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The Simple Pendulum

Module by: OpenStax College. E-mail the author

Summary:

  • Measure acceleration due to gravity.

Figure 1: A simple pendulum has a small-diameter bob and a string that has a very small mass but is strong enough not to stretch appreciably. The linear displacement from equilibrium is ss size 12{s} {}, the length of the arc. Also shown are the forces on the bob, which result in a net force of mg sinθmg sinθ size 12{ - ital "mg""sin"θ} {} toward the equilibrium position—that is, a restoring force.
In the figure, a horizontal bar is drawn. A perpendicular dotted line from the middle of the bar, depicting the equilibrium of pendulum, is drawn downward. A string of length L is tied to the bar at the equilibrium point. A circular bob of mass m is tied to the end of the string which is at a distance s from the equilibrium. The string is at an angle of theta with the equilibrium at the bar. A red arrow showing the time T of the oscillation of the mob is shown along the string line toward the bar. An arrow from the bob toward the equilibrium shows its restoring force asm g sine theta. A perpendicular arrow from the bob toward the ground depicts its mass as W equals to mg, and this arrow is at an angle theta with downward direction of string.

Pendulums are in common usage. Some have crucial uses, such as in clocks; some are for fun, such as a child’s swing; and some are just there, such as the sinker on a fishing line. For small displacements, a pendulum is a simple harmonic oscillator. A simple pendulum is defined to have an object that has a small mass, also known as the pendulum bob, which is suspended from a light wire or string, such as shown in Figure 1. Exploring the simple pendulum a bit further, we can discover the conditions under which it performs simple harmonic motion, and we can derive an interesting expression for its period.

We begin by defining the displacement to be the arc length ss size 12{s} {}. We see from Figure 1 that the net force on the bob is tangent to the arc and equals mgsinθmgsinθ size 12{ - ital "mg""sin"θ} {}. (The weight mgmg size 12{ ital "mg"} {} has components mgcosθmgcosθ size 12{ ital "mg""cos"θ} {} along the string and mgsinθmgsinθ size 12{ ital "mg""sin"θ} {} tangent to the arc.) Tension in the string exactly cancels the component mgcosθmgcosθ size 12{ ital "mg""cos"θ} {} parallel to the string. This leaves a net restoring force back toward the equilibrium position at θ=0θ=0 size 12{θ=0} {}.

Now, if we can show that the restoring force is directly proportional to the displacement, then we have a simple harmonic oscillator. In trying to determine if we have a simple harmonic oscillator, we should note that for small angles (less than about 15º15º size 12{"15"°} {}), sinθθsinθθ size 12{"sin"θ approx θ} {}(sinθsinθ size 12{"sin"θ} {} and θθ size 12{θ} {} differ by about 1% or less at smaller angles). Thus, for angles less than about 15º15º size 12{"15"°} {}, the restoring force FF size 12{F} {} is

F mg θ. F mg θ. size 12{F= - ital "mg"θ} {}
(1)

The displacement ss size 12{s} {} is directly proportional to θθ size 12{θ} {}. When θθ size 12{θ} {} is expressed in radians, the arc length in a circle is related to its radius (LL size 12{L} {} in this instance) by:

s = , s = , size 12{s=Lθ} {}
(2)

so that

θ = s L . θ = s L . size 12{θ= { {s} over {L} } } {}
(3)

For small angles, then, the expression for the restoring force is:

F mg L s F mg L s size 12{F approx - { { ital "mg"} over {L} } s} {}
(4)

This expression is of the form:

F = kx , F = kx , size 12{F= - ital "kx"} {}
(5)

where the force constant is given by k=mg/Lk=mg/L and the displacement is given by x=sx=s size 12{x=s} {}. For angles less than about 15º15º, the restoring force is directly proportional to the displacement, and the simple pendulum is a simple harmonic oscillator.

Using this equation, we can find the period of a pendulum for amplitudes less than about 15º15º. For the simple pendulum:

T = m k = m mg / L . T = m k = m mg / L . size 12{T=2π sqrt { { {m} over {k} } } =2π sqrt { { {m} over { ital "mg"/L} } } } {}
(6)

Thus,

T = L g T = L g size 12{T=2π sqrt { { {L} over {g} } } } {}
(7)

for the period of a simple pendulum. This result is interesting because of its simplicity. The only things that affect the period of a simple pendulum are its length and the acceleration due to gravity. The period is completely independent of other factors, such as mass. As with simple harmonic oscillators, the period TT size 12{T} {} for a pendulum is nearly independent of amplitude, especially if θθ size 12{θ} {} is less than about 15º15º size 12{"15"°} {}. Even simple pendulum clocks can be finely adjusted and accurate.

Note the dependence of TT size 12{T} {} on gg size 12{g} {}. If the length of a pendulum is precisely known, it can actually be used to measure the acceleration due to gravity. Consider the following example.

Example 1: Measuring Acceleration due to Gravity: The Period of a Pendulum

What is the acceleration due to gravity in a region where a simple pendulum having a length 75.000 cm has a period of 1.7357 s?

Strategy

We are asked to find gg size 12{g} {} given the period TT size 12{T} {} and the length LL size 12{L} {} of a pendulum. We can solve T=LgT=Lg size 12{T=2π sqrt { { {L} over {g} } } } {} for gg size 12{g} {}, assuming only that the angle of deflection is less than 15º15º size 12{"15º"} {}.

Solution

  1. Square T=LgT=Lg size 12{T=2π sqrt { { {L} over {g} } } } {} and solve for gg size 12{g} {}:
    g = 2 L T 2 . g = 2 L T 2 . size 12{g=4π rSup { size 8{2} } { {L} over {T rSup { size 8{2} } } } } {}
    (8)
  2. Substitute known values into the new equation:
    g = 2 0 . 75000 m 1 . 7357 s 2 . g = 2 0 . 75000 m 1 . 7357 s 2 . size 12{g=4π rSup { size 8{2} } { {0 "." "75000"" m"} over { left (1 "." "7357 s" right ) rSup { size 8{2} } } } } {}
    (9)
  3. Calculate to find gg size 12{g} {}:
    g = 9 . 8281 m / s 2 . g = 9 . 8281 m / s 2 . size 12{g=9 "." "828"m/s rSup { size 8{2} } } {}
    (10)

Discussion

This method for determining g g g can be very accurate. This is why length and period are given to five digits in this example. For the precision of the approximation sin θ θ sin θ θ size 12{"sin"θ approx θ} {} to be better than the precision of the pendulum length and period, the maximum displacement angle should be kept below about 0.5º 0.5º size 12{0 "." 5°} {} .

Making Career Connections:

Knowing g g g can be important in geological exploration; for example, a map of gg size 12{g} {} over large geographical regions aids the study of plate tectonics and helps in the search for oil fields and large mineral deposits.

Take Home Experiment: Determining g g g :

Use a simple pendulum to determine the acceleration due to gravity g g g in your own locale. Cut a piece of a string or dental floss so that it is about 1 m long. Attach a small object of high density to the end of the string (for example, a metal nut or a car key). Starting at an angle of less than 10º10º size 12{"10"°} {}, allow the pendulum to swing and measure the pendulum’s period for 10 oscillations using a stopwatch. Calculate gg size 12{g} {}. How accurate is this measurement? How might it be improved?

Check Your Understanding

An engineer builds two simple pendula. Both are suspended from small wires secured to the ceiling of a room. Each pendulum hovers 2 cm above the floor. Pendulum 1 has a bob with a mass of 10kg10kg size 12{"10"`"kg"} {}. Pendulum 2 has a bob with a mass of 100 kg100 kg size 12{"100"`"kg"} {}. Describe how the motion of the pendula will differ if the bobs are both displaced by 12º12º size 12{"12"°} {}.

PhET Explorations: Pendulum Lab:

Play with one or two pendulums and discover how the period of a simple pendulum depends on the length of the string, the mass of the pendulum bob, and the amplitude of the swing. It’s easy to measure the period using the photogate timer. You can vary friction and the strength of gravity. Use the pendulum to find the value of gg on planet X. Notice the anharmonic behavior at large amplitude.

Figure 2: Pendulum Lab
Figure 2 (pendulum-lab_en.jar)

Section Summary

  • A mass mm size 12{m} {} suspended by a wire of length LL size 12{L} {} is a simple pendulum and undergoes simple harmonic motion for amplitudes less than about 15º.15º size 12{"15"°} {}.

    The period of a simple pendulum is

    T=Lg,T=Lg, size 12{T=2π sqrt { { {L} over {g} } } } {}
    (11)

    where LL size 12{L} {} is the length of the string and gg is the acceleration due to gravity.

Conceptual Questions

Exercise 1

Pendulum clocks are made to run at the correct rate by adjusting the pendulum’s length. Suppose you move from one city to another where the acceleration due to gravity is slightly greater, taking your pendulum clock with you, will you have to lengthen or shorten the pendulum to keep the correct time, other factors remaining constant? Explain your answer.

Problems & Exercises

As usual, the acceleration due to gravity in these problems is taken to be g=9.80m/s2g=9.80m/s2, unless otherwise specified.

Exercise 1

What is the length of a pendulum that has a period of 0.500 s?

Exercise 2

Some people think a pendulum with a period of 1.00 s can be driven with “mental energy” or psycho kinetically, because its period is the same as an average heartbeat. True or not, what is the length of such a pendulum?

Exercise 3

What is the period of a 1.00-m-long pendulum?

Exercise 4

How long does it take a child on a swing to complete one swing if her center of gravity is 4.00 m below the pivot?

Exercise 5

The pendulum on a cuckoo clock is 5.00 cm long. What is its frequency?

Exercise 6

Two parakeets sit on a swing with their combined center of mass 10.0 cm below the pivot. At what frequency do they swing?

Exercise 7

(a) A pendulum that has a period of 3.00000 s and that is located where the acceleration due to gravity is 9.79m/s29.79m/s2 size 12{9 "." "79"`"m/s" rSup { size 8{2} } } {} is moved to a location where it the acceleration due to gravity is 9.82m/s29.82m/s2 size 12{9 "." "82"`"m/s" rSup { size 8{2} } } {}. What is its new period? (b) Explain why so many digits are needed in the value for the period, based on the relation between the period and the acceleration due to gravity.

Exercise 8

A pendulum with a period of 2.00000 s in one location (g=9.80m/s2)(g=9.80m/s2 size 12{g=9 "." "80"`"m/s" rSup { size 8{2} } } {}) is moved to a new location where the period is now 1.99796 s. What is the acceleration due to gravity at its new location?

Exercise 9

(a) What is the effect on the period of a pendulum if you double its length?

(b) What is the effect on the period of a pendulum if you decrease its length by 5.00%?

Exercise 10

Find the ratio of the new/old periods of a pendulum if the pendulum were transported from Earth to the Moon, where the acceleration due to gravity is 1.63m/s21.63m/s2 size 12{1 "." "63"`"m/s" rSup { size 8{2} } } {}.

Exercise 11

At what rate will a pendulum clock run on the Moon, where the acceleration due to gravity is 1.63m/s21.63m/s2 size 12{1 "." "63"`"m/s" rSup { size 8{2} } } {}, if it keeps time accurately on Earth? That is, find the time (in hours) it takes the clock’s hour hand to make one revolution on the Moon.

Exercise 12

Suppose the length of a clock’s pendulum is changed by 1.000%, exactly at noon one day. What time will it read 24.00 hours later, assuming it the pendulum has kept perfect time before the change? Note that there are two answers, and perform the calculation to four-digit precision.

Exercise 13

If a pendulum-driven clock gains 5.00 s/day, what fractional change in pendulum length must be made for it to keep perfect time?

Glossary

simple pendulum:
an object with a small mass suspended from a light wire or string

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