideways pushing force, then the crate cannot be moved, no matter how great the applied force. That is, µk (F sin q + mg) > F cos q If F is very large, then mg is negligible by comparison, and then: µk F sin q > F cos q So, tan q > 1/µk = 1/0.41 Or, q > 68◦ 63