Equilibrio di corpi collegati da corde e carrucole: applicazione della prima legge di Newton, problemi e soluzioni

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 forza normale (N)!

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

Soluzione

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 = 24.5 Newton

ΣFy = 0

N – w cos 30o = 0

N = w cos 30o

N = (49)(0.87)

N = 43 Newton

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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 e T2.

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

Soluzione

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 - w1 = 0

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

APPLICA Prima legge di Newton to object 2 :

ΣFy = 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 peso 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 Frizione statica 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

Soluzione

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 – oB cos 45o = 0

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

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

ΣFx = 0

Fk +wB peccato 45o – T = 0

μs N + wB peccato 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. Particelle in equilibrio unidimensionale
  2. Particelle in equilibrio bidimensionale
  3. Equilibrio dei corpi collegati da corde e pulegge
  4. Equilibrio dei corpi su un piano inclinato

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