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15 • Oscillatory Motion - ECHSPhysics

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The inverse of the period is called the frequency f of the motion. Whereas the period<br />

is the time interval per oscillation, the frequency represents the number of oscillations<br />

that the particle undergoes per unit time interval:<br />

(<strong>15</strong>.11)<br />

The units of f are cycles per second, or hertz (Hz). Rearranging Equation <strong>15</strong>.11 gives<br />

(<strong>15</strong>.12)<br />

We can use Equations <strong>15</strong>.9, <strong>15</strong>.10, and <strong>15</strong>.11 to express the period and frequency of<br />

the motion for the particle–spring system in terms of the characteristics m and k of the<br />

system as<br />

(<strong>15</strong>.13)<br />

(<strong>15</strong>.14)<br />

That is, the period and frequency depend only on the mass of the particle and the<br />

force constant of the spring, and not on the parameters of the motion, such as A or .<br />

As we might expect, the frequency is larger for a stiffer spring (larger value of k) and<br />

decreases with increasing mass of the particle.<br />

We can obtain the velocity and acceleration 2 of a particle undergoing simple harmonic<br />

motion from Equations <strong>15</strong>.7 and <strong>15</strong>.8:<br />

v dx<br />

dt<br />

f 1<br />

T<br />

T 2<br />

f 1<br />

T<br />

1<br />

<br />

2f 2<br />

2 √ m<br />

2 √ k<br />

A sin(t )<br />

a d 2 x<br />

dt 2 2 A cos(t )<br />

(<strong>15</strong>.<strong>15</strong>)<br />

(<strong>15</strong>.16)<br />

From Equation <strong>15</strong>.<strong>15</strong> we see that, because the sine and cosine functions oscillate<br />

between 1, the extreme values of the velocity v are A. Likewise, Equation <strong>15</strong>.16<br />

tells us that the extreme values of the acceleration a are 2 A. Therefore, the maximum<br />

values of the magnitudes of the velocity and acceleration are<br />

v max A √ k<br />

m A<br />

a max 2 A k<br />

m A<br />

(<strong>15</strong>.17)<br />

(<strong>15</strong>.18)<br />

Figure <strong>15</strong>.6a plots position versus time for an arbitrary value of the phase constant.<br />

The associated velocity–time and acceleration–time curves are illustrated in Figures<br />

<strong>15</strong>.6b and <strong>15</strong>.6c. They show that the phase of the velocity differs from the phase of the<br />

position by /2 rad, or 90°. That is, when x is a maximum or a minimum, the velocity<br />

is zero. Likewise, when x is zero, the speed is a maximum. Furthermore, note that the<br />

2 Because the motion of a simple harmonic oscillator takes place in one dimension, we will denote<br />

velocity as v and acceleration as a, with the direction indicated by a positive or negative sign, as in<br />

Chapter 2.<br />

2<br />

T<br />

k<br />

m<br />

SECTION <strong>15</strong>.2 <strong>•</strong> Mathematical Representation of Simple Harmonic <strong>Motion</strong> 457<br />

▲ PITFALL PREVENTION<br />

<strong>15</strong>.4 Two Kinds of<br />

Frequency<br />

We identify two kinds of frequency<br />

for a simple harmonic oscillator—f,<br />

called simply the frequency,<br />

is measured in hertz, and<br />

, the angular frequency, is measured<br />

in radians per second. Be<br />

sure that you are clear about<br />

which frequency is being discussed<br />

or requested in a given<br />

problem. Equations <strong>15</strong>.11 and<br />

<strong>15</strong>.12 show the relationship between<br />

the two frequencies.<br />

Period<br />

Frequency<br />

Velocity of an object in simple<br />

harmonic motion<br />

Acceleration of an object in<br />

simple harmonic motion<br />

Maximum magnitudes of speed<br />

and acceleration in simple<br />

harmonic motion

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