To show that frequency of a Helmholtz resonator varies inversely as the square root of its volume and to estimate the neck correction
1. Aim
To verify experimentally that the frequency of a Helmholtz resonator varies inversely as the square root of its volume, and to determine the effective length correction of the neck.
2. Apparatus Used
- Set of Helmholtz resonators with the same neck diameter but different volumes
- Tuning forks of various frequencies
- Digital frequency meter/oscilloscope (optional)
- Rubber mallet for striking tuning forks
- Measuring scale
- Vernier calipers
- Thermometer
- Rubber stoppers or clay (for varying volume)
- Microphone and amplifier setup (optional)
- Water (for varying volume)
3. Diagram
Figure 1: Experimental setup for Helmholtz resonator experiment
4. Theory
A Helmholtz resonator consists of a cavity (volume V) connected to the outside air through a narrow neck of cross-sectional area A and length L. When air is forced into the cavity through the neck, the pressure inside increases, pushing the air back out. Due to inertia, the air overshoots and creates a pressure lower than atmospheric pressure, drawing air back in. This oscillatory motion creates a resonance at a specific frequency.
The resonator can be modeled as a mass-spring system where:
- The air in the neck acts as a mass (m)
- The air in the cavity acts as a spring (with stiffness k)
The resonance frequency (f) of a Helmholtz resonator is given by:
Where:
- c is the speed of sound in air
- A is the cross-sectional area of the neck
- V is the volume of the cavity
- L' is the effective length of the neck (L + ΔL)
- ΔL is the end correction
The end correction (ΔL) accounts for the fact that the oscillating air extends slightly beyond the physical ends of the neck. For a flanged opening, ΔL ≈ 0.85r, where r is the radius of the neck.
Rearranging the equation:
This shows that $f^2 \propto \frac{1}{V}$, meaning $f \propto \frac{1}{\sqrt{V}}$, which is what we aim to verify.
5. Formula
The primary formula used:
Where:
- f is the resonance frequency (Hz)
- c is the speed of sound in air (≈ 343 m/s at 20°C)
- A is the cross-sectional area of the neck (m²)
- V is the volume of the cavity (m³)
- L' is the effective length of the neck (m) = L + ΔL
- ΔL is the end correction (m)
Speed of sound in air at temperature T (in °C):
For plotting:
From the slope, we can calculate L' and then determine ΔL = L' - L.
6. Procedure
Part A: Verification of f ∝ 1/√V
- Measure the dimensions of each Helmholtz resonator:
- Neck diameter (d) using vernier calipers
- Neck length (L) using measuring scale
- Calculate the neck area A = πd²/4
- Measure the internal volume (V) of each resonator
- For each resonator:
- Hold a vibrating tuning fork near the mouth of the resonator
- Try different tuning forks until maximum resonance is observed
- Record the frequency of the tuning fork that produces maximum resonance
- Alternatively, use a frequency generator and speaker, varying the frequency until maximum resonance is detected
- Repeat the procedure for all resonators with different volumes.
- Record the room temperature to calculate the speed of sound.
Part B: Determining the End Correction
- Use a single resonator with adjustable volume (e.g., by adding water to change the air volume)
- Measure the initial volume V₁ and find the resonance frequency f₁
- Change the volume to V₂ by adding a measured amount of water and find the new resonance frequency f₂
- Repeat for 5-6 different volumes
- Plot f² vs 1/V and determine the slope
- From the slope, calculate L' and then ΔL = L' - L
7. Observation Table
Table 1: Resonator Dimensions
Resonator | Neck Diameter (d) (m) | Neck Length (L) (m) | Neck Area (A) (m²) | Cavity Volume (V) (m³) |
---|---|---|---|---|
1 | ||||
2 | ||||
3 | ||||
4 | ||||
5 |
Table 2: Resonance Frequency Measurements
Resonator | Volume (V) (m³) | 1/V (m⁻³) | Resonance Frequency (f) (Hz) | f² (Hz²) |
---|---|---|---|---|
1 | ||||
2 | ||||
3 | ||||
4 | ||||
5 |
Table 3: Variable Volume Measurements (For End Correction)
Trial | Volume (V) (m³) | 1/V (m⁻³) | Resonance Frequency (f) (Hz) | f² (Hz²) |
---|---|---|---|---|
1 | ||||
2 | ||||
3 | ||||
4 | ||||
5 | ||||
6 |
Room Temperature: _____ °C
Speed of sound (c): _____ m/s
8. Calculations
-
For each resonator, calculate:
- 1/V (m⁻³)
- f² (Hz²)
-
Plot a graph of f² vs 1/V
- The graph should be a straight line passing through the origin
- Calculate the slope (m) of the best-fit line
-
From the slope, calculate L':
$$ m = \frac{c^2A}{4\pi^2L'} $$ $$ L' = \frac{c^2A}{4\pi^2m} $$ -
Calculate the end correction:
$$ \Delta L = L' - L $$ -
Verify the theoretical end correction:
- For a flanged opening: ΔL ≈ 0.85r (where r = d/2)
- Compare your experimental value with this theoretical value
9. Result
-
The graph of f² vs 1/V shows a linear relationship, confirming that f ∝ 1/√V.
-
The experimental value of the end correction (ΔL) = _____ m
-
The theoretical value of the end correction = _____ m
-
Percentage error = [(|Experimental - Theoretical|)/Theoretical] × 100 = _____ %
-
The relationship between frequency and volume of a Helmholtz resonator has been verified, and the end correction of the neck has been experimentally determined.