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Good morning, class! Today weβre going to dive into the speed of travelling waves. Can anyone tell me how we might measure the speed of a wave?
Is it by measuring how fast it travels from one point to another?
Exactly right! We generally measure it by looking at a specific point on the wave, usually where the crest is, and observing how far it travels over a specific time.
How do we actually calculate that then?
Great question! The formula we use is speed equals distance divided by time, or v = Ξx/Ξt. This helps us determine the speed of the wave if we know how far it moved in a certain time.
So, if we look at the equation, are there other factors that affect wave speed?
Yes, absolutely! The wave speed also incorporates the wavelength and frequency related through the equation v = λν. Weβll explore how different mediums influence speeds shortly.
That sounds interesting!
To sum up, we see how measuring the wave's distance and time helps identify its speed. Remember, the wave speed varies with the medium due to its unique properties. Let's proceed to see how this is applied in different contexts.
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Now, letβs talk about two important factors that affect wave speed: tension and mass density. Can you guess how these might change the speed of a wave on a string?
If the tension increases, I think the wave speed increases too?
Exactly! Higher tension means greater restoring force, which translates to a faster wave speed. The formula for a transverse wave on a string is v = β(T/ΞΌ). Can anyone explain what ΞΌ represents?
I believe ΞΌ is the linear mass density of the string.
Correct! So, higher mass density means slower wave speed. Now, can someone compare this with how sound waves travel through air?
For sound, it depends on the bulk modulus and the density of the air, right?
Absolutely! The speed of sound can be calculated using v = β(B/Ο), where B is the bulk modulus. Thus, heavier gases will typically slow sound down.
This shows why sound travels faster through solids than through gases!
Exactly! Just remember: tension and density play crucial roles in determining the speed of a wave in any medium. Letβs move on to how we derive these formulas!
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Letβs connect everything by estimating the speed of sound in gases. To find this speed, we use the formula v = β(Ξ³P/Ο). Can anyone break down what each of those variables means?
I think Ξ³ is the ratio of specific heats, P is the pressure, and Ο is the density of the gas?
Exactly right! This formula tells us how sound speed is affected by gas properties and shows why sound travels faster in hot air compared to cold air.
So, higher temperatures mean lower density?
Precisely! Warmer air has molecules moving faster, reducing density while increasing sound speed. Can anyone give a practical example of this?
Maybe when we hear distant thunder? The speed of sound is faster in the warmer air near the ground.
Spot on! Never forget the real-life applications of these wave concepts. In conclusion, remember that wave speeds are influenced by both density and tension in strings and the characteristics of air or gas for sound waves.
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The speed of a traveling wave is analyzed by fixing attention on a point on the wave and examining its motion over time. The relationship between wave speed, frequency, and wavelength is defined, alongside specific expressions for waves in strings and longitudinal waves in fluids.
In this section, we explore the concept of wave speed, which is the speed at which a wave propagates through a medium. The speed of a wave can be derived by observing a specific point of the wave, typically the crest, and noting its movement over time.
Key Points:
1. Wave Speed Calculation: If we observe a point moving with a fixed phase on the wave (denoted by the relationship kx - Οt = constant), we can derive the wave speed as the ratio of the distance traveled (βx ) to the time taken ( 08βt 09), leading to the equation
\[ v = \frac{\Delta x}{\Delta t} = \frac{\omega}{k} \]
where Ο represents the angular frequency and k is the angular wave number.
Here, Ξ» is the wavelength, and Ξ½ represents the frequency of the wave.
This section serves as a fundamental basis for understanding wave dynamics and their propagation characteristics.
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To determine the speed of propagation of a travelling wave, we can fix our attention on any particular point on the wave (characterised by some value of the phase) and see how that point moves in time. It is convenient to look at the motion of the crest of the wave. Fig. 14.8 gives the shape of the wave at two instants of time, which differ by a small time interval βt. The entire wave pattern is seen to shift to the right (positive direction of x-axis) by a distance βx. In particular, the crest shown by a dot (β’) moves a distance βx in time βt. The speed of the wave is then βx/βt.
When we want to understand how fast a wave travels, we focus on a specific point on the wave, often the crest. By observing the wave at two different times, we see how far that crest has moved in a very short duration (βt). The distance the crest moves during that time (βx) gives us the speed of the wave when we divide the distance by the time.
Think of a floating leaf on a wave in a pond. If you watched the leaf for a short time, youβd see it rise and fall as the wave passes, but if you measured how far it moved horizontally across the surface, youβd get a sense of the wave's speed.
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The motion of a fixed phase point on the wave is given by kx β Οt = constant (14.10). Thus, as time t changes, the position x of the fixed phase point must change so that the phase remains constant. Thus, kx β Οt = k(x+βx) β Ο(t+βt) or kβx β Οβt = 0 Taking βx, βt vanishingly small, this gives Ο = v k.
To understand wave motion mathematically, we can use the equation kx β Οt = constant. Here, k represents the wave number, and Ο is the angular frequency. This equation implies that as time changes, the position of a wave point also changes to keep the wave pattern consistent. By taking the limits as the shifts become infinitesimally small, we find a relationship where the speed of the wave (v) is directly related to the angular frequency (Ο) and wave number (k).
Imagine a dancer performing twirls on stage. The dancer's position changes over time, but the flow of their movements remains smooth. In this analogy, the dancer's position is like the wave's position, and the rhythm of their steps aligns with the wave's frequency and wavelength.
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Relating Ο to T and k to Ξ», we get v = Ξ»/T = fΞ» (14.12). Eq. (14.12), a general relation for all progressive waves, shows that in the time required for one full oscillation by any constituent of the medium, the wave pattern travels a distance equal to the wavelength of the wave.
Here we connect the speed of a wave to its wavelength (Ξ») and the frequency (f). The equation v = Ξ»/T shows that the speed of a wave depends on both how long the wave is (wavelength) and how frequently it oscillates (frequency). Essentially, in the time it takes for one oscillation, the wave travels a distance equal to its wavelength.
Consider a train moving along a track. If you measure the distance between each train car (the wavelength) and how fast the train runs (the speed), you can also think about how often the train passes noted points (the frequency). Together, these measures help you understand the overall motion of the train.
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The speed of a mechanical wave is determined by the restoring force setup in the medium when it is disturbed and the inertial properties (mass density) of the medium. The speed is expected to be directly related to the former and inversely to the latter. For waves on a string, the restoring force is provided by the tension T in the string. The inertial property will in this case be linear mass density Β΅, which is mass m of the string divided by its length L.
To find the speed of waves on a string, we consider two main factors: the tension in the string and the mass per unit length (linear mass density). The greater the tension, the faster the wave travels because the string can return to its resting position more quickly. Conversely, if the string is heavier (higher mass density), the speed decreases because more energy is needed to move the string.
Think of a tightrope walker. A tight and well-strung wire allows for a fast response to movements, similar to how higher tension in a string allows faster wave propagation. If the wire were heavier and thicker, it would sway more slowly, representing how mass density affects wave speed.
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For longitudinal waves, the speed is determined by the bulk modulus of the medium (B) and its density (Ο). The general formula for longitudinal waves is given by v = B/Ο (14.19). This shows that the speed of sound waves in gases, liquids, and solids is different due to their unique elastic and inertial properties.
In a longitudinal wave, such as sound traveling through air, the speed depends on how compressible the medium is (bulk modulus) and how heavy the medium is (density). The formula v = B/Ο highlights this relationship. The stiffer the medium and the less it weighs, generally, the faster the wave travels.
Imagine blowing through a straw into a glass of water. The water (liquid) reacts quickly to your breath, showing sound's fast travel in liquids due to better compressibility. Now, if you tried this with a dense material like steel, sound travels even faster due to its rigidity and lower compressibility compared with gases.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Wave Speed: The speed at which a wave travels through a medium, influenced by density and tension.
Tension: The force that influences the propagation speed of a wave on a string.
Linear Mass Density: Represents the mass distribution along the length of the medium.
Bulk Modulus: The property that affects how sound waves propagate in fluids, defined as resistance to compression.
Frequency: The rate of oscillation of a wave, affecting its energy and wavelength.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example 1: The speed of sound in air at room temperature is typically about 343 m/s.
Example 2: A tensioned string with a tension of 100 N and linear density of 0.05 kg/m results in wave speed v = β(100 N / 0.05 kg/m) β 44.72 m/s.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Waves in speed, tension is the key, heavier the load, slower they be.
Imagine a tightrope walker (waving through the air) β the tighter the rope (tension), the faster he balances (waves), but if itβs too heavy (density), heβs slowed down.
To remember wave properties, think 'STB': Speed, Tension, Bulk modulus.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Wave Speed
Definition:
The speed at which a wave propagates through a medium.
Term: Tension
Definition:
The force exerted along the length of a medium that causes waves to propagate.
Term: Linear Mass Density (ΞΌ)
Definition:
Mass per unit length of the medium through which waves travel.
Term: Bulk Modulus (B)
Definition:
A measure of a material's resistance to uniform compression.
Term: Frequency (Ξ½)
Definition:
The number of oscillations or wave cycles that occur in a unit of time.