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Today we will talk about eigenfrequencies, which are specific frequencies at which a system tends to oscillate. Can anyone tell me why these frequencies might be important?
They are important for musical instruments, right? Different strings vibrate at different frequencies.
Exactly! The eigenfrequencies depend on the length of the string and its tension. Letβs see how we define these eigenfrequencies mathematically. The allowed wavelengths are given by \( \lambda_n = \frac{2L}{n} \). Who can explain what L and n represent?
L is the length of the string and n is the harmonic number!
Great! So, for each mode of vibration, you get a different frequency. This leads us to the formula for frequencies, \( f_n = \frac{n v}{2L} \). Any questions about this?
Does that mean if I change the length of the string, I also change the frequency?
Correct! Reducing the length increases the frequency. In summary, the standing wave can only exist at certain wavelengths and frequencies on a fixed string.
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Let's apply what we've learned about eigenfrequencies. Who can think of an example where eigenfrequencies play a crucial role?
In musical instruments! The strings on a guitar resonate at different frequencies.
Exactly! Each guitar string produces a different note depending on its thickness, tension, and length. Can someone tell me how changing the tension impacts the frequency?
More tension means a higher frequency, right?
That's right! This fundamental understanding of eigenfrequencies helps designers tune instruments accurately to desired pitches.
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Now that we understand eigenfrequencies, letβs derive the formulas for wavelength and frequency together. Can anyone explain the physical significance of \( n \)?
It's the harmonic number that tells us which frequency mode we are in.
Right! Let's start with the formula for wavelength: \( \lambda_n = \frac{2L}{n} \). What happens as n increases?
The wavelength decreases, which means the frequency increases.
Perfect! And now we calculate the frequency using \( f_n = \frac{n v}{2L} \). Can anybody explain how changing length affects l frequencies?
A shorter string length gives higher frequencies!
Well done! We can definitely see how these concepts connect. Remember to always relate the physical properties to the mathematical forms.
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The section explains how standing waves occur on a fixed string, detailing the allowed wavelengths and corresponding eigenfrequencies. This understanding is crucial for applications ranging from musical instruments to engineering design.
When a string is fixed at both ends, it can support standing waves that resonate at specific frequencies known as eigenfrequencies. The allowed wavelengths are determined by the length of the string (L) and the harmonic number (n). The formula for the allowed wavelengths is:
$$ \lambda_n = \frac{2L}{n}, \quad n = 1, 2, 3, ...$$
The corresponding frequencies for these wavelengths can be calculated using the wave speed (v), yielding:
$$ f_n = \frac{n v}{2L} $$
where n represents the harmonic mode of vibration. This section underscores the relationship between physical length, wave properties, and frequency, which are foundational for understanding wave behavior in strings.
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Allowed wavelengths:
\[ \lambda_n = \frac{2L}{n}, \quad n = 1, 2, 3, ... \]
The formula states that the allowed wavelengths (denoted as \( \lambda_n \)) for standing waves on a string with fixed ends are determined by the length of the string (\( L \)) and a positive integer (\( n \)), which represents the mode number. The wavelengths are inversely proportional to the mode number, implying that as \( n \) increases, the wavelength decreases. For example, for the first mode (n=1), the wavelength is equal to twice the length of the string, while for the second mode (n=2), it is equal to the length of the string.
Think of a guitar string when you pluck it. The fundamental frequency (first mode) produces a long wavelength, generating a deep sound. When you press the string at certain points to shorten it, you create different modes with shorter wavelengths and higher pitches. These modes are directly tied to the integer values of \( n \).
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Frequencies:
\[ f_n = \frac{n v}{2L} \]
This formula calculates the frequencies (\( f_n \)) of the standing waves on the string based on the wave speed (\( v \)), the length of the string (\( L \)), and the mode number (\( n \)). The frequency increases with the mode number, meaning higher modes produce higher frequencies. The factor of \( \frac{n}{2L} \) shows that for each increase in \( n \), the frequency rises proportionately. The wave speed is determined by the tension in the string and its mass per unit length.
Imagine tuning a piano. When you press a key, the string vibrates at a certain frequency. The different frequencies correspond to the different notes you hear. By adjusting the length of the string (like using the piano's pedals), you can create various tones, which relate directly to the formulas for standing wave frequencies.
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Key Concepts
Eigenfrequencies: Specific resonant frequencies of a string determined by its fixed length and tension.
Wavelength: The distance between consecutive points in a wave, related to the string length and harmonic number.
Frequency: The rate of oscillation of the wave, calculated with the help of the wave speed and string length.
See how the concepts apply in real-world scenarios to understand their practical implications.
A guitar string of length 1 m fixed at both ends vibrating at its fundamental mode (n=1) produces an eigenfrequency of 200 Hz if the wave speed is 200 m/s.
In a 2 m long violin string, the second harmonic (n=2) will have a wavelength of 1 m and a frequency of 100 Hz if the wave speed is 200 m/s.
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Fixed at both ends, a string will sing,
Once upon a string, fixed tight at each end, it could only play notes that would ascend. Each length and tension twisted fate, creating eigenfrequencies for all to celebrate.
Remember 'L + n = Wave', where 'L' is the string length and 'n' is the harmonic number that helps us find our wave properties!
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Review the Definitions for terms.
Term: Eigenfrequency
Definition:
The specific frequencies at which a string can resonate, determined by its length and tension.
Term: Wave Speed
Definition:
The speed at which waves travel along the string, given by \( v = \sqrt{\frac{T}{\mu}} \), where T is tension and \( \mu \) is mass per unit length.
Term: Harmonic Number (n)
Definition:
A positive integer that defines each mode of vibration on the string.
Term: Wavelength (\( \lambda \))
Definition:
The distance between two consecutive points of phase on a wave, such as crest to crest.
Term: Frequency (f)
Definition:
The number of oscillations that occur in a unit of time.