Kūnų, sujungtų virvėmis ir skriemuliais, pusiausvyra – pirmojo Niutono dėsnio uždavinių ir sprendimų taikymas

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

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

Sprendimas

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/s2) sin 30o

T = (49)(0.5)

T = 24.5 niutonų

Fy = 0

N – w cos 30o = 0

N = w cos 30o

N = (49)(0.87)

N = 43 niutono

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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 ir t2.

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

Sprendimas

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

Aplikuoti Pirmasis Niutono dėsnis to object 2 :

Fy = 0

T2 - w2 = 0

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

T1 = T.2 = 19.6 N.

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3. An object of svoris 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 statinė trintis 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

Sprendimas

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 niutonų

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

Fy = 0

Š – vB cos 45o = 0

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

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

Fx = 0

Fk +wB 45. nuodėmėo – T = 0

μs N + wB 45. nuodėmėo – 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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  4. Equilibrium of bodies on inclined plane

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