Dual Op Amp
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To be continued...Don't stop there, continue please.
For Zapperz:
This part knew, not all of it, but this part.
The answer to why a certain configuration fo electrons are more stable than others is pretty complicated, and if you are looking for a one or two sentence answer, others have provided some good ones. I will try to give more detailed understanding.
First of all, a five minute introduction to quantum mechanics. Classically, energy can be absorbed or emitted in any amount. For example, I can hit a pool ball at 1 m/s, 1.5 m/s, 2 m/s or any value in between. However, when physicists tried to apply classical mechanics to small pecies such as atoms, there arose three problems: (1) Black Body Radiation(also called The Ultraviolet Catastrophe), (2) The Photoelectric Effect and what I call (3) The Electron Orbital Catastrophe. (1) and (2) are quite involved, but let me see if I can explain (3) briefly . By that time (circa 1900) the results of Rutherford's experiments had shown that the atom consisted of a small, positively charged nucleus surrounded by negatively charged electrons. They then began to theorize how the electrons moved about the nucleus. In the Bohr model, you can imagine the atom as forming a minuature planetary system, where the electrons rotate around the nucleus in more or less circular orbits. As you will learn later in physics moving charges should radiate electromagnetic energy, so the electron as it revolves, or moves somehow about the nucleus should lose energy and crash into the nucleus. Clearly that does not happen.
The failure of the classical theory to these phenomenon led physicists, among them Max Plank, to develop a model whereby energy could only be omitted in certain bundles, or quanta. These quanta are represented by photons (light, radio, and other electromagnetic radiation) The energy carried by a photon is equal to E = hv, where h is the universal constant called Plank's constant. and v is the greek leter "nu" standing for frequency. It turns out that small particles like electrons, protons, atoms, and molecules are not like pool balls. They can only absorb quantized energy. In other words, they can only absorb or emit photons, and in addtion only photons or a certain wavelength or frequency. Since the particles can only absorb energy in certain bundles, we can speak of energy 'states' at which the particle has absorbed n = 1, 2, 3 ... etc. photons. The state in which the particle can emit no more photons is said to be its 'ground' state, n = 1. As the particle absorbs the photon, it gains energy. As it loses energy, it will re-emit the photon. This effect can easily be seen in light bulbs: a filiament is heated, which excites an electron. The electron will return to its ground state and re-emit the photon, which produces light in the visible spectrum. Knowing the charge and mass of the proton and electron allows us to calculate these energy levels, using the principles of electromagnetic theory.
But first, we have another problem, and it has to do with something called Wave-Particle Duality. For a very long time, physicists were debating over what light consisted of. Newton suspected it consisted of particles, which he called corpsucles. Others such as Robert Hooke, one of Newton's contemporaries, believe it to be carried by a wave. By the middle of the 19th century it appeared the question was settled when Henry performed his infamous double slit experiment. When you pass a wave through a small aperture that is on the order on the wavelength of the wave, you get a phenomenon known as diffraction. This means that the wave spreads out like it originated from a point source. You can then detect the intensity of the wave(related to its amplitude) at some distance from the apeture. Waves also exhibit another property called interference. This means that waves can pass through one another, and as they do they will add or subtract together. You can see this phenomenon if you get a long rope or slinky, hold it fixed at one end, and then send one wave down it and another a short time afterwards. You will observe the two waves interfere with each other as they meet, then pass through one another. If you are still not convinced(they could merely be rebounding off of each other), send a small wave then a big one. If you do the calculations as you pass a wave through two slits, you can calculate what the intensity will be at a plane that is some distance from the slits and parallel to both slits. You should get a 'band' pattern, where you have alternating fringes of constructive and destructive interference. Well when Henry performed his experiment, he detected these bands of light, and it was accepted that light traveled as a wave.
For Zapperz:
This part knew, not all of it, but this part.
The answer to why a certain configuration fo electrons are more stable than others is pretty complicated, and if you are looking for a one or two sentence answer, others have provided some good ones. I will try to give more detailed understanding.
First of all, a five minute introduction to quantum mechanics. Classically, energy can be absorbed or emitted in any amount. For example, I can hit a pool ball at 1 m/s, 1.5 m/s, 2 m/s or any value in between. However, when physicists tried to apply classical mechanics to small pecies such as atoms, there arose three problems: (1) Black Body Radiation(also called The Ultraviolet Catastrophe), (2) The Photoelectric Effect and what I call (3) The Electron Orbital Catastrophe. (1) and (2) are quite involved, but let me see if I can explain (3) briefly . By that time (circa 1900) the results of Rutherford's experiments had shown that the atom consisted of a small, positively charged nucleus surrounded by negatively charged electrons. They then began to theorize how the electrons moved about the nucleus. In the Bohr model, you can imagine the atom as forming a minuature planetary system, where the electrons rotate around the nucleus in more or less circular orbits. As you will learn later in physics moving charges should radiate electromagnetic energy, so the electron as it revolves, or moves somehow about the nucleus should lose energy and crash into the nucleus. Clearly that does not happen.
The failure of the classical theory to these phenomenon led physicists, among them Max Plank, to develop a model whereby energy could only be omitted in certain bundles, or quanta. These quanta are represented by photons (light, radio, and other electromagnetic radiation) The energy carried by a photon is equal to E = hv, where h is the universal constant called Plank's constant. and v is the greek leter "nu" standing for frequency. It turns out that small particles like electrons, protons, atoms, and molecules are not like pool balls. They can only absorb quantized energy. In other words, they can only absorb or emit photons, and in addtion only photons or a certain wavelength or frequency. Since the particles can only absorb energy in certain bundles, we can speak of energy 'states' at which the particle has absorbed n = 1, 2, 3 ... etc. photons. The state in which the particle can emit no more photons is said to be its 'ground' state, n = 1. As the particle absorbs the photon, it gains energy. As it loses energy, it will re-emit the photon. This effect can easily be seen in light bulbs: a filiament is heated, which excites an electron. The electron will return to its ground state and re-emit the photon, which produces light in the visible spectrum. Knowing the charge and mass of the proton and electron allows us to calculate these energy levels, using the principles of electromagnetic theory.
But first, we have another problem, and it has to do with something called Wave-Particle Duality. For a very long time, physicists were debating over what light consisted of. Newton suspected it consisted of particles, which he called corpsucles. Others such as Robert Hooke, one of Newton's contemporaries, believe it to be carried by a wave. By the middle of the 19th century it appeared the question was settled when Henry performed his infamous double slit experiment. When you pass a wave through a small aperture that is on the order on the wavelength of the wave, you get a phenomenon known as diffraction. This means that the wave spreads out like it originated from a point source. You can then detect the intensity of the wave(related to its amplitude) at some distance from the apeture. Waves also exhibit another property called interference. This means that waves can pass through one another, and as they do they will add or subtract together. You can see this phenomenon if you get a long rope or slinky, hold it fixed at one end, and then send one wave down it and another a short time afterwards. You will observe the two waves interfere with each other as they meet, then pass through one another. If you are still not convinced(they could merely be rebounding off of each other), send a small wave then a big one. If you do the calculations as you pass a wave through two slits, you can calculate what the intensity will be at a plane that is some distance from the slits and parallel to both slits. You should get a 'band' pattern, where you have alternating fringes of constructive and destructive interference. Well when Henry performed his experiment, he detected these bands of light, and it was accepted that light traveled as a wave.