*Notes to a video lecture on http://www.unizor.com*

__Periodic Movement__

Mechanics, as a subject, deals with movements of different objects. Among these movements there are those that we can call "repetitive". Examples of these repetitive movements, occurring during certain time segment, are rotation of a carousel, swinging of a pendulum, vibration of a musical tuning fork, etc. Here we are talking about certain time segment during which these movements are repetitive, because after some time these movements are changing, if left to themselves.

These repetitive movements might be of a kind when the repetitions are to a high degree exactly similar to each other (like in case of a pendulum) or some of the characteristics of the motion change in time (like in case of a tuning fork).

Repetitive movements that can be divided into equal time segments, during which the movements to a high precision repeat exactly each other, are called

*periodic*.

The time segments of such a repetitive movement are called

*periods*.

If a position

*of an object making periodic movement with a period*

**P***is defined by a set of Cartesian coordinates*

**T***as a vector function of time*

**P=(x**,**y**,**z)***, the periodicity means that for any time moment*

**P(t)**

**t**

**P(t) = P(t+T)**which is exactly the mathematical definition of a periodic function.

For example, a

*period*of rotational movement of a carousel equals to a time it takes to make one circle. The period of a movement of a pendulum is the time it moves from left most position all the way to the right most and back to the left.

A case of a vibrating tuning fork is a bit more complex because gradually the vibrations, after being initiated, diminish with time. The

*period*of vibration might be the same during this process, but the amplitude (deviation from a middle point) would diminish with time.

A special type of

*periodic*movement is

*oscillation*. It's characterized by a periodic movement of an object that repeats the same trajectory of movement in alternating directions, back and forth. For example, a pendulum, an object on a spring, a tuning fork, a buoy on a surface of water under ideal weather conditions etc.

In all those systems we can observe a specific middle point position from which an object can deviate in both directions. If put initially at this position, an object would remain there, unless some external force acts on it. This is a point of a

*stable equilibrium*. Then, after some external force is applied, it will move along its trajectory back and forth, each time passing this

*equilibrium*point.

From this point an object can move along a trajectory to some extreme position, then back through an

*equilibrium*point to another extreme position, then back again, repeating a movement along the same trajectory in alternating directions.

*Oscillation*is only possible if some external forces act on a moving object towards

*stable equilibrium*point. Otherwise, it would never return to an

*equilibrium*. These forces must depend on the position, not acting at the equilibrium point, acting in one direction in case an object deviated from an equilibrium to one side along its trajectory and acting in the opposite direction in case an object deviated to the other side along a trajectory.

A very important type of

*oscillations*are so-called

*harmonic oscillations*.

An example of this type of a movement is an object on an initially stretched (or squeezed) spring with the only force acting on an object during its movement to be the spring's elasticity.

According to the Hooke's Law, the force of elasticity of a spring is proportional to its stretch or squeeze length and directed towards a neutral point of no stretch nor squeeze.

If a string is positioned along the X-axis on a Cartesian system of coordinates with one end fixed to some point with negative coordinate on this axis, while its neutral point at

*, the position of an object attached to this spring and oscillating can be described as a function of time*

**x=0***that satisfies two laws:*

**x(t)**(1) the Second Newton's Law connecting the force of elasticity

*to the*

**F(t)****mass**

*and acceleration (second derivative of position)*

**m**

**F(t) = m·x"(t) = m·**d²**x(t)/**d**x²**(2) the Hooke's Law connecting the force of elasticity

*with a displacement of a free end of a spring from its neutral position*

**F**

**F(t) = −k·x(t)**(where

*is a*

**k****coefficient of elasticity**that is a characteristic of a spring).

From these two equations we can exclude the force

*and get a simple differential equation that defines the position of an object at the free end of a spring*

**F(t)***.*

**x(t)**

**m·x"(t) = m·**d²**x(t)/**d**x² = −k·x(t)**or

**x"(t) = −(k/m)·x(t)**Obviously, trigonometric functions

*sin(t)*and

*cos(t)*are good candidates for a solution to this equation since their second derivative looks like the original function with some coefficients

**sin"(t) = -sin(t)**

**cos"(t) = -cos(t)**General solution to the above linear differential equation is

**x(t) = C**_{1}·cos(ωt) + C_{2}·sin(ωt)where

*depends on coefficients of the differential equation and constants*

**ω***and*

**C**_{1}*depend on initial conditions (initial displacement of the object off the neutral position on a spring and its initial speed).*

**C**_{2}Then

**x'(t) = −C**

+ C_{1}·ω·sin(ωt) ++ C

_{2}·ω·cos(ωt)

**x"(t) = −C**

− C_{1}·ω²·cos(ωt) −− C

_{2}·ω²·sin(ωt)Since

**x"(t) = −(k/m)·x(t)**we conclude that

**−(k/m)·x(t) = −C**

− C_{1}·ω²·cos(ωt) −− C

_{2}·ω²·sin(ωt)or

**−(k/m)·[C**

+ C

−C

− C_{1}·cos(ωt) ++ C

_{2}·sin(ωt)] =−C

_{1}·ω²·cos(ωt) −− C

_{2}·ω²·sin(ωt)from which immediately follows

**ω = √k/m**Assume, initially we stretch a spring by a distance

*from the neutral position (that is,*

**a***) and let it go without any push (that is,*

**x(0)=a***).*

**x'(0)=0**From these initial conditions we can derive the values of constants

*and*

**C**_{1}

**C**_{2}

**a = x(0) =**

= C= C

_{1}·cos(0) + C_{2}·sin(0) = C_{1}

**0 = x'(0) =**

= −C

= C= −C

_{1}·ω·sin(0) + C_{2}·ω·cos(0) == C

_{2}·ωfrom which immediately follows

**C**_{1}= a

**C**_{2}= 0and the solution for our differential equation with given initial conditions is

**x(t) = a·cos(√k/m·t)**The oscillations described by the above function

*in its general form*

**x(t)***are called*

**x(t)=a·cos(ω·t)***simple harmonic oscillations*.

Parameter

*characterizes the*

**a****amplitude**of harmonic oscillations, while parameter

**ω**represents the

**angular speed**of oscillations.

Function

*cos(t)*is periodical with a period

*T=2π*.

Function

*cos(ωt)*is also periodical with a period

*T=2π/ω*.

Indeed,

*cos(ω(t+T)) =*

= cos(ω(t+2π/ω)) =

= cos(ωt+2π) =

= cos(ωt)

= cos(ω(t+2π/ω)) =

= cos(ωt+2π) =

= cos(ωt)

Therefore, the simple harmonic oscillations in our case have a period (the shortest time the object returns to its original position)

**T = 2π/ω = 2π·√m/k**If one full cycle the oscillation process makes in time

*T*, we can find how many cycles it makes in a unit of time (1 sec) using a simple proportion

*1*cycle -

*T*sec

*f*cycles -

*1*sec

Hence,

*f = 1/T*

Therefore, the object on a spring we deal with makes

**f = 1/T = (1/2π)·√k/m**oscillations per second.

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