Solving for Natural Frequency in a Si-Based NEMS Resonator

In this case, since the dimensions are doubled, the mass will also be doubled, resulting in a decrease in the natural frequency by a factor of 2. Therefore, the new natural frequency would be 125MHz.
  • #1
Cookiesm8
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NEMS Resonator

I need a hint to help with my homework.

The question:

"A Si-Based NEMS resonator has dimensions length=150nm, width=5nm and thickness=5nm and an effective spring constant of 100Nm^-1 and natural frequency of vibration of 250MHz"

I am looking for an equation linking the natural frequency to the effective spring constant, as for the first part of the question i have to show what would happen to them if the dimensions of the resonator were doubled.

Any advice, been trawling the net and my notes for a while and no joy.
 
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  • #2
Hint: The equation linking the natural frequency and the effective spring constant is given by the equation f = 1/(2π√(k/m)), where f is the natural frequency, k is the effective spring constant, and m is the mass of the resonator.
 
  • #3


To solve for the natural frequency in a Si-Based NEMS resonator, you can use the equation:

f = 1/2π * √(k/m)

where f is the natural frequency, k is the effective spring constant, and m is the mass of the resonator.

To show what would happen to the natural frequency and effective spring constant if the dimensions of the resonator were doubled, you can use the equation:

k = 1/2 * E * (t/w)^3 * (l/w)

where E is the Young's modulus, t is the thickness, w is the width, and l is the length.

By doubling the dimensions, we can see that the thickness and length will both double, while the width remains the same. This means that the effective spring constant will increase by a factor of 8 (2^3), while the mass will increase by a factor of 4 (2*2). Plugging these values into the first equation, we can see that the natural frequency will increase by a factor of 2 (√(8/4) = 2).

Therefore, if the dimensions of the resonator were doubled, the natural frequency would increase by a factor of 2 and the effective spring constant would increase by a factor of 8.
 

1. What is natural frequency in a Si-based NEMS resonator?

Natural frequency refers to the characteristic frequency at which a system or structure will vibrate when disturbed from its equilibrium position. In a Si-based NEMS (nanoelectromechanical systems) resonator, this is the frequency at which the structure will vibrate when subjected to an external force or electrical signal.

2. How is natural frequency calculated in a Si-based NEMS resonator?

The natural frequency in a Si-based NEMS resonator can be calculated using the equation: f = 1/(2π√(m_eff*k)) where f is the natural frequency, m_eff is the effective mass of the resonator, and k is the spring constant of the structure.

3. What factors affect the natural frequency of a Si-based NEMS resonator?

The natural frequency of a Si-based NEMS resonator is affected by several factors including the mass of the structure, the stiffness of the material, and any external forces or electrical signals applied to the resonator. The dimensions and design of the structure can also impact the natural frequency.

4. Why is it important to solve for natural frequency in a Si-based NEMS resonator?

Solving for natural frequency in a Si-based NEMS resonator is important because it allows for the precise control and manipulation of the resonator's vibration. This is crucial for applications in sensing, signal processing, and other nanoscale technologies where the resonator's frequency response is critical.

5. How is natural frequency used in the design of Si-based NEMS resonators?

The natural frequency is an important parameter in the design of Si-based NEMS resonators as it helps determine the optimal dimensions and materials for the structure. By adjusting the natural frequency, the resonator's sensitivity and selectivity can be optimized for specific applications. Additionally, the natural frequency can be used to monitor the performance and stability of the resonator over time.

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