Putting this here, because you can't handle the truth 

https://www.youtube.com/live/vAWRGupuh3Y?feature=shared

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.