Learning Objectives

1. Arthrokinematics Of Knee Joint
2. Arthrokinematics Def
3. Arthrokinematics Of Talocrural Joint
4. Arthrokinematics Spin
5. Aethro-kinematics

By the end of this section, you will be able to:

Aethro-Kinematic Answer: 'The mass increase of an accelerated particle 'is not an illusion of some relatively moving observers. It is a simple hydrodynamic calculation, based on Newton's third law of action and reaction between the kinetic energies of the particle and the opposing resistance of the aether, which is explicitly. An Aethro-Kinematic Description of Gravity This supposition is based on the uncertainty principle: A particle's position and speed can never be simultaneously measured with perfect accuracy. AN ALTERNATIVE THEORY FOR THE PERPLEXITIES OF MODERN THEORETICAL PHYSICS THE COSMOS OF THE ALL-PERVADING AETHER. Book 1: Aethro-kinematics. Copenhagen interpretation, book and CD-ROM. Understanding Einstein, physics without sophisticated mathematics, Doppler effect, Hubble's constant, expanding universe, Big-Bang, Aether rotation, & Aether vortex's. Double-quantum vortex in superfluid (He-3)-A. Source: CSA's SearchAbstracts, the World's Most Powerful Research Tool!

• Observe the kinematics of rotational motion.
• Derive rotational kinematic equations.
• Evaluate problem solving strategies for rotational kinematics.

Kinematics is the description of motion. The kinematics of rotational motion describes the relationships among rotation angle, angular velocity, angular acceleration, and time. Let us start by finding an equation relating ω, α, and t. To determine this equation, we recall a familiar kinematic equation for translational, or straight-line, motion:

[latex]v={v}_{0}+{at}[/latex] (constant a)

Note that in rotational motion a = a_t, and we shall use the symbol a for tangential or linear acceleration from now on. As in linear kinematics, we assume a is constant, which means that angular acceleration α is also a constant, because a = rα. Now, let us substitute v = rω and a = rα into the linear equation above:

rω =rω₀ + rat.

The radius r cancels in the equation, yielding

ω =ω₀ + at. (constant a)

where ω₀ is the initial angular velocity. This last equation is a kinematic relationship among ω, α, and t —that is, it describes their relationship without reference to forces or masses that may affect rotation. It is also precisely analogous in form to its translational counterpart.

Making Connections

Starting with the four kinematic equations we developed in One-Dimensional Kinematics, we can derive the following four rotational kinematic equations (presented together with their translational counterparts):

In these equations, the subscript 0 denotes initial values (θ₀, x₀, and t₀ are initial values), and the average angular velocity [latex]bar{omega}[/latex] and average velocity [latex]bar{v}[/latex] are defined as follows:

[latex]bar{omega}=frac{{omega }_{0}+omega }{2}text{ and }overline{v}=frac{{v}_{0}+v}{2}[/latex].

The equations given above in Table 1 can be used to solve any rotational or translational kinematics problem in which a and α are constant.

Problem-Solving Strategy for Rotational Kinematics

1. Examine the situation to determine that rotational kinematics (rotational motion) is involved. Rotation must be involved, but without the need to consider forces or masses that affect the motion.
2. Identify exactly what needs to be determined in the problem (identify the unknowns). A sketch of the situation is useful.
3. Make a list of what is given or can be inferred from the problem as stated (identify the knowns).
4. Solve the appropriate equation or equations for the quantity to be determined (the unknown). It can be useful to think in terms of a translational analog because by now you are familiar with such motion.
5. Substitute the known values along with their units into the appropriate equation, and obtain numerical solutions complete with units. Be sure to use units of radians for angles.
6. Check your answer to see if it is reasonable: Does your answer make sense?

Example 1. Calculating the Acceleration of a Fishing Reel

A deep-sea fisherman hooks a big fish that swims away from the boat pulling the fishing line from his fishing reel. The whole system is initially at rest and the fishing line unwinds from the reel at a radius of 4.50 cm from its axis of rotation. The reel is given an angular acceleration of 110 rad/s² for 2.00 s as seen in Figure 1. (a) What is the final angular velocity of the reel? (b) At what speed is fishing line leaving the reel after 2.00 s elapses? (c) How many revolutions does the reel make? (d) How many meters of fishing line come off the reel in this time?

Strategy

In each part of this example, the strategy is the same as it was for solving problems in linear kinematics. In particular, known values are identified and a relationship is then sought that can be used to solve for the unknown.

Solution for (a)

Here α and t are given and ω needs to be determined. The most straightforward equation to use is ω = ω₀+αt because the unknown is already on one side and all other terms are known. That equation states that

We are also given that ω₀ = 0 (it starts from rest), so that

ω = 0 + (110 rad/s²)(2.00 s) = 220 rad/s

Solution for (b)

Now that ω is known, the speed v can most easily be found using the relationship

where the radius r of the reel is given to be 4.50 cm; thus,

Note again that radians must always be used in any calculation relating linear and angular quantities. Also, because radians are dimensionless, we have m × rad = m .

Solution for (c)

Here, we are asked to find the number of revolutions. Because 1 rev=2π rad, we can find the number of revolutions by finding θ in radians. We are given α and t, and we know ω₀ is zero, so that θ can be obtained using [latex]theta = omega_{0}t+frac{1}{2}{{alpha t}}^{2}[/latex].

[latex]begin{array}{lll}theta &=& omega_{0}t+frac{1}{2}{{alpha t}}^{2} &=& 0+left(text{0.500}right)left(text{110}{text{rad/s}}^{2}right){left(text{2.00 s}right)}^{2}=text{220 rad}.end{array}[/latex]

Converting radians to revolutions gives

[latex]theta =(220 text{ rad})frac{1 text{ rev}}{2pi text{rad}}=35.0 text{ rev}[/latex]

Solution for (d)

The number of meters of fishing line is x, which can be obtained through its relationship with θ:

Discussion

This example illustrates that relationships among rotational quantities are highly analogous to those among linear quantities. We also see in this example how linear and rotational quantities are connected. The answers to the questions are realistic. After unwinding for two seconds, the reel is found to spin at 220 rad/s, which is 2100 rpm. (No wonder reels sometimes make high-pitched sounds.) The amount of fishing line played out is 9.90 m, about right for when the big fish bites.

Figure 1. Fishing line coming off a rotating reel moves linearly. Example 10.3 and Example 10.4 consider relationships between rotational and linear quantities associated with a fishing reel.

Example 2. Calculating the Duration When the Fishing Reel Slows Down and Stops

Now let us consider what happens if the fisherman applies a brake to the spinning reel, achieving an angular acceleration of -300 rad/s². How long does it take the reel to come to a stop?

Strategy

We are asked to find the time t for the reel to come to a stop. The initial and final conditions are different from those in the previous problem, which involved the same fishing reel. Now we see that the initial angular velocity is ω₀ = 220 rad/s and the final angular velocity ω is zero. The angular acceleration is given to be α = -300 rad/s². Examining the available equations, we see all quantities but t are known in ω = ω₀+αt, making it easiest to use this equation.

Solution

The equation states

ω = ω₀ + αt.

We solve the equation algebraically for t, and then substitute the known values as usual, yielding

[latex]t=frac{omega -{omega }_{0}}{alpha }=frac{0-text{220 rad/s}}{-text{300}{text{rad/s}}^{2}}=0text{.}text{733 s}[/latex].

Discussion

Note that care must be taken with the signs that indicate the directions of various quantities. Also, note that the time to stop the reel is fairly small because the acceleration is rather large. Fishing lines sometimes snap because of the accelerations involved, and fishermen often let the fish swim for a while before applying brakes on the reel. A tired fish will be slower, requiring a smaller acceleration.

Example 3. Calculating the Slow Acceleration of Trains and Their Wheels

Large freight trains accelerate very slowly. Suppose one such train accelerates from rest, giving its 0.350-m-radius wheels an angular acceleration of 0.250 rad/s². After the wheels have made 200 revolutions (assume no slippage): (a) How far has the train moved down the track? (b) What are the final angular velocity of the wheels and the linear velocity of the train?

Strategy

In part (a), we are asked to find x, and in (b) we are asked to find ω and v. We are given the number of revolutions θ, the radius of the wheels r, and the angular acceleration α.

Solution for (a)

The distance x is very easily found from the relationship between distance and rotation angle:

Solving this equation for x yields

x = rθ.

Before using this equation, we must convert the number of revolutions into radians, because we are dealing with a relationship between linear and rotational quantities:

[latex]theta =left(text{200}text{rev}right)frac{2pi text{rad}}{text{1 rev}}=text{1257}text{rad}[/latex].

Now we can substitute the known values into x=rθ to find the distance the train moved down the track:

x = rθ = (0.350 m)(1257 rad) = 440 m

Solution for (b)

We cannot use any equation that incorporates t to find ω, because the equation would have at least two unknown values. The equation [latex]{omega }^{2}={{omega }_{0}}^{2}+2alphatheta [/latex] will work, because we know the values for all variables except ω:

Arthrokinematics Of Knee Joint

[latex]{omega }^{2}={{omega }_{0}}^{2}+2alphatheta[/latex]

Taking the square root of this equation and entering the known values gives

[latex]begin{array}{lll}omega & =& {left[0+2left(0text{.}text{250}{text{ rad/s}}^{2}right)left(text{1257}text{ rad}right)right]}^{1/2} & =& text{25.1 rad/s.}end{array}[/latex]

We can find the linear velocity of the train, v, through its relationship to ω:

Arthrokinematics Def

Discussion

The distance traveled is fairly large and the final velocity is fairly slow (just under 32 km/h).

There is translational motion even for something spinning in place, as the following example illustrates. Figure 2 shows a fly on the edge of a rotating microwave oven plate. The example below calculates the total distance it travels.

Figure 2. The image shows a microwave plate. The fly makes revolutions while the food is heated (along with the fly).

Example 4. Calculating the Distance Traveled by a Fly on the Edge of a Microwave Oven Plate

A person decides to use a microwave oven to reheat some lunch. In the process, a fly accidentally flies into the microwave and lands on the outer edge of the rotating plate and remains there. If the plate has a radius of 0.15 m and rotates at 6.0 rpm, calculate the total distance traveled by the fly during a 2.0-min cooking period. (Ignore the start-up and slow-down times.)

Strategy

First, find the total number of revolutions θ, and then the linear distance x traveled.[latex]theta =bar{omega}t[/latex] can be used to find θ because [latex]bar{omega}[/latex] is given to be 6.0 rpm.

Solution

Entering known values into [latex]theta =bar{omega} t[/latex] gives

[latex]theta =bar{omega }t=left(text{6.0 rpm}right)left(text{2.0 min}right)=text{12 rev}[/latex].

As always, it is necessary to convert revolutions to radians before calculating a linear quantity like x from an angular quantity like θ:

[latex]theta =left(text{12 rev}right)left(frac{2pi text{rad}}{text{1 rev}}right)=75.4 text{ rad}[/latex].

Now, using the relationship between x and θ, we can determine the distance traveled:

Discussion

Quite a trip (if it survives)! Note that this distance is the total distance traveled by the fly. Displacement is actually zero for complete revolutions because they bring the fly back to its original position. The distinction between total distance traveled and displacement was first noted in One-Dimensional Kinematics.

Check Your Understanding

Solution

Rotational kinematics (just like linear kinematics) is descriptive and does not represent laws of nature. With kinematics, we can describe many things to great precision but kinematics does not consider causes. For example, a large angular acceleration describes a very rapid change in angular velocity without any consideration of its cause.

Section Summary

• Kinematics is the description of motion.
• The kinematics of rotational motion describes the relationships among rotation angle, angular velocity, angular acceleration, and time.
• Starting with the four kinematic equations we developed in the One-Dimensional Kinematics, we can derive the four rotational kinematic equations (presented together with their translational counterparts) seen in Table 1.
• In these equations, the subscript 0 denotes initial value ([latex]{x}_{0}[/latex] and [latex]{t}_{0}[/latex] are initial values), and the average angular velocity [latex]bar{omega}[/latex] and average velocity [latex]bar{v}[/latex] are defined as follows:
  [latex]bar{omega }=frac{{omega }_{0}+omega }{2}text{ and }bar{v}=frac{{v}_{0}+v}{2}[/latex].

Problems & Exercises

1. With the aid of a string, a gyroscope is accelerated from rest to 32 rad/s in 0.40 s. (a) What is its angular acceleration in rad/s²? (b) How many revolutions does it go through in the process?

2. Suppose a piece of dust finds itself on a CD. If the spin rate of the CD is 500 rpm, and the piece of dust is 4.3 cm from the center, what is the total distance traveled by the dust in 3 minutes? (Ignore accelerations due to getting the CD rotating.)

3. A gyroscope slows from an initial rate of 32.0 rad/s at a rate of 0.700 rad/s². (a) How long does it take to come to rest? (b) How many revolutions does it make before stopping?

4. During a very quick stop, a car decelerates at 700 m/s².

(a) What is the angular acceleration of its 0.280-m-radius tires, assuming they do not slip on the pavement?
(b) How many revolutions do the tires make before coming to rest, given their initial angular velocity is 95.0 rad/s?
(c) How long does the car take to stop completely?
(d) What distance does the car travel in this time?
(e) What was the car’s initial velocity?
(f) Do the values obtained seem reasonable, considering that this stop happens very quickly?

Figure 3. Yo-yos are amusing toys that display significant physics and are engineered to enhance performance based on physical laws. (credit: Beyond Neon, Flickr)

5. Everyday application: Suppose a yo-yo has a center shaft that has a 0.250 cm radius and that its string is being pulled.

(a) If the string is stationary and the yo-yo accelerates away from it at a rate of 1.50 m/s², what is the angular acceleration of the yo-yo?
(b) What is the angular velocity after 0.750 s if it starts from rest?
(c) The outside radius of the yo-yo is 3.50 cm. What is the tangential acceleration of a point on its edge?

Glossary

Arthrokinematics Of Talocrural Joint

kinematics of rotational motion:

describes the relationships among rotation angle, angular velocity, angular acceleration, and time

Selected Solutions to Problems & Exercises

Arthrokinematics Spin

1. (a) [latex]80{text{rad/s}}^{2}[/latex] (b) 1.0 rev

3. (a) 45.7 s (b) 116 rev

Aethro-kinematics

5. (a) 600 rad/s² (b) 450 rad/s (c) 21.0 m/s

The kinematics of the 'Magnetic Field': The Bar Magnet
Symmetrically aligned sink-source flow of electrons produces the distinct flowlines that correspond exactly with a
Atoms page to understand the kinematics of a
others' individual sink-source flows. Thus, a magnet acts like a giant electron—that is, a magnet's induced sink-source
linking them in a way similar to that of a proton and neutron.