Block 1 (m1 = 1.0 kg) sits on a frictionless inclined surface and is connected to block 2 (m2 = 2.0 kg). The pulley is massless and frictionless. An upward force of magnitude F = 6.0 N acts on block 2, which has a downward acceleration of 5.5 m/s2 . What is (a) the tension in the connecting cord and (b) the angle ?

Respuesta :

1) 2.6 N

2) [tex]18.4^{\circ}[/tex]

Explanation:

1)

The force acting on block 2, which is the one hanging vertically, are:

- The upward force of magnitude F = 6.0 N

- The tension in the rope, T, upward

- The force of gravity, [tex]m_2 g[/tex], downward

So the equation of the forces on block 2 is

[tex]F+T-m_2 g = m_2 a[/tex]

where

[tex]m_2 = 2.0 kg[/tex] is the mass

[tex]g=9.8 m/s^2[/tex] is the acceleration due to gravity

[tex]a=-5.5 m/s^2[/tex] is the downward acceleration

Solving the equation for T, we find the tension in the cord:

[tex]T=m_2 a +m_2 g-F=(2.0)(-5.5)+(2.0)(9.8)-6.0=2.6 N[/tex]

2)

For this part instead, we analyze the situation for block 1.

Block 1 sits on the frictionless inclined surface, connected to block 2 via the rope.

Therefore, the forces acting on block 1 along the inclined plane are:

- The tension in the cord, T, forward (up along the plane)

- The force F, acting in the same direction of T

- The component of the weight parallel to the plane, backward (down along the plane), [tex]m_1g sin \theta[/tex]

So the equation of the forces for block 1 is

[tex]T+F-m_1 g sin \theta = m_1 a[/tex]

where:

[tex]T=2.6 N[/tex] is the tension in the cord

F = 6.0 N

[tex]m_1=1.0 kg[/tex] is the mass of the block

[tex]\theta[/tex] is the angle of the incline

[tex]a=5.5 m/s^2[/tex] is the acceleration of the block (up along the plane, so positive)

Therefore, the angle is:

[tex]sin \theta = \frac{T+F-m_1 a}{m_1 g}=\frac{2.6+6.0-(1.0)(5.5)}{(1.0)(9.8)}=0.316[/tex]

[tex]\theta=sin^{-1}(0.316)=18.4^{\circ}[/tex]

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