Block Around a Track: Find Force & Coeff of Friction

In summary: It is important to include units and have them cancelled out properly when you do your calculations.In summary, a block of mass 0.50 kg is fired with an initial speed of 4.0 m/s along a horizontal frictionless track, then moves along a frictionless semicircular vertical track of radius 1.5 m. The force exerted by the track on the block at points A and B is 15.13 N and 20.03 N, respectively. The bottom of the track consists of a 0.40 m section with friction, and the coefficient of kinetic friction between the block and that portion of the bottom track is 0.17, as determined by applying the Work-Energy theorem and the equation
  • #1
minimario
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2

Homework Statement


A small block of mass m = 0.50 kg is fired with an initial speed of v0 = 4.0 m/s along a horizontal section of frictionless track, as shown in the top portion of Figure P7.58. The block then moves along the frictionless, semicircular, vertical tracks of radius R = 1.5 m. (a) Determine the force exerted by the track on the block at points A and B. (b) The bottom of the track consists of a section (L = 0.40 m) with friction. Determine the coefficient of kinetic friction between the block and that portion of the bottom track if the block just makes it to point C on the first trip. (Hint: If the block just makes it to point C, the force of contact exerted by the track on the block at that point is zero.)

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Homework Equations



## a_c = m v^2 / r ##, ## F = ma ##

The Attempt at a Solution



(a) We begin by using CoE with the level at B defined as 0. Right before sliding onto the track, the total energy is ## \frac{1}{2} m 4^2 + m g 3 = m(8+3g) ##

At point A, the total energy is ## \frac{1}{2} m v^2 + mg(1.5) = m(\frac{v^2}{2} + 1.5g) ##. Energy is conserved, so ## 2(8+3g-1.5g) = v^2 \Rightarrow v^2 = 45.4 ## (Assuming g = 9.8).

Since the only force at point A is the one causing the centripetal acceleration, the force of track on block is ## \frac{mv^2}{r} = 15.13 ## N.

At point B, the total energy is ## \frac{1}{2} mv^2 ##. Energy conserved, so ## 2 (8+3g) = v^2 = 74.8 ##. At the bottom, however, the weight of the object takes role, and net force = ## \frac{mv^2}{r} - mg = 20.03 ## N. (Not sure it's supposed to be + mg or -mg, but I think it should be mg. Any ideas on this would be appreciated)

Is this right? If so, I will proceed to post my part B solution. No answer attached with this one, so not sure.

Edit:

(b) At the top, normal force is 0, so mg is the only force contributing to the centripetal force. Therefore, ## mg = mv^2 / r \Rightarrow v^2 = 14.7 ##. Conservation of energy with the point at the bottom of the semicircle and point C gives ## \frac{1}{2} m 14.7 + 3mg = \frac{1}{2} mv^2 \Rightarrow v^2 = 73.5 ## at the bottom.

Now, by the Work-Energy theorem, the work done by friction is equal to the change in energy. Since no change in potentional energy, all change is in kinetic energy, so ## W_fric = 1/2*m*(74.8-73.5) = 0.325 ##. In addition, ## W = Fd##, so ##0.325 = 0.4F \Rightarrow F = 0.8125 ##. In addition, ##F = \mu * mg \Rightarrow \mu = 0.17 ##.

Is all of this correct, or did I make a mistake somewhere? (Again, can't find the same problem anywhere online)

Thanks!

-minimario
 
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  • #2
minimario said:
Not sure it's supposed to be + mg or -mg

The force from the track on the block has to be such that the resultant force keeps the block in the circular orbit. What is the resultant force and what magnitude should it have?

Your reasoning otherwise seems essentially ok - but - You really should not insert values into your equations until the final step. Inserting numbers really obscures the physics and makes it difficult to check limiting cases. Furthermore, your equations are missing units which makes things even more difficult to read (and technically even wrong). Without units, your expressions do not mean anything. For example, v^2 = 45.4 does not tell you anything - v could be measured in cm/hour, lightyears/Myr, m/s, or km/day.
 

FAQ: Block Around a Track: Find Force & Coeff of Friction

1. How do I calculate the force and coefficient of friction for a block around a track?

The force and coefficient of friction for a block around a track can be calculated using the formula F = μN, where F is the force, μ is the coefficient of friction, and N is the normal force. The normal force can be determined by multiplying the mass of the block by the acceleration due to gravity, and the force can be found by measuring the speed and radius of the track.

2. What is the significance of finding the force and coefficient of friction for a block around a track?

Finding the force and coefficient of friction for a block around a track can help us understand the physics of circular motion and how friction affects the motion of objects. It can also be used to calculate the minimum speed required for the block to stay on the track without slipping.

3. Can the coefficient of friction change as the block moves around the track?

Yes, the coefficient of friction can change as the block moves around the track. This can be due to factors such as changes in surface conditions or the addition of a lubricant. It is important to account for any changes in the coefficient of friction when calculating the force required for the block to stay on the track.

4. How does the mass of the block affect the force and coefficient of friction?

The mass of the block affects the force and coefficient of friction in two ways. First, a heavier block will require a greater force to stay on the track due to its increased weight. Second, the mass of the block affects the normal force, which in turn affects the coefficient of friction. A heavier block will have a greater normal force, resulting in a higher coefficient of friction.

5. What are some real-life applications of calculating the force and coefficient of friction for a block around a track?

Some real-life applications of calculating the force and coefficient of friction for a block around a track include designing roller coasters or other amusement park rides, determining the minimum speed for a car to take a turn without slipping, and understanding the physics of circular motion in sports such as ice skating and figure skating.

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