SambaNova + Aider + ClaudeDev + Continue : FREE & FAST AI Coding Setup with Llama-3.1 405B

In this video, a guide is shared on setting up a free AI coding editor using the **SambaNova Llama-3.1 405B API**. This is a 100% free and open-source alternative to **Cursor**. It shows how to stop paying for the **Cursor AI Coding Editor** by switching to a **local and open-source** solution based on **VSCode**, paired with tools like **ClaudeDev**, **Aider**, and **ContinueDev**.

This setup combines **VSCode** (or **NeoVim**) with **SambaNova Llama-3.1 405B**, and it works with any open-source LLM or popular models like GPT-4O, Claude-3, CodeQwen, Mixtral, Grok-1.5, and Gemini Code Assist.

For anyone looking to save on AI coding tools or wanting an open-source alternative, this guide is a great resource.

https://youtu.be/MNuRBOB2r38?feature=shared

This model is huge, but seems to be actually really good unlike Reflection 70B.

This is also open source, this video shows how to install via LM Studio.

https://youtu.be/mvpkZ1yFy7o?feature=shared

This open source model apparently outperforms most of the paid models.

And an even bigger model is coming next week.

https://www.reddit.com/r/LocalLLaMA/comm...orlds_top/

According to this video, good prompting is still the key.
https://www.youtube.com/watch?v=1WpC-UPrmVU

How to install locally
https://www.youtube.com/watch?v=pIX7G1xfHYQ

Here is the chart in my video "Improved Bedini Switch"

   

I'd like to provide an update on the progress with my PCB. While I was working on switching the spike, another approach came to mind.
Many people aim to achieve a self-looping system or to recover some of the power efficiently. Typically, this involves methods like using isolation, transformers, or inverters to feed the loop in an isolated manner. However, these methods often come with significant drawbacks, such as low efficiency and substantial losses, which diminish most of the potential gains. As a result, Bedini found it more practical to use the spike energy to charge batteries that are isolated from the input.
In this session, I'd like to discuss a method to achieve this more simply, through some modifications. It’s surprising that no one seems to mention running Bedini switches in this manner. It appears to be a much more efficient approach.

Because someone asked on Youtube about it for reference here are some personal notes. 

Please don't mind the mess and scribbles. I used this to help me originally find a good choice of electrodes for the PEG cell. 

   

   

   

DIY GUIDE:

https://docs.google.com/document/u/0/d/1...obilebasic

https://www.youtube.com/live/xNm8iIcPt3I...AVqb4j37QK

   

### Parts List for the Corrected Circuit

Here’s a comprehensive list of the components you’ll need to build this circuit:

1. **Resistors:**
  - R1: 1.5 kΩ Fixed Resistor
  - R2: 330 Ω  Potentiometer (variable resistor)
  - R3: 470 Ω Fixed Resistor
  - R4: 2.2 kΩ Fixed Resistor
  - R5: 190 Ω Fixed Resistor (two pieces, one for Q2 gate and one for Q3 gate)

2. **Capacitors:**
  - C1: 0.1 µF (100 nF) Ceramic Capacitor

3. **MOSFETs:**
  - Q1: IRF 510 or IRF 511 N-channel Power MOSFET (for the inverter stage)
  - Q2: IRF 510 or IRF 511 N-channel Power MOSFET
  - Q3: IRF 510 or IRF 511 N-channel Power MOSFET

4. **Timer IC:**
  - TLC 555 CMOS Timer IC (Radio Shack Cat. # 276-1718)

5. **Power Supplies:**
  - V1: 14-18V DC Power Supply (for the timer circuit)
  - V2: 7-9V DC Battery (for the "potential" source driving Q2 and Q3)

6. **Inductive "Collector":**
  - This can be a spool of wire, as described in the original circuit:
    - **Option 1**: 500 ft of solid 12 gauge wire
    - **Option 2**: 100 ft of 22 gauge solid hookup wire
    - **Option 3**: 40 ft of 22 gauge magnet wire
    - **Option 4**: Experiment. Use Coax Spool ( Velocity Factor )

7. **Load Resistor:**
  - Load: 1 Ω Fixed Resistor (for testing current gain across this load)

The corrected circuit looks well-designed for achieving the desired 3 kHz frequency with low microsecond pulse widths. Your adjustments to R1 and R2, along with the gate connection of Q3 to the drain of Q2, appear correct and should help in capturing the inductive kickback effectively, potentially leading to the observed current and power gains.


Optionally: 
Incorporating a spool of coaxial cable into your circuit, taking advantage of its velocity factor, can offer enhanced control over the timing and energy dynamics of the circuit. This approach can improve the synchronization of inductive kickback with the switching events, potentially leading to greater energy efficiency and a higher observed power gain.If you decide to implement this, carefully calculate the delay you need and choose the appropriate length of coaxial cable. Experiment with different configurations to see which offers the best results in terms of energy recovery and gain.

Summary:

The rapid switching effectively "locks in" some of the energy within the magnetic coil, preventing it from dissipating and allowing it to be reused in subsequent cycles. This leads to a scenario where the energy is partially recycled, contributing to the overall gain in the circuit. The quick switching at the input stages delays the current and maintains a higher level of energy in the system, which could explain the observed gains.

This process is highly dependent on precise timing and component selection, especially in relation to the inductive properties of the coil and the switching characteristics of the MOSFETs. By optimizing these factors, the circuit can maximize the energy recovery from each cycle, leading to an over-unity behavior where the output power appears greater than the input power.

Key Points About the Switching and Inductive Kickback:

1. Fast Switching Prevents Energy Loss:
   • By switching the circuit at microsecond intervals, the system operates faster than the energy dissipation mechanisms (like resistive losses or leakage) can effectively drain the stored energy.
     
   • This rapid switching means that some of the energy stored in the magnetic field (within the coil or core) during the energization phase does not have time to fully dissipate. Instead, this energy remains partially stored in the core and is available for the next energization cycle.
     
2. Inductive Kickback Utilization:
   • The inductive kickback is a high-voltage spike generated when the current through an inductor (like the coil) is suddenly interrupted.
     
   • If the switching is fast enough, the circuit can capture this kickback before it has a chance to fully dissipate. This captured energy is then directed back into the system, potentially increasing the current and energy available for the load.
     
   • By carefully timing the activation of Q3, the circuit can ensure that this kickback is applied in reverse polarity across the load at just the right moment, boosting the overall energy transfer to the load.
     
3. Energy Accumulation and Gain:
   • The concept of energy remaining in the core for the next cycle is akin to resonant energy storage, where the energy is not entirely lost between cycles but is instead carried forward.
     
   • This can lead to a cumulative effect, where each subsequent energization cycle builds upon the previous one, gradually increasing the energy within the system.
     
   • Because the input stages are switching too quickly for the energy to be fully "loaded down" (or dissipated), more of the energy from each cycle remains available for the next, contributing to the observed gain.
     

   

Overview:
This device appears to be an electrostatic power generator that leverages the principles of ionization, capacitance, and electrostatic interactions to generate and store electrical energy. The setup involves a combination of hybrid ion valves functioning as capacitors (similar to Leyden jars), copper coils for high-frequency (HF) filtering, and a configuration of dissimilar metals to create a potential difference and generate current.
Components Breakdown:

1. Hybrid Ion Valves as Capacitors (Leyden Jar Configuration):
   • These are used to store charge and create a potential difference. The ion valves function similarly to Leyden jars, where a dielectric material (ionized air in this case) is sandwiched between conductive plates or surfaces (MG mesh electrodes).
     
   • The center rod inside each ion valve is a copper coil. This coil serves two purposes: filtering high-frequency signals and helping ionize the air around it.
     
2. Copper Coil for HF Filtering and Ionization:
   • The copper coil in the center of the ion valve serves as a high-frequency filter, ensuring that only the desired frequencies are allowed through while unwanted frequencies are filtered out.
     
   • Additionally, the high voltage applied to this coil creates an intense electric field around it, which ionizes the surrounding air. This ionized air acts as a dielectric medium with enhanced properties, increasing the capacitance of the system.
     
3. Dissimilar Metals Reaction:
   • The device utilizes dissimilar metals (e.g., magnesium mesh and other metallic components) to create a galvanic reaction. This reaction contributes to generating a real potential difference (voltage) and current within the magnetic field of the system.
     
   • This galvanic effect works alongside the electrostatic storage and helps to maintain a steady potential difference, further charging the internal capacitors.
     
4. MG Mesh Electrodes and Ionized Air Dielectric:
   • The internal capacitors are made of magnesium (MG) mesh electrodes with a small gap of air between them. This air is ionized by the high voltage field generated by the copper coil, which significantly enhances the dielectric properties of the air.
     
   • As the dielectric constant of the air increases due to ionization, the capacitance of these internal capacitors increases, allowing them to store more energy.
     
5. Cap Dump Outputs:
   • The energy stored in the capacitors is periodically released or "dumped" into the circuit, providing a burst of electrical energy. This is the "cap dump" output mentioned in the diagram.
     
   • The enhanced capacitance due to ionized air allows for more substantial energy storage and, consequently, more powerful outputs when the stored energy is released.
     

• The device begins by generating a high voltage through an electrostatic generator (depicted by the hand-crank mechanism on the left).
  
• This high voltage is applied to the hybrid ion valves, which store the energy in the form of an electrostatic charge.
  
• The copper coils inside these valves help filter out unwanted frequencies and ionize the air around the MG mesh electrodes.
  
• The dissimilar metals create a small but constant potential difference, contributing to the overall energy generation process.
  
• The internal capacitors, with their enhanced capacitance due to the ionized air, store a significant amount of energy, which is then periodically released to produce a high-power output.
  

   



Understanding the Magnetic Rectifier: Analyzing a Novel AC to DC Conversion Technique
The concept illustrated in the provided image describes a magnetic rectifier designed to convert alternating current (AC) to direct current (DC) using the magnetic properties of a core and coils, combined with the influence of permanent magnets. This method is distinct from conventional semiconductor-based rectifiers, offering a different approach to rectification that could be of interest in various energy conversion and harvesting applications.
How the Magnetic Rectifier Works

1. Coils and Cores:
   • The rectifier consists of two cores, each with a coil wound around it. The coils are wound in the same direction using No. 30 S.S.C. wire (which likely stands for single-stranded copper wire). Each core has 1,000 feet of wire wound onto it.
     
   • The cores are cylindrical, measuring 2 inches long by ⅞ inches in diameter, and are likely made of soft iron to enhance magnetic flux concentration.
     
2. Permanent Magnets:
   • Two bar magnets are positioned as close as possible to the cores without touching them. These magnets are pivotal in the operation of the rectifier. The diagram specifies that the like poles of these magnets should face each other, creating a strong magnetic field across the gap between them.
     
3. AC Input and Grounding:
   • The AC line is connected such that one side is grounded to one core, and the other side of the AC line is connected to the second core. This setup allows the alternating current to flow through the coils wound around the cores.
     
4. Rectification Process:
   • The magnetic field created by the permanent magnets interacts with the AC current flowing through the coils. As the AC current oscillates, the changing magnetic field in the cores due to the interaction with the permanent magnets forces the current to flow in a single direction when taken from the contact points at the pivot of the magnets. This results in a rectified DC output.
     
   • The output DC is taken from the contact points holding the permanent magnets. The magnetic field from the bar magnets induces a directional flow of current, effectively rectifying the AC input into DC output.
     

1. Magnetic Saturation and Switching:
   • The operation of this rectifier hinges on magnetic saturation and switching effects caused by the alternating magnetic field. As the AC current oscillates, it alternates the magnetization of the cores, which interacts with the permanent magnetic field to favor current flow in one direction more than the other.
     
2. Use of Soft Iron Cores:
   • Soft iron cores are used because they can easily be magnetized and demagnetized, which is essential for the switching action that occurs with each cycle of AC input.
     
3. Symmetrical Magnetic Field:
   • The like poles of the permanent magnets facing each other create a symmetrical and opposing magnetic field across the cores. This configuration might help in maintaining a more stable and steady DC output by ensuring that the magnetic influence is consistent as the AC current changes direction.
     

1. Energy Harvesting:
   • This magnetic rectifier could be adapted for low-power energy harvesting applications, where ambient AC electromagnetic fields are rectified into usable DC. Its simplicity and lack of semiconductor components make it potentially useful in environments with high electromagnetic noise or where conventional diodes might fail due to thermal or electrical stresses.
     
2. Passive Rectification:
   • In scenarios where passive components are preferred over active components (e.g., in high-radiation or high-temperature environments), this rectifier could provide a reliable means of converting AC to DC without the need for traditional semiconductors.
     
3. Electromagnetic Compatibility:
   • Given its reliance on magnetic fields rather than direct electrical connections to rectify current, this approach might offer unique benefits in systems where electromagnetic compatibility (EMC) is a concern. It could be used to design rectifiers that minimize electrical noise or interference.
     
4. Exploring Negative Resistance:
   • In line with your research into negative resistance and non-linear effects, this magnetic rectifier could be part of a broader exploration into non-linear magnetic systems. The magnetic interaction here introduces non-linearity that could be exploited in advanced energy systems or novel power conditioning technologies.
     

   

The diagram you've provided is labeled as a "G Wave Device" by Joel Lagace. It appears to be a conceptual design for a system that generates or manipulates gravitational waves or some form of thrust force through electromagnetic means. Let’s break down the components and speculate on how this device might operate.

Components and Configuration:

1. Tank Capacitor:
   • Function: The tank capacitor is likely part of a resonant circuit, possibly an LC circuit (inductor-capacitor circuit), that is designed to store and release energy in a controlled manner. The capacitor stores electrical energy and, in conjunction with the inductor (primary coil), oscillates at a specific frequency.
     
   • Role in Resonance: This capacitor, paired with the primary coil, helps establish a resonant frequency for the circuit. The resonance would allow the system to build up large oscillating currents and magnetic fields with minimal input power.
     
2. Primary Coil:
   • Function: The primary coil, which is coupled with the tank capacitor, generates a magnetic field when current flows through it. This coil is a key part of the resonant circuit and is responsible for producing the magnetic field that interacts with other parts of the device.
     
   • Electromagnetic Interaction: The coil’s magnetic field likely interacts with the magnetic field lines shown in the diagram, contributing to the generation of the G waves or thrust forces.
     
3. Controller (400 Hz, Phased 180 Degrees):
   • Purpose: This controller modulates the current flowing through the coils at a frequency of 400 Hz and ensures that the current in the coils is 180 degrees out of phase. This phasing is crucial for creating alternating magnetic fields that could interfere constructively or destructively, depending on the desired outcome.
     
   • Frequency Modulation: The specific choice of 400 Hz might be related to the natural resonant frequency of the device or a frequency at which the device is most efficient at generating the desired effects.
     
4. Coils (High Current Modulation):
   • Function: These coils are modulated with high current, which likely means they are designed to handle large amounts of power. The modulation of these coils would create varying magnetic fields, which could interact with each other and the environment to produce a thrust force or gravitational wave effect.
     
   • Magnetic Field Interaction: The diagram shows magnetic field lines around these coils, suggesting that they play a crucial role in shaping and directing the magnetic fields generated by the system.
     
5. Magnetic Field Lines:
   • Visualization: The diagram shows magnetic field lines (green arrows) emanating from the central circular structure. These lines represent the path along which the magnetic flux travels, and they are likely manipulated by the currents in the coils to produce the desired force.
     
   • Interaction with Current: The yellow arrows represent the direction of current flow within the circular structure. The interaction between the current and the magnetic field lines could be responsible for generating the thrust force or the gravitational wave effect.
     
6. Thrust Force:
   • Generation: The thrust force is indicated at the top of the device, suggesting that the interaction of the magnetic fields and currents within the device produces a mechanical force. This could be due to the Lorentz force, where a current-carrying conductor in a magnetic field experiences a force.
     
   • Possible Gravitational Wave Production: If this device is intended to generate gravitational waves, the thrust force might be a byproduct of the manipulation of spacetime, where the electromagnetic fields interact with the fabric of space to produce ripples or waves.
     
7. Mass or Sensor:
   • Role: This component at the top right could either be a mass that responds to the generated thrust force or a sensor that measures the effects of the device. If it’s a sensor, it might be detecting changes in gravitational fields or measuring the force produced by the device.
     

1. Electromagnetic Interaction:
   • The device operates by generating and modulating strong magnetic fields through the coils and capacitors. The phased modulation at 400 Hz could create conditions where the magnetic fields interfere in a way that produces a net force or generates gravitational waves.
     
2. Resonance and Energy Build-Up:
   • The LC circuit formed by the tank capacitor and primary coil is likely tuned to resonate at a specific frequency, allowing the system to build up significant energy. This energy is then used to drive the high-current coils, creating intense magnetic fields.
     
3. Thrust or Gravitational Wave Production:
   • The interaction between the magnetic fields and the structure of the device could lead to the production of a thrust force. If the device is designed to manipulate gravitational waves, the alternating magnetic fields might induce perturbations in spacetime, generating the desired waves.
     
4. Phased Magnetic Field Manipulation:
   • The 180-degree phasing ensures that the magnetic fields produced by the coils are carefully timed to either enhance or cancel each other out in specific regions. This careful control of the magnetic fields is crucial for directing the force or wave generation in a controlled manner.
     

1. Electromagnetic Fields and Resonance:
   • The device utilizes electromagnetic fields, which are fundamental to many alternative energy and propulsion concepts. The resonance created by the LC circuit (tank capacitor and primary coil) is key to amplifying the energy within the system. Resonance allows for the buildup of large oscillating currents and magnetic fields with minimal input power, which is crucial for achieving the desired effects.
     
2. Lorentz Force:
   • The Lorentz force is the force experienced by a charged particle moving through a magnetic field, given by the equation F=q(E+V x B) 
     
     1. • In this device, the current-carrying coils interact with the magnetic fields they generate, producing a force. If designed correctly, this force could be directed to produce thrust.
          
     2. Gravitational Waves and Spacetime Manipulation:
        • Gravitational waves are ripples in spacetime caused by accelerated masses, as predicted by Einstein's General Theory of Relativity. While conventional gravitational waves are generated by astronomical events (like merging black holes), the idea here might be to use electromagnetic fields to induce similar effects on a much smaller scale. This would involve advanced theoretical physics, possibly leveraging concepts like electromagnetic stress-energy tensors to influence spacetime.
          
     3. Phased Magnetic Fields:
        • The use of phased magnetic fields (with a 180-degree phase difference) is crucial for creating constructive or destructive interference patterns. This can either amplify the effects (constructive interference) or cancel out unwanted interactions (destructive interference). The careful control of these fields might allow for the generation of directed thrust or other exotic effects like gravitational wave emission.
          
     Potential Applications:
     
     1. Propulsion Systems:
        • If the device can generate a significant thrust force through electromagnetic means, it could be a candidate for advanced propulsion systems, particularly for space exploration. Unlike conventional propulsion that relies on expelling mass (rocketry), this system might offer a form of "reactionless" propulsion, reducing the need for fuel.
          
     2. Energy Generation:
        • The device might be able to convert ambient or external energy sources into usable electrical power, possibly with very high efficiency if the resonant conditions are optimized. This could be applied in scenarios where conventional energy generation is impractical, such as deep-space missions or remote locations.
          
     3. Gravitational Wave Research:
        • If the device indeed interacts with or generates gravitational waves, it could serve as a research tool in the field of gravitational wave detection and manipulation. This would be groundbreaking, as it could provide a new method to study spacetime and gravitational phenomena on a smaller, more controllable scale.
          
     4. Field Manipulation and Shielding:
        • The ability to generate and control strong magnetic fields could have applications in shielding sensitive equipment from external electromagnetic interference or even in controlling the behavior of charged particles in a given space (such as in particle accelerators or plasma containment systems).
          
     Challenges and Considerations:
     
     1. Technical Challenges:
        • Material Science: The materials used must withstand high currents and strong magnetic fields without degrading or introducing unwanted losses. High-temperature superconductors could be a candidate material if cooling systems are feasible.
          
        • Precision Control: The phasing and modulation of currents must be precisely controlled to maintain the desired electromagnetic field interactions. This requires advanced electronics and possibly real-time feedback systems to adjust the phase and amplitude dynamically.
          
     2. Theoretical Validation:
        • Scientific Scrutiny: The underlying physics, especially if it claims to generate gravitational waves or "reactionless" thrust, would need to be rigorously tested and validated against existing physical laws. There may be skepticism, as such concepts challenge conventional physics, so careful experimentation and peer-reviewed research are essential.
          
        • Resonance Stability: Maintaining resonance in a dynamic system can be challenging, especially under varying external conditions. The system must be designed to adapt or stabilize itself to avoid drifting out of resonance.
          
     3. Energy Efficiency:
        • Power Input vs. Output: The system's overall energy efficiency needs to be carefully evaluated. If the energy required to maintain the system's operations exceeds the output or the benefits (e.g., thrust produced), it might not be practical.
          
        • Heat Dissipation: High currents and magnetic fields can generate significant heat, which needs to be managed effectively to prevent damage or loss of efficiency.
          
     4. Ethical and Safety Considerations:
        • Unintended Consequences: Generating strong magnetic fields or gravitational waves could have unintended effects on nearby electronics, biological tissues, or even the environment. Proper safety measures and thorough testing are crucial.
          
        • Regulatory Approvals: Devices that manipulate fundamental forces might be subject to regulatory oversight, particularly if they involve high energy levels or could have far-reaching effects.
          Conclusion:
          
     
     The G Wave Device represents a fascinating blend of theoretical physics and advanced engineering, with potential applications in propulsion, energy generation, and fundamental research. However, it also presents significant challenges, both in terms of technical implementation and theoretical validation. Moving forward, detailed experimentation, careful design, and open scientific collaboration will be crucial to explore the full potential of this concept.
     

• Material: Use copper wire for the coils due to its excellent conductivity and availability.
  • Specification:
    • Wire Gauge: 14 to 18 AWG, depending on the current handling requirements.
      
    • Insulation: Use enamel-coated magnet wire to ensure efficient winding with minimal losses.
      
  • Example Part Number: Magnet Wire AWG 18 - Remington Industries
    
  • Coil Form: You can use plastic or ceramic coil forms to wind the wire, which can be sourced from suppliers like McMaster-Carr or custom-made using 3D printing.
    

• Material: High-quality, high-voltage capacitors are necessary for the tank circuit to handle the energy storage and release cycles.
  • Specification:
    • Capacitance: 10 µF to 100 µF (depending on the frequency of operation and desired resonance).
      
    • Voltage Rating: 1000V or higher, depending on the expected voltage swings in the circuit.
      
  • Example Part Number: Cornell Dubilier 940C30P1K-F - 10µF, 1000V Polypropylene Capacitor.
    

• Purpose: To generate the necessary control signals at the specified frequency (400 Hz in the diagram) with 180-degree phase shifts.
  
• Specification:
  • Frequency Range: 0.1 Hz to 1 MHz (to allow for tuning and experimentation).
    
  • Phase Control: Ability to set phase shifts with fine precision.
    
  • Output: Should be capable of driving the coils directly or through a power amplifier.
    
  • Example Product: Agilent/Keysight 33500B Series Waveform Generator - Known for its precision and reliability.
    
  • Alternative: Rigol DG1022Z Function Generator - A more budget-friendly option with similar functionality.
    

• Purpose: To amplify the signal from the frequency generator to drive high-current coils.
  
• Specification:
  • Power Output: Depending on the coil's current requirements, an amplifier capable of delivering several amps at the desired voltage might be necessary.
    
  • Example Product: Texas Instruments TPA3255EVM Evaluation Module - Capable of delivering high power output with efficient heat management.
    

• Material: Similar to the primary and secondary coils, using thicker gauge copper wire if higher current is needed.
  • Specification: 10 AWG to 14 AWG copper wire with appropriate insulation.
    
  • Example Part Number: Southwire 10 AWG Copper Magnet Wire - Easily available in different gauges.
    

• Material: Soft iron or ferrite cores are common for inductors to concentrate and enhance the magnetic field.
  • Specification: Choose a core material that suits the frequency and power levels.
    
  • Example Part Number: Micrometals Iron Powder Cores - Various cores available for different applications.
    

• Coil Winding: Wind the primary coil using the chosen wire gauge on a non-conductive form. Calculate the number of turns based on the desired inductance and the resonance frequency.
  
• Capacitor Connection: Connect the chosen tank capacitor in parallel with the primary coil to form the resonant circuit.
  

• Frequency Generator Configuration: Program the generator to output a 400 Hz sine wave, ensuring the ability to adjust the phase. Connect the output to the power amplifier.
  
• Amplification: Use the amplifier to boost the signal from the frequency generator to a level sufficient to drive the coils.
  

• High Current Modulation: Connect the output of the power amplifier to the high current modulation coil, ensuring it’s capable of handling the current without overheating.
  
• Secondary Coil Integration: The secondary coil should be placed in proximity to the primary coil, ensuring proper coupling for magnetic field interaction.
  

• Mass or Sensor Integration: Attach a sensor or mass to the location where the thrust force is expected, and use instruments like a force gauge or accelerometer to measure any generated forces.
  
• Data Collection: Use an oscilloscope or data acquisition system to monitor the current, voltage, and magnetic field interactions, ensuring the system operates as expected.
  

• Frequency Tuning: Adjust the frequency slightly around 400 Hz to find the optimal resonant point, which might differ slightly depending on the actual inductance and capacitance values.
  
• Phase Adjustment: Experiment with the phase settings to see how different phase shifts affect the magnetic field interactions and any generated thrust.