Determining Steel String Diameter for Standing Wave Node

In summary, the figure below shows a snapshot of a standing wave on a composite string with a node at the composite point. To determine the diameter of the steel string, we can use the equation v/f = √(F/ρA) and the fact that the frequency is the same for both strings. By carefully rearranging the equation and plugging in the given values, we can solve for the diameter of the steel string, which should be 1.76 mm. However, in the given attempt at a solution, there were errors with the grouping under the square roots and the use of the variables d1 and d2.
  • #1
Firben
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0

Homework Statement



The figure below shows a snapshot of a standing wave on a composite string. It is a node in the composite point. If the aluminium string has a diameter of 1.50 mm, which diameter does the steel string have ?

http://s716.photobucket.com/user/Pitoraq/media/Fys22222_zps61d0eb53.png.html


Homework Equations



V = √(F/ρ(length)) = √(F/ρA)


The Attempt at a Solution



Al: Node in both endpoints

y = f(ωt)*sin(kx) <==> sin(k1L1) = 0 <==>

2π/λ1*L1 = P1π <==>

λ1 = 2/p1*L1

Steel: Node in both endpoints


sin(K2L2) = 0 <==> 2π/λ2*L2 = P2π <==>

λ2 = 2/p2*L2

λ = v/f

λ1 = v/f1 = 2/p1*L1 <==> vp1/2L1 = f1 <==>

vp2/2L2 = f2

Same frequency

vp2/2L2 = vp1/2L1 <==>

√(F/ρ(al)A1)*P1/2L1 = √(F/ρ(Steel)A2)*P2/2L2 <==>


√(F/ρ(al)4πd1)*P1/2L1 = √(F/ρ(Steel)4πd2)*P2/2L2 , breaking out d2 <==>

d2 = ((p2)^2*(L1)^2*(ρ(Al))*d1)/((p1)^2*(L2)^2*ρ(Steel))

Where d1 = 0.0015
ρ(Al) = 2.7+ * 10^3/m^3
ρ(Steel) = 7.87*10^3/m^3
L1 = 0.3 m
L2 = 0.25 m

p2 = 5
p1 = 3

Are the nodes from the figure

when i put does values into the equation above i got 2.058 * 10^-3 m

In the answer it should be 1.76 mm
 
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  • #2
I think if you are more careful writing the equations (especially the grouping under the square roots) you'll can see more clearly where the problem is. I'll rewrite some of it

Starting from:
Firben said:
Same frequency

vp2/2L2 = vp1/2L1 <==>

$$
\begin{align}
\frac{vp_2}{L_2} &= \frac{vp_1}{L_1} \\
\frac{p_2}{L_2} \sqrt{\frac{F}{\mu_2}} &= \frac{p_1}{L_1} \sqrt{\frac{F}{\mu_1}} \\
\frac{p_2}{L_2} \sqrt{\frac{F}{\pi(d_2/2)^2\rho_\mathrm{Steel}}}
&= \frac{p_1}{L_1} \sqrt{\frac{F}{\pi(d_1/2)^2\rho_\mathrm{Al}}} \\
\frac{p_2/L_2}{p_1/L_1} \sqrt{\frac{\rho_\mathrm{Al}}{\rho_\mathrm{Steel}}}
&= \frac{d_2}{d_1}
\end{align}
$$

d2 = ((p2)^2*(L1)^2*(ρ(Al))*d1)/((p1)^2*(L2)^2*ρ(Steel))

So it seems as if you forgot d1, d2 were inside the √ and as a result your p1, L1, p2, L2 got squared by accident.
 
Last edited:

FAQ: Determining Steel String Diameter for Standing Wave Node

How do you determine the steel string diameter for a standing wave node?

To determine the steel string diameter for a standing wave node, you need to know the tension of the string, the length of the string, and the frequency of the desired standing wave. Using these variables, you can calculate the required string diameter using the formula: diameter = √(T / (μ * L * f^2)), where T is the tension, μ is the linear density of the string, L is the length, and f is the frequency.

What is a standing wave node?

A standing wave node is a point on a vibrating string or other medium where the amplitude of the wave is zero. This occurs when two waves of the same frequency and amplitude traveling in opposite directions interfere with each other, resulting in a stationary pattern.

What is the importance of determining the steel string diameter for a standing wave node?

Determining the steel string diameter for a standing wave node is important because it allows for the proper selection of string size for a given instrument. If the string is too thin, it may break under tension, and if it is too thick, it may not produce the desired sound. By finding the appropriate diameter, the string can vibrate at the desired frequency and produce the desired pitch.

How does the tension of the string affect the standing wave node?

The tension of the string directly affects the frequency of the standing wave and therefore, the location of the standing wave node. Higher tension results in a higher frequency and shorter wavelength, which means the standing wave node will occur at a shorter distance from the fixed end of the string.

What other factors can affect the determination of the steel string diameter for a standing wave node?

Besides tension, length, and frequency, other factors that can affect the determination of the steel string diameter for a standing wave node include the material and density of the string, the temperature and humidity of the environment, and the stiffness and thickness of the string. These factors can all impact the wave speed and therefore, the frequency of the standing wave.

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