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

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In the context of preparing for an acoustics course, the approximation of sin(theta) as dy/dx arises from the small angle assumption, where sin(theta) closely resembles tan(theta) when theta is small. This approximation is crucial in deriving the one-dimensional wave equation, particularly in analyzing the transverse force on a tensioned string. The discussion highlights that for small angles, the relationship between the change in vertical position (Δy) and horizontal position (Δx) simplifies the sine function. This simplification is valid because, under these conditions, Δy becomes negligible compared to Δx. Understanding this approximation is essential for grasping the underlying physics of wave motion in strings.
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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
 
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