A simple electric heater, which has efficiency greater than 1
Moderator: scott
re: PERPETUAL FLOATING TURD THREAD
That's a false dilemma.
If the peterless wonder actually had some fantastic idea he'd take it to market in
a multi-billion dollar industry and change the world instead of fighting windmills.
Speaking of windmills, they have a CoP close to infinity.
Put that in your electrolysis process and ionize it.
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this is a test
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If the peterless wonder actually had some fantastic idea he'd take it to market in
a multi-billion dollar industry and change the world instead of fighting windmills.
Speaking of windmills, they have a CoP close to infinity.
Put that in your electrolysis process and ionize it.
...................................................................................................................
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this is a test
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........................¯\_(ツ)_/¯
¯\_(ツ)_/¯ the future is here ¯\_(ツ)_/¯
Advocate of God Almighty, maker of heaven and earth and redeemer of my soul.
Walter Clarkson
© 2023 Walter W. Clarkson, LLC
All rights reserved. Do not even quote me w/o my expressed written consent.
¯\_(ツ)_/¯ the future is here ¯\_(ツ)_/¯
Advocate of God Almighty, maker of heaven and earth and redeemer of my soul.
Walter Clarkson
© 2023 Walter W. Clarkson, LLC
All rights reserved. Do not even quote me w/o my expressed written consent.
- MrTim
- Aficionado
- Posts: 922
- Joined: Thu Nov 06, 2003 11:05 pm
- Location: "Excellent!" Besslerwheel.com's C. Montgomery Burns
- Contact:
re: A simple electric heater, which has efficiency greater t
Ah-ha, I now know where PeterAX has lifted his 'formulas' from.
Prof. S. L. Srivastava's Solved Problems of Bong Theory and Physics
PeterAX has merely replaced bong terminology in the formulas with science-y electrical terms (he's still wrong, of course, and laughably.)
Much more importantly, PeterAX has neglected exhaling from his calculations. So his 'simple electric heater' (i.e bong) only works as he promises if you don't exhale, so to speak. Nice trick, if it could work.
So to him I say : Breathe, PeterAX, breathe! Free your constipated brain from the inhaled fog surrounding it! We all worry for you...!
;-)
Prof. S. L. Srivastava's Solved Problems of Bong Theory and Physics
PeterAX has merely replaced bong terminology in the formulas with science-y electrical terms (he's still wrong, of course, and laughably.)
Much more importantly, PeterAX has neglected exhaling from his calculations. So his 'simple electric heater' (i.e bong) only works as he promises if you don't exhale, so to speak. Nice trick, if it could work.
So to him I say : Breathe, PeterAX, breathe! Free your constipated brain from the inhaled fog surrounding it! We all worry for you...!
;-)
"....the mechanism is so simple that even a wheel may be too small to contain it...."
"Sometimes the harder you look the better it hides." - Dilbert's garbageman
re: A simple electric heater, which has efficiency greater t
To MrTim and to WaltzCee.
======================
You both have really some severe mental problems. You both really need to see your doctor. You both really need a psychiatry help. You both really need an intensive medical treatment. I am serious.
======================
You both have really some severe mental problems. You both really need to see your doctor. You both really need a psychiatry help. You both really need an intensive medical treatment. I am serious.
re: A simple electric heater, which has efficiency greater t
"You need to see your doctor".....That is Georges mating call.
re: A simple electric heater, which has efficiency greater t
To Tarsier79.
==================
Hi Nobel prize winner number 3,
It's always a great pleasure to correspond with you!
But why it seems to me that one and same psychiatric hospital patient uses three different pseudonims simultaneously and these three different pseudonims are Tarsier79, MrTim and WaltzCee, respectively?
==================
Hi Nobel prize winner number 3,
It's always a great pleasure to correspond with you!
But why it seems to me that one and same psychiatric hospital patient uses three different pseudonims simultaneously and these three different pseudonims are Tarsier79, MrTim and WaltzCee, respectively?
re: A simple electric heater, which has efficiency greater t
To Tarsier79.
==================
Hi Nobel prize winner number 3,
It's always a great pleasure to correspond with you!:)
But why it seems to me that one and same psychiatric hospital patient uses three different pseudonims simultaneously and these three different pseudonims are Tarsier79, MrTim and WaltzCee, respectively?:)
==================
Hi Nobel prize winner number 3,
It's always a great pleasure to correspond with you!:)
But why it seems to me that one and same psychiatric hospital patient uses three different pseudonims simultaneously and these three different pseudonims are Tarsier79, MrTim and WaltzCee, respectively?:)
- MrTim
- Aficionado
- Posts: 922
- Joined: Thu Nov 06, 2003 11:05 pm
- Location: "Excellent!" Besslerwheel.com's C. Montgomery Burns
- Contact:
re: A simple electric heater, which has efficiency greater t
Exhale, PeterAX, exhale! Your bong smoke has clouded your mind. Clear it out before the spiders start to eat you...
"....the mechanism is so simple that even a wheel may be too small to contain it...."
"Sometimes the harder you look the better it hides." - Dilbert's garbageman
re: A simple electric heater, which has efficiency greater t
To MrTim.
====================
Take your medicine!:) Triple dose!:)
====================
Take your medicine!:) Triple dose!:)
re: A simple electric heater, which has efficiency greater t
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
Looking forward to your answer.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
Looking forward to your answer.
re: A simple electric heater, which has efficiency greater t
Start:
 Do while red dots<3
(
Paste_ridiculous_Information:
   ".....Looking forward to your answer."
   If "Answer" = positive then insert flattery, else make comment on Nobel Prize Winner or Take Medicine.
Goto "Paste_ridiculous_Information")
Loop
Create new user account
Goto Start
 Do while red dots<3
(
Paste_ridiculous_Information:
   ".....Looking forward to your answer."
   If "Answer" = positive then insert flattery, else make comment on Nobel Prize Winner or Take Medicine.
Goto "Paste_ridiculous_Information")
Loop
Create new user account
Goto Start
re: A simple electric heater, which has efficiency greater t
I have nearly figured out the programming for Georgebot
re: A simple electric heater, which has efficiency greater t
To Tarsier79.
===================
You are really very, very sick!:) You reject the validity of numerous real experiments! You reject the validity of physical reality! I'll call your doctor! You are a really dangerous mad person!:)
===================
You are really very, very sick!:) You reject the validity of numerous real experiments! You reject the validity of physical reality! I'll call your doctor! You are a really dangerous mad person!:)
re: A simple electric heater, which has efficiency greater t
PLEASE NOTE -- THE TEXT BELOW DESCRIBES REAL EXPERIMENTS!
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES REAL EXPERIMENTS!
===============================
Looking forward to your answer.
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES REAL EXPERIMENTS!
===============================
Looking forward to your answer.
re: A simple electric heater, which has efficiency greater t
PLEASE NOTE -- THE TEXT BELOW DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
===============================
Looking forward to your answer. (It's impossible to reject obvious physical reality.)
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being described in our previous post) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
===============================
Looking forward to your answer. (It's impossible to reject obvious physical reality.)
re: A simple electric heater, which has efficiency greater t
PLEASE NOTE -- THE TEXT BELOW DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being already described above) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
===============================
Looking forward to your answer for the 2nd time. (It's impossible to reject obvious physical reality.)
======================
Here is a detailed description of our first group of experiments.
======================
======================
EXPERIMENT 1.
1) A standard copper wire (a standard SOLID conductor) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through a copper wire of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the copper wire, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the copper wire, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
=======================
=======================
EXPERIMENT 2.
1) A standard sulphuric acid solution (a standard LIQUID conductor/a standard electrolyte) is connected to a standard DC source thus forming a circuit.
2) The circuit is equipped with a standard ammeter and with a standard ohmmeter. Besides we have at our disposal a standard chronometer.
3) The ammeter registers a current of 7.98 A.
4) The ohmmeter registers an Ohmic resistance of 0.5 Ohm.
5) The chronometer registers a time interval of 1 second. (A current of 7.98 A flows through an electrolyte of Ohmic resistance of 0.5 Ohm within a period of 1 second.)
6) Using (a) the above three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) the first Joule's law of heating we can easily calculate that:
a) the electric energy, consumed by the electrolyte, is just equal to 31.84 J;
b) the so called Joule's heat, generated by the electrolyte, is just equal to 31.84 J too.
7) Please note that in order to get the amount of generated Joule's heat of 31.84 J we need solely and only (a) three experimental results (7.98 A, 0.5 Ohm and 1 second) and (b) three measuring devices (an ammeter, an ohmmeter and a chronometer). No electric engineer in the world would measure the generated heat of 31.84 J by using of calorimetry methods. Every electric engineer in the world would take for granted this generated heat of 31.84 J. Because otherwise he/she would accept the fact that the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor) is not valid.
-------------------------------------------
(Note. It is evident that the last items 1 - 7 of this Experiment 2 are absolutely identical to items 1 - 7 of previous Experiment 1. The latter is a clear manifestation of the first Joule' law of heating, which has been experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor.)
-------------------------------------------
8/ While a current of 7.98 A flows through the electrolyte within a period of 1 second however a certain amount of hydrogen has been generated. The mass of the generated hydrogen is just equal to 0.0000000833112 kg as follows from the first Faraday's law of electrolysis.
9) Please note that in order to get the mass of the released hydrogen we need solely and only (a) two experimental results (7.98 A and 1 second) and (b) two related measuring devices (an ammeter and a chronometer). No expert in electrochemistry in the world would measure the mass of the generated hydrogen by using of balance, scales or any other weighing machine. Every expert in electrochemistry in the world would take for granted this mass of 0.0000000833112 kg. Because otherwise he/she would accept the fact that the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years) is not valid.
10) If we burn/explode the released hydrogen, then a certain amount of heat would be generated. And this heat would be just equal to 11.83 J . In other words, we can write down the equality
H = (HHV) x (m) = 11.83 J,
where
H = heat generated by burning/exploding of the released hydrogen
HHV = higher heating value of hydrogen = 142 MJ/kg
m = mass of the released hydrogen = 0.0000000833112 kg
11) Please note that no expert in thermodynamics in the world would measure the generated heat of 11.83 J by using of calorimetry methods. Every expert in thermodynamics in the world would take for granted this generated heat of 11.83 J. Because otherwise he/she would accept the fact that the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years) is not valid.
12) In one word, on one hand we have a consumed electric energy of 31.84 J and this is the inlet energy. On the other hand we have (a) Joule's heat of 31.84 J and (b) heat H of 11.83 J, which is generated by burning/exploding of the released hydrogen. The sum of the two last pieces of energy is just equal to the outlet energy.
13) Therefore we can write down the inequalities
(31.84 J) + (11.83 J) > 31.84 J <=> 43.67 J > 31.84 J <=> outlet energy > inlet energy.
14) For the efficiency/COP of the above described process we can write down the equality
efficiency = COP = (43.67 J)/(31.84 J) = 1.37
15) And it is evident that COP = 1.37 <=> COP > 1.
==============================
==============================
SUMMARY.
1) The above experimental results for inlet and outlet energies are based on:
a) the readings of three standard measuring devices (an ammeter, an ohmmeter and a chronometer);
b) the validity of the first Joule's law of heating (experimentally proved millions of times within a period of 200 years for any standard solid, liquid or gaseous conductor);
c) the validity of the first Faraday's law of electrolysis (experimentally proved millions of times within a period of 200 years for any standard electrolyte);
d) the validity of the value of the hydrogen's HHV (experimentally proved millions of times within a period of 200 years).
2) In one word, having in mind the text above we can conclude that any of the millions (either industrial or laboratory) standard electrolyzers all over the world is actually a heater, which has COP/efficiency greater than 1.
-----------------------------------------------------
(Note. Any standard (either industrial or laboratory) electrolyzer could be designed as a built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger. In this way there would be more emphasis on cramming more heat-transfer surfaces into less and less volume. This approach could be suitable for a better utilization of the released Joule's heat. Besides the same built-with-fin-tubes (i.e. with extended-surfaces) heat exchanger design could be used for the box/container, in which the burning of the released hydrogen would take place. In this way as if there would be a better utilization of the heat, generated by the burning of the released hydrogen.)
------------------------------------------------------
3) If the first Joule's law of heating and/or the first Faraday's law of electrolysis and/or the value of the hydrogen's HHV proved to be experimentally invalid, then this fact would lead to the creation of entirely new and revolutionary branch of science and technology. The latter would be a wonderful alternative too.
===============================
===============================
That's all about our first group of experiments.
===============================
===============================
And here is a short description of our second group of experiments.
1) Actually our second group of experiments is absolutely identical to our first group of experiments (the latter being already described above) with the only difference that Ohmic resistance is decreased 10 times and as a result the ohmmeter registers an Ohmic resistance of 0.05 Ohm. In this case:
a) the consumed electric energy is equal to 3.184 J;
b) the generated Joule's heat is equal to 3.184 J too;
c) the heat, generated by the burning/exploding of the released hydrogen, is equal to 11.83 J (which is just the same as in our first group of experiments),
2) So for efficiency/COP we can write down the equalities
COP = ((3.184 J) + (11.83 J))/(3.184 J) <=> COP = (15.014 J)/(3.184 J) <=> COP = 4.72
3) It is evident that
COP = 4.72 <=> COP > 1.
4) In one word, (keeping constant current I and time period t) the smaller the Ohmic resistance R, the bigger the efficiency/COP.
===============================
===============================
There is a third group of experiments of ours, which has even a greater scientific, technology and commercial value than the above described two groups of experiments of ours. But for the present we would not like to reveal the secret of our third group of experiments.
===============================
===============================
PLEASE NOTE -- THE TEXT ABOVE DESCRIBES SOLELY AND ONLY REAL EXPERIMENTS!
===============================
Looking forward to your answer for the 2nd time. (It's impossible to reject obvious physical reality.)