Équilibre des corps reliés par des cordes et des poulies – application de la première loi de Newton : problèmes et solutions

1. A box of masse 5 kg is on an inclined plane at an angle 30o. The box supported by a cord. Determine the tension force (T) and the force normale (N)!

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 1

Solution

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 2ΣFx = 0

T – w sin 30o = 0

T = w sin 30o

T = (5 kg)(9.8 m/s2) sin 30o

T = (49)(0.5)

T = 30 000 Newtons

ΣFy = 0

N – w cos 30o = 0

N = w cos 30o

N = (49)(0.87)

N = 43 Newtons

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2. Two objects of mass m1 = m2 = 2 kg, connected by a massless string over a frictionless pulley. Find the tension force T1 et T2.

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 3

Solution

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 4

(a) Free-body diagram for object 1 (b) Free-body diagram for object 2

Apply Newton’s first law to object 1 :

ΣFy = 0

T1 - dans1 = 0

T1 =w1 = m1 g = (2 kg)(9.8 m/s2) = 19.6 N

Appliquer Newton’s first law to object 2 :

ΣFy = 0

T2 - dans2 = 0

T2 =w2 = m2 g = (2 kg)(9.8 m/s2) = 19.6 N

T1 = T2 = 19.6 XNUMX N.

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3. An object of poids wA = 30 N and an object of weight wB = 40 N, are attached by a lightweight cord that passes over a frictionless pulley of the negligible mass. Determine the coefficient of the maximum frottement statique between wB and inclined surface, if the system is at rest.

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 5

Solution

Equilibrium of bodies connected by cord and pulley – application of Newton's first law problems and solutions 6

(a) Free-body diagram for object wA (b) Free-body diagram for object wB

Apply Newton’s first law to object wA in vertical (y) direction :

ΣFy = 0 (no acceleration in vertical direction)

T – wA = 0

T = wA = 30 Newton

Apply Newton’s first law to object wB in vertical (y) direction :

ΣFy = 0

N – wB cos 45o = 0

N = wB cos 45o = (40)(0.7) = 28 Newtons

Apply Newton’s first law to object wB in horizontal (x) direction :

ΣFx = 0

Fk +wB péché 45o – T = 0

μs N + wB péché 45o – T = 0

μs (28) + (40)(0.7) – 30 = 0

μs (28) + 28 – 30 = 0

μs (28) = 30 – 28

μs (28) = 2

μs = 2 / 28

μs = 0.07

The coefficient of the maximum static friction between wB and inclined surface = 0.07.

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  1. Particules en équilibre unidimensionnel
  2. Particules en équilibre bidimensionnel
  3. Équilibre des corps reliés par des cordes et des poulies
  4. Equilibrium of bodies on inclined plane

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