Bessler's secret

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Re: re: Bessler's secret

Post by Grimer »

pequaide wrote:The F is greater because of the sine of the greater angle. But the greater force is applied for a shorter period of time. If you do a close F * t study the force times time will be equal.

The down swing velocities are equal. And the rise distances are equal. The potential energy of each is equal. The down swing linear momentum s are equal. And in this rare case even the kinetic energies are equal. F*t and f*T are equal. About the only thing that is not equal is L = mvr - angular momentum.
...
Quite so.
And it is that difference that one can exploit.
cf. the Stirling engine example I gave in Cloud's thread where the heat content was the same but the heat intensity (analogous to difference in angular momentum = jerk) was different. It is that difference that Bessler must have exploited.
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re: Bessler's secret

Post by Grimer »

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Re: re: Bessler's secret

Post by Grimer »

Grimer wrote:
pequaide wrote:The F is greater because of the sine of the greater angle. But the greater force is applied for a shorter period of time. If you do a close F * t study the force times time will be equal.

The down swing velocities are equal. And the rise distances are equal. The potential energy of each is equal. The down swing linear momentum s are equal. And in this rare case even the kinetic energies are equal. F*t and f*T are equal. About the only thing that is not equal is L = mvr - angular momentum.
...
Quite so.
And it is that difference that one can exploit.
cf. the Stirling engine example I gave in Cloud's thread where the heat content was the same but the heat intensity (analogous to difference in angular momentum = jerk) was different. It is that difference that Bessler must have exploited.
I can see what the problem is with harnessing Newtonian/Ersatz gravity interaction. It's the same problem the ancients had with the colour blue.

http://uk.businessinsider.com/what-is-b ... lor-2015-2

This is a story "about the way that humans see the world and how until we have a way to describe something, even something so fundamental as a color, we may not even notice that it's there.
As the delightful Radiolab episode "Colors" describes, ancient languages didn't have a word for blue — not Greek, not Chinese, not Japanese, not Hebrew. And without a word for the color, there is evidence that they may not have seen it at all.

How we realized blue was missing
In "The Odyssey," Homer famously describes the "wine-dark sea." But why "wine-dark" and not deep blue or green?

In 1858 a scholar named William Gladstone, who later became the prime minister of Great Britain, noticed that this wasn't the only strange color description. Though the poet spends page after page describing the intricate details of clothing, armor, weaponry, facial features, animals, and more, his references to color are strange. Iron and sheep are violet; honey is green.

So Gladstone decided to count the color references in the book. And while black is mentioned almost 200 times and white about 100, other colors are rare. Red is mentioned fewer than 15 times, and yellow and green fewer than 10. Gladstone started looking at other ancient Greek texts and noticed the same thing — there was never anything described as "blue." The word didn't even exist.

It seemed the Greeks lived in a murky and muddy world, devoid of color, mostly black and white and metallic, with occasional flashes of red or yellow.

Gladstone thought this was perhaps something unique to the Greeks, but a philologist named Lazarus Geiger followed up on his work and noticed this was true across cultures.

He studied Icelandic sagas, the Koran, ancient Chinese stories, and an ancient Hebrew version of the Bible. Of Hindu Vedic hymns, he wrote: "These hymns, of more than ten thousand lines, are brimming with descriptions of the heavens. Scarcely any subject is evoked more frequently. The sun and reddening dawn's play of color, day and night, cloud and lightning, the air and ether, all these are unfolded before us, again and again ... but there is one thing no one would ever learn from these ancient songs ... and that is that the sky is blue."

There was no blue, not in the way that we know the color — it wasn't distinguished from green or darker shades.

Geiger looked to see when "blue" started to appear in languages and found an odd pattern all over the world.

Every language first had a word for black and for white, or dark and light. The next word for a color to come into existence — in every language studied around the world — was red, the color of blood and wine.

After red, historically, yellow appears, and later, green (though in a couple of languages, yellow and green switch places). The last of these colors to appear in every language is blue.

The only ancient culture to develop a word for blue was the Egyptians — and as it happens, they were also the only culture that had a way to produce a blue dye.
..."

And that's the problem. We don't have a word for change in angular momentum. Well we do, actually - jerk - but that is generally used in relation to linear acceleration and not acceleration towards the centre. Come to think of it they don't have a word for acceleration towards the centre which is why they have to qualify it with the words "towards the centre" since it is a different thing from "acceleration" which is implicitly acceleration in a straight line.

In Cloud Camper's thread I pointed out the same problem arises with heat engines. The fact that heat engines are not HEAT engines but difference in temperature engines - and we don't as far as I know have a word for difference in temperature.

I suppose people would have been in the same difficulty before they had a word for acceleration and had to think of it as a difference in velocity.

What it comes to is that we are only slowly beginning to invent a colour language for motion.
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re: Bessler's secret

Post by Grimer »

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By analysing the boundary conditions for the Milkovic I've discovered how to get Newtonian Gravity (NG) potential energy from Ersatz Gravity (EG) potential energy.

Executive summary

As a pendulum swings through 120° (4 o'clock to 8 o'clock) at the nadir it generates a force on the pivot of twice NG. Half of this force is down to Newtonian Gravity (NG) and the other half is down to Ersatz Gravity (EG).

If the pivot is allowed to move down a distance, d, then the work done is

FNG • d + FEG • d
but
FNG = FEG
so
FNG • d + FEG • d = 2.FNG • d

So the swinging pendulum will lift double the mass of a hanging pendulum on the other side of the beam pivot.

So far so good.

For a repeat cycle we have to lift the pendulum back distance d.
We have twice the work we need to do that.

We can use half the work to lift the pendulum back and the other half is free energy.

Some small fraction of it will be needed to make up for the losses due to air resistance, etc. but the rest is free to drive machinery.

But what about EG? Don't we have to restore that as well?

No.

But surely, when we drop the pivot the velocity of the pendulum bob as it passes through the nadir (through 6 o'clock) will be reduced so the bob won't climb to the 60° angle.

Mmm... that was the point that really had me worried until I saw the answer.
The force vector is in the vertical direction. The velocity vector is in the horizontal direction. The the force vector resolved in the horizontal direction is, ...... F • (cos 90°) which is equal to zero

So no work is needed for EG to reset.
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Post by Grimer »

I can see a way how to modify a Milkovic to give us a Newcomen kind of engine - but I can't see how Bessler can have used this principle to get the circular motion of wheel.

That he used the free EG work available in the swinging weights I have little doubt - but he would also have needed some kind of escapement mechanism (perhaps one should say, entrapment mechanism, since it's the inverse of an escapement) and that would be difficult for a weight both swinging and rotating.
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re: Bessler's secret

Post by Grimer »

I've been giving some more thought on turning the basic action of the Milkovic into an inverted clock mechanism, i.e. one that sends energy back from the infinite gravitational sink to the finite source which is a spring or falling weights, say in the case of a traditional clock.

Fortunately we have an example of such a reversal in the case of the simple Stirling engine so that should encourage us to recognise the possibility.

The most obvious difference between a clock pendulum and the Milkovic pendulum is the amplitude of swing. In a clock this amplitude is kept to the minimum practical since though the effect of amplitude on period is small it is not negligible.

As Cloud points out, we're not concerned with the timekeeping aspects of the pendulum but merely with its generation of jerk energy (Ersatz Gravity- EG). For a swing of 120° (4 o'clock to 8 o'clock) the downward Newtonian Gravity (NG) pull at 6 o'clock is doubled by this jerk contribution.

We have to capture the work potential of this extra force by allowing the combined EG+NG to do work by pulling down the pendulum pivot Milkovic style.

This work then has to be transferred to the other side of the beam pivot and used to increase the NG potential of a static pendulum. In this way EG on the dynamic pendulum side is transduced into NG on the static pendulum side.

The NG component has to be returned to reset the system by lifting the dynamic pendulum pivot to its starting position. This leaves the EG free to do useful work.

To prevent the EG from also being returned as in the conventional Milkovic a suitable entrapment mechanism has to be devised.

I'm drawing up a sketch of a possible mechanism which I will present in a later post.
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Post by cloud camper »

Grimer wrote:I can see a way how to modify a Milkovic to give us a Newcomen kind of engine - but I can't see how Bessler can have used this principle to get the circular motion of wheel.

That he used the free EG work available in the swinging weights I have little doubt - but he would also have needed some kind of escapement mechanism (perhaps one should say, entrapment mechanism, since it's the inverse of an escapement) and that would be difficult for a weight both swinging and rotating.
How bout this idea Frank?

Incoming pulses ratchet the wheel, lever returns with a light spring.

Cheap and easy. Add rim weight as desired.

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Post by Grimer »

That would make a good hour hand for your anti-clock. ;-)
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re: Bessler's secret

Post by marco »

what i could make of it so far.
notice the wheel is locked until all oil has gone up.
also it's a crude diagram some more engineering should allow for a definite direction.[/img]
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re: Bessler's secret

Post by Trevor Lyn Whatford »

Hi CC,

nice bit of engineering, I love bike wheels, and there gears, they form 80% of my builds, recycling old bikes :-)

Marco,

Welcome to the forum.

Oil only floats on Water when it is lighter that water, if the oil is heaver than water then water floats on oil, just a thought.
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re: Bessler's secret

Post by AB Hammer »

marco

First off, Welcome to the forum.

Interesting idea. The weight values of the water and oil can do that. But how to control the catch and release and hopefully don't bleed out sideways as it moves. I would suggest a timer device that the half rotation resets with each release.

Here is one of my old designs that can only be a slow mover as well, but it needs a water source and no guaranties it will work of course.

http://www.besslerwheel.com/forum/downl ... er=user_id
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re: Bessler's secret

Post by Art »

Welcome Marco .

I'm afraid the first problem to solve is one of design due to the principle you are trying to utilise .

No problem getting an oil that floats - from memory most have a specific gravity of about 0.8 which means that the volume of 1 Kg will be one divided by 0.8 times the volume of 1 litre of water ie 1.250 Litres .

Therefore 2 Kg of oil will need a container of 2.500 Litres . When you transfer the water into this container it will be less than half full with a space of 1.500 Litres of either air or vacuum above the water.

If you redraw your diagrams showing this you will see that it changes everything .

For example the first diagram will have 2 Kg of oil on the bottom with the centre of gravity at the centre of the lower container .The upper container will be less than half full of water with the centre of gravity closer to the proposed axle location .

The third diagram will have 1 Kg of water in the bottom 1 Litre of the lower container , the other 1.500 Litres of that container will be filled with oil (1.5 x 0.8 = 1.2 Kg ) and the rest of the oil (1 litre or 0.8 Kg) will be in the lower part of the upper container with a gap of 1.500 Litres of air or vacuum above it . In other words the bottom cylinder will weigh 2.2 Kg and the upper container will weigh 0.8 Kg with the centre of that 0.8 Kg weight almost at the axle of the wheel .

Don't like to pour water on your idea but the Universe can be a hard taskmaster when it comes to building an idea !

I have just finished up the testing tonight of the umteenth attempt to find out what is so special about storksbills .Got a perfect set of negative results for a brilliant (if I may say so myself ) idea that I just had to see built to understand it properly .

I don't feel so bad though because now I can concentrate fully on the design to test my current next brilliant idea which came to me last week as I vacantly stared at some posts in this forum which had very little relationship to that idea . Ideas come from the funniest places sometimes ! : )

Anyway don't be discouraged , Fluids / Specific Gravities / Atmospheric pressures are well worth investigating ,

All the best with the pursuit !
Have had the solution to Bessler's Wheel approximately monthly for over 30 years ! But next month is "The One" !
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