Equilibri de cossos connectats per cordes i politges: aplicació dels problemes i solucions de la primera llei de Newton

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

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

Solució

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

T – w sin 30o = 0

T = w sin 30o

T = (5 kg)(9.8 m/s)2) sin 30o

T = (49)(0.5)

T = 24.5 Newtons

Fy = 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 i T2.

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

Solució

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 :

Fy = 0

T1 - w1 = 0

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

Aplica Primera llei de Newton to object 2 :

Fy = 0

T2 - w2 = 0

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

T1 =T2 = 19.6 N.

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3. An object of pes 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 fricció estàtica 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

Solució

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 :

Fy = 0 (no acceleration in vertical direction)

T – wA = 0

T = wA = 30 Newtons

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

Fy = 0

N – oB cos 45o = 0

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

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

Fx = 0

Fk +wB pecat 45o – T = 0

μs N + wB pecat 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. Partícules en equilibri unidimensional
  2. Partícules en equilibri bidimensional
  3. Equilibri de cossos connectats per cordes i politges
  4. Equilibri dels cossos en un pla inclinat

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