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A \(1.50-\mathrm{m}\) -long rope is stretched between two supports with a tension that makes the speed of transverse waves \(62.0 \mathrm{~m} / \mathrm{s}\). What are the wavelength and frequency of (a) the fundamental; (b) the second overtone; (c) the fourth harmonic?

Short Answer

Expert verified
The wavelength and frequency of the fundamental are \(3.00\, m\) and \(20.7\, Hz\), of the second overtone-\(2.00\, m\) and \(31.0\, Hz\) and of the fourth harmonic-\(0.75\, m\) and \(82.7\, Hz\). These values are found using the relationship \(v = f\lambda\) and knowing the harmonic number.

Step by step solution

01

Fundamental Frequency

The speed of the wave is given by \(v = f \lambda\), where \(f\) is the frequency and \(\lambda\) is the wavelength. For a string of length \(L\), the fundamental wavelength is \(\lambda = 2L\). Using this, we can find the fundamental frequency as \(f = v / \lambda = v / 2L\). Here, \(v = 62.0 \, m/s\) and \(L = 1.50\, m\).
02

Second Overtone

The second overtone is the third harmonic for a string fixed at both ends. So, it corresponds to \(3f\), where \(f\) is the fundamental frequency. Similarly, its wavelength is \(\lambda = 2L/3\).
03

Fourth Harmonic

The fourth harmonic is simply \(4f\), where \(f\) is the fundamental frequency. Its wavelength is \(\lambda = 2L/4\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Transverse Waves
Transverse waves are waves where the motion of the medium is perpendicular to the direction of the wave. Imagine a snake moving side to side while slithering forward; that side-to-side motion is similar to what happens in a transverse wave. In physics, these waves are common in materials like strings or ropes.

When a transverse wave travels through a rope, each portion of the rope moves up and down while the wave itself travels horizontally. Such waves are characterized by peaks (crests) and valleys (troughs), like the waves you might see on the surface of the ocean.

Important characteristics of transverse waves include:
  • Amplitude: The height of a wave crest or depth of a trough, measuring how far the medium moves from its place of rest.
  • Velocity: The speed at which the wave travels through the medium, determined by the tension and mass of the medium in the case of a rope.
  • Length: Simply the distance between two consecutive crests or troughs.
Harmonics
In wave motion, harmonics refer to specific patterns of vibration that occur at particular frequencies. These are seen in systems like strings, which can vibrate at multiple frequencies.

Fundamental Frequency: It's the lowest frequency at which the system vibrates. It's also called the first harmonic.

The fundamental wavelength for a string fixed at both ends is given by \[ \lambda = 2L \]where \(L\) is the length of the string.

Overtones and Higher Harmonics: After the fundamental, the next possible vibrations occur at higher frequencies called overtones or higher harmonics. They have nodes where the string appears motionless.

Each harmonic can be numbered:
  • Second Harmonic: The first overtone, frequency is twice the fundamental.
  • Third Harmonic: Second overtone, frequency is three times the fundamental.
  • Fourth Harmonic: Third overtone, frequency is four times the fundamental.
Harmonics are important in many applications, such as music and acoustics, since they determine the richness of sounds.
Wave Frequency
Frequency refers to the number of waves that pass a fixed point in a unit of time, typically measured in hertz (Hz), where 1 Hz equals one wave per second. In the context of transverse waves on a rope, the frequency is the number of complete vibrations per second.

For a wave traveling along a string, the frequency equation is:\[f = \frac{v}{\lambda}\]where \(v\) is the wave speed and \(\lambda\) is the wavelength. The frequency changes depending on harmonic as it multiples of the fundamental level.

When considering harmonics on a string, the fundamental frequency is the lowest, and it increases with higher harmonics. Each subsequent harmonic vibration has a frequency that is an integer multiple of the fundamental frequency.

In music, different frequencies can determine the pitch of a sound. Higher frequencies correspond to higher pitches.
Wavelength
Wavelength is a fundamental property of waves that measures the distance over which the wave's shape repeats. For example, in a transverse wave on a rope, the distance between two consecutive crests or troughs is the wavelength, often denoted by \(\lambda\).

In the context of waves on a rope, the formula for wavelength is tied to the length of the rope and how the wave fits into it. The fundamental wavelength for a rope fixed at both ends is:\[\lambda = 2L\]For higher harmonics, the wavelength changes since the wave pattern adjusts to include more nodes. For example:
  • Second harmonic: \(\lambda = L \), meaning the wave fits two times into the rope length.
  • Third harmonic: \(\lambda = \frac{2L}{3} \), meaning three waves fit over the length.
Wavelength is inversely related to frequency. That means a higher frequency results in a shorter wavelength and vice versa. This is crucial for sound waves and other wave phenomena in understanding how waves interact with environments.

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Most popular questions from this chapter

A transverse sine wave with an amplitude of \(2.50 \mathrm{~mm}\) and a wavelength of \(1.80 \mathrm{~m}\) travels from left to right along a long, horizontal, stretched string with a speed of \(36.0 \mathrm{~m} / \mathrm{s}\). Take the origin at the left end of the undisturbed string. At time \(t=0\) the left end of the string has its maximum upward displacement. (a) What are the frequency, angular frequency, and wave number of the wave? (b) What is the function \(y(x, t)\) that describes the wave? (c) What is \(y(t)\) for a particle at the left end of the string? (d) What is \(y(t)\) for a particle \(1.35 \mathrm{~m}\) to the right of the origin? (e) What is the maximum magnitude of transverse velocity of any particle of the string? (f) Find the transverse displacement and the transverse velocity of a particle \(1.35 \mathrm{~m}\) to the right of the origin at time \(t=0.0625 \mathrm{~s}\)

A transverse wave on a rope is given by $$ y(x, t)=(0.750 \mathrm{~cm}) \cos \pi\left[\left(0.400 \mathrm{~cm}^{-1}\right) x+\left(250 \mathrm{~s}^{-1}\right) t\right] $$ (a) Find the amplitude, period, frequency, wavelength, and speed of propagation. (b) Sketch the shape of the rope at these values of \(t: 0,\) \(0.0005 \mathrm{~s}, 0.0010 \mathrm{~s} .\) (c) Is the wave traveling in the \(+x\) - or \(-x\) -direction? (d) The mass per unit length of the rope is \(0.0500 \mathrm{~kg} / \mathrm{m}\). Find the tension. (e) Find the average power of this wave.

For a violin, estimate the length of the portions of the strings that are free to vibrate. (a) The frequency of the note played by the open E5 string vibrating in its fundamental standing wave is 659 Hz. Use your estimate of the length to calculate the wave speed for the transverse waves on the string. (b) The vibrating string produces sound waves in air with the same frequency as that of the string. Use \(344 \mathrm{~m} / \mathrm{s}\) for the speed of sound in air and calculate the wavelength of the E5 note in air. Which is larger: the wavelength on the string or the wavelength in air? (c) Repeat parts (a) and (b) for a bass viol, which is typically played by a person standing up. Start your calculation by estimating the length of the bass viol string that is free to vibrate. The G2 string produces a note with frequency \(98 \mathrm{~Hz}\) when vibrating in its fundamental standing wave.

A large rock that weighs \(164.0 \mathrm{~N}\) is suspended from the lower end of a thin wire that is \(3.00 \mathrm{~m}\) long. The density of the rock is \(3200 \mathrm{~kg} / \mathrm{m}^{3} .\) The mass of the wire is small enough that its effect on the tension in the wire can be ignored. The upper end of the wire is held fixed. When the rock is in air, the fundamental frequency for transverse standing waves on the wire is \(42.0 \mathrm{~Hz}\). When the rock is totally submerged in a liquid, with the top of the rock just below the surface, the fundamental frequency for the wire is \(28.0 \mathrm{~Hz}\). What is the density of the liquid?

You are designing a two-string instrument with metal strings \(35.0 \mathrm{~cm}\) long, as shown in Fig. \(\mathrm{P} 15.52 .\) Both strings are under the same tension. String \(S_{1}\) has a mass of \(8.00 \mathrm{~g}\) and produces the note middle \(\mathrm{C}\) (frequency \(262 \mathrm{~Hz}\) ) in its fundamental mode. (a) What should be the tension in the string? (b) What should be the mass of string \(S_{2}\) so that it will produce A-sharp (frequency \(466 \mathrm{~Hz}\) ) as its fundamental? (c) To extend the range of your instrument, you include a fret located just under the strings but not normally touching them. How far from the upper end should you put this fret so that when you press \(S_{1}\) tightly against it, this string will produce \(\mathrm{C}\) -sharp (frequency \(277 \mathrm{~Hz}\) ) in its fundamental? That is, what is \(x\) in the figure? (d) If you press \(S_{2}\) against the fret, what frequency of sound will it produce in its fundamental?

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