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A block of mass 0.500 kg is pushed against a horizontal spring of negligible mass until the spring is compressed a distance x (Fig. P8.65). The force constant of the spring is 450 N/m. When it is released, the block travels along a frictionless, horizontal surface to point A, the bottom of a vertical circular track of radius R 5 1.00 m, and continues to move up the track. The block’s speed at the bottom of the track is vA 5 12.0 m/s, and the block experiences an average friction force of 7.00 N while sliding up the track.(a) What is x?(b) If the block were to reach the top of the track, what would be its speed at that point?(c) Does the block actually reach the top of the track, or does it fall off before reaching the top?

Respuesta :

Answer:

Part a)

[tex]x = 0.4 m[/tex]

Part b)

[tex]v_i = 11.7 m/s[/tex]

Part c)

Speed is more than the required speed so it will reach the top

Explanation:

Part a)

As we know that there is no frictional force while block is moving on horizontal plane

so we can use energy conservation on the block

[tex]\frac{1}{2}mv^2 = \frac{1}{2}kx^2[/tex]

[tex]\frac{1}{2}0.500(12^2) = \frac{1}{2}(450)x^2[/tex]

[tex]x = 0.4 m[/tex]

Part b)

If the track has average frictional force of 7 N then work done by friction while block slides up is given as

[tex]W_f = -7( \pi R)[/tex]

[tex]W_f = -7(\pi \times 1.00)[/tex]

[tex]W_f = -22 J[/tex]

work done against gravity is given as

[tex]W_g = - mg(2R)[/tex]

[tex]W_g = -(0.500)(9.8)(2\times 1)[/tex]

[tex]W_g = -9.8 J[/tex]

Now by work energy equation we have

[tex]\frac{1}{2}mv_i^2 + W_f + W_g = \frac{1}{2}mv_f^2[/tex]

[tex]\frac{1}{2}0.5(12^2) - 9.8 - 22 = \frac{1}{2}(0.5)v_f^2[/tex]

[tex]v_f = 4.1 m/s[/tex]

Part c)

now minimum speed required at the top is such that the normal force must be zero

[tex]mg = \frac{mv^2}{R}[/tex]

[tex]v = \sqrt{Rg}[/tex]

[tex]v = 3.13 m/s[/tex]

so here we got speed more than the required speed so it will reach the top

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