1. A 2-kg block lies on a rough inclined plane at an angle 37o to the horizontal. Determine the magnitude of the external force exerted on the block, so the block is not slides down the plane. (sin 37o = 0.6, cos 37o = 0.8, g = 10 m.s-2, µk = 0.2)
Mōhiotia:
Mass (m) = 2 kg
Whakaterenga na te kaha o te kaha (g) = 10 m/s2
Block’s taimaha (w) = mg = (2)(10) = 20 Ngā Newton
Hara 37o = 0.6
Kohinga 37o = 0.8
Tauwehenga o te te waku nekeneke (µk) = 0.2
The y-component of the weight (wy) =w whaimana 37o = (20)(0.8) = 16 Ngā Newton
The x-component of the weight (wx) = w sin θ = (20)(sin 37) = (20)(0.6) = 12 Newton
the normal force (N) = wy = 16 Niutona
hiahia : The external force (F)
otinga :
wx = 12 Niutona
The force of the kinetic friction (fk) = µk N = (0.1)(16) = 1.6 Ngā Niutoni
The magnitude of the external force F exerted on the block :
F + fk - wx = 0
F = wx - fk
F = 12 – 1.6
F = 10.4 Newton
The external force F greater than 10.4 Newton.
2. Mass of a block = 2 kg, coefficient of static friction µs = 0.4 and θ = 45o. Determine the magnitude of the force F so the block start to slides up.
Mōhiotia:
The coefficient of the static friction (µs) = 0.4
Koki (θ) = 45o
Te whakaterenga nā te kaha ā-papa (g) = 10 m/s2
Block’s mass (m) = 2 kilogram
Block’s weight (w) = m g = (2 kg)(10 m/s2) = 20 kg m/s2 = 20 Niutona
The x-component of the weight (wx) = w sin θ = (20)(sin 45) = (20)(0.5√2) = 10√2 Newton
The y-component of the weight (wy) = w cos θ = (20)(cos 45) = (20)(0.5√2) = 10√2 Newton
hiahia : The magnitude of the force F
Rongoā:
Block starts to slide up, if F ≥ wx + fs.
The x-component of the weight :
wx = 10√2 Nūtene
the y-component of the weight :
wy = 10√2 Nūtene
Te kaha noa :
N = wy = 10√2 Nūtene
The force of the static friction :
fs = µs N = (0,4)(10√2) = 4√2
The magnitude of the force F so that the block starts to slide up :
F ≥ wx + fs
F ≥ 10√2 + 4√2
F ≥ 14√2 Newton
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- Ngā matūriki i roto i te taurite kotahi-ahu
- Ngā matūriki i roto i te taurite rua-ahu
- Te taurite o ngā tinana e honoa ana e ngā taura me ngā pūwero
- Equilibrium of bodies on the inclined plane