A 3 kg block is placed at the top of a track consisting of two frictionless quarter circles of radius R equal to 2 m connected by a 7 m long, straight, horizontal surface. The coefficient of kinetic friction between the block and the horizontal surface is mu k equal to .1. The block is released from rest. From an expression that describes where the block stops, as measured from the left end of the horizontal surface, marked x=0.

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Answer:

6m

Explanation:

The initial potential energy of the block P.E =mgh

where mass m = 3kg

g= 9.81 m/s2

h = 2m

Hence P.E = 3*9.81*2 = 58.8 Joules

This energy converts to kinetic energy when the block is released from the top

K.E = [tex] mv^2/2 = 58.8 [/tex]

Solving for v, we obtain 6.26 m/s

The acceleration of the block by Newton's second law of motion,

ma = (μk)*mg

where μk = 0.1

Hence, a = 0.1*9.81 = 0.98m/s/s

Applying Newton's second equation of motion to solve,

[tex] v^2 - u^2 =2as [/tex]

where u = 0 m/s (released from rest0

Hence, [tex] 6.26^2 = 2*0.98*s [/tex]

Solving for s,

s= 20m

Therefore, the distance after two complete cycles = 20 -2(7) = 6m

The expressions that describes where the block stops from the left end of the horizontal surface, marked x = 0 is; [tex]x = \dfrac{0.3 \cdot R}{\mu_k}[/tex]

The reasons why the above values are correct are as follows;

The given parameters are;

Mass of the block, m = 3 kg

Radius of the quarter circular track, R = 2 m

Length of the horizontal track, L = 7 m

Coefficient of friction between the block and the horizontal surface, [tex]\mu_{k}[/tex] = 0.1

Required:

To form an expression that describes where the block stops as measured from the left end of the horizontal surface marked x = 0

Solution;

A quarter of a circle has the radii lengths arranged at right angles to each other, both of which are perpendicular to tangents of the circle

A flat surface, such as the horizontal surface in the question is a tangent to the circle

Therefore;

The radius of the circle, perpendicular to the horizontal surface = The height from which the block is released

Potential energy = m·g·h

Where;

g = Acceleration due to gravity ≈ 9.81 m/s²

Therefore, the potential energy of the block, P.E., is given as follows;

P.E. = m·g·R

P.E. = 3 kg × 2 m × 9.81 m/s² = 58.86 J

The potential energy of the block, P.E. = 58.86 J

The frictional force due to the block, [tex]F_f[/tex] = m·g·[tex]\mu_{k}[/tex]

3 kg × 9.81 m/s²× 0.1 = 2.943 N

Work done by the friction as the block moves along the horizontal surface, is given as follows;

Work done = Force × Distance moved in the direction of the force

∴ Work done by friction = [tex]F_f[/tex] × d

Where;

d = The distance from the left end where the block reaches

Work done by friction also = Energy transferred = ΔE

When the block stops, the total energy in the block is transferred

Therefore, when the block stops, according to the law of conservation of energy;

Work done by friction = [tex]F_f[/tex] × d = Energy transferred = ΔE = P.E.

2.943·d = 58.86

[tex]d = \dfrac{m \cdot g \cdot R}{m \cdot g \cdot \mu_k} = \dfrac{R}{\mu_k}[/tex]

[tex]d = \dfrac{58.86 \, J}{2.943 \, N } = 20 \, m[/tex]

Therefore, given that work is done by friction only on the horizontal plane, we have;

The distance travelled on the horizontal surface = 20 m

Therefore, the block traverses the horizontal surface twice, and then for another 6 meters

Let N represent the number of times the block traverses on the horizontal surface, and let L represent the length of the horizontal surface, we have;

d = N·L + x (when N is even)

d = N·L + L - x = L·(N + 1) - x (when N is odd)

[tex]\dfrac{R}{\mu_k} = N \cdot L + x[/tex]

[tex]\dfrac{R}{\mu_k} - N \cdot L = x[/tex]

[tex]x = L \cdot (N + 1) - \dfrac{R}{\mu_k}[/tex]

Therefore;

The expressions that describe where the block stops as measured from the left end of the horizontal surface marked x = 0 are;

[tex]\dfrac{R}{\mu_k} - 7 \cdot N_{even} = x[/tex] and  [tex]x = 7 \cdot(N_{odd} + 1) - \dfrac{R}{\mu_k}[/tex]

The distance where the block stops from the left end is 6 meters, therefore, we have;

[tex]\dfrac{R}{\mu_k} = 20[/tex]

[tex]x = 6 = \dfrac{0.3 \cdot R}{\mu_k}[/tex]

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