Solving Sin(theta) = dy/dx | Acoustics Course Prep

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Discussion Overview

The discussion revolves around the approximation of the sine function in the context of deriving the one-dimensional wave equation for a tensioned string in an acoustics course. Participants explore the relationship between the angle theta, the sine function, and the derivative dy/dx, particularly for small angles.

Discussion Character

  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant expresses confusion over the statement that sin(theta) can be replaced by dy/dx for small angles, expecting the approximation sin(theta) = theta instead.
  • Another participant clarifies that for small theta, sin(theta) can be approximated by tan(theta), which equals dy/dx, indicating that theta represents the slope angle of the string.
  • A further contribution explains the geometric relationship, stating that sin(theta) can be expressed as Δy / sqrt(Δy^2 + Δx^2), leading to the approximation sin(theta) ≈ Δy / Δx when Δy is small compared to Δx.

Areas of Agreement / Disagreement

Participants present differing perspectives on the approximation of sin(theta) in relation to dy/dx, with no consensus reached on the preferred interpretation or method of approximation.

Contextual Notes

The discussion involves assumptions about the small angle approximation and its implications for the derivation of the wave equation, which may not be universally applicable without further context.

rexregisanimi
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In preparing for an acoustics course, I ran across the following sentence which confused me:

"If (theta) is small, sin(theta) may be replaced by [partial]dy/dx."

I expected to see sin(theta) = (theta) so this threw me off. This came up in the derevation of the one dimensional wave equation after approximating (by Taylor series) the transverse force on a mass element of a tensioned string with [partial]d(Tsin(theta))/dx. The approximation in question thus gave T*([partial]d2y/dx2)*dx.

In the original setup, x and y are cartesian axis in physical 2D space and (theta) is the angle the string (with tension T) makes from the x-axis after displacement from equalibrium.

I've never seen sine approximated by dy/dx before and was hoping somebody might shed some light for me :)
 
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When ##\theta## is small, ##sin\theta \approx \tan\theta = \frac{dy}{dx}##. In the derivation for the vibrating string, ##\theta## is the slope angle of the string.
 
Thank you! :)
 
sin(θ) = Δy / sqrt(Δy^2 + Δx^2). For small θ, Δy is small compared to Δx, so

sin(θ) ≈ Δy / sqrt(0 + Δx^2) = Δy / Δx
 
Last edited:

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