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In 1924, the French scientist Louis de Broglie pointed out that in many ways the behavior of Bohr’s quantized electron orbits was similar to the known behavior of waves. The Heisenberg Uncertainty Principle The Heisenberg uncertainty principle states that it is impossible to determine the position and velocity of an electron at the same time. The Schrödinger Wave Equation Provides a mathematical model to describe the motion of particles like electron as waves which supports quantum theory. The Bohr model was a one-dimensional model that used one quantum number to describe the electrons in the atom. Only the size of the orbit was important in the Bohr Model, which was described by the n quantum number. Schrödinger described an atomic model with electrons in three dimensions. This model required three coordinates, or three quantum numbers, to describe where electrons could be found. The three coordinates from Schrödinger's wave equations are the principal quantum number (n), angular quantum number (l), and magnetic quantum number (m). These quantum numbers describe the size, shape, and orientation in space of the orbitals of an atom. We will come back to the Quantum Numbers shortly, but first a word from Our Sponsor: The Standing wave: de Broglie Wave Wave Behavior Interference: When waves overlap each other and change to become one final wave Diffraction: The bending of a wave as it passes by the edge of an object Derived from the wave Particle Duality The Basis for Quantum Theory wave properties of electrons and other very small particles are described mathematically The Bohr model: The first model to incorporate all of the particles of an atom, it is a stepping stone to the modern model of the atom. Bohr used hydrogen for his example; this meant that he only modeled the principle quantum number. Schrödinger described an atomic model with electrons in three dimensions. He took the Bohr model to the next level. Electron Wave Behavior as a standing wave “de Broglie Wave”. Electrons as de Broglie waves Returning now to the problem of the atom, it was realized that if, for a moment, we pictured the electron not as a particle but as a wave, then it was possible to get stable configurations. Imagine trying to establish a wave in a circular path about a nucleus. One possibility might look like the illustration to the left. Figure 12.2: This is an unstable wave orbit; for this configuration, the wave starts at a given point of the orbit, and ends up after one complete revolution at a different point on the wave. The incoming wave will then be out of phase with the original wave, and destructive interference will occur; which will destroy the wave Imagine a rollercoaster ride; the operators have a switch that can divert the rollercoaster cars off the rollercoaster. This is like the unstable wave orbit, it cannot return to the same spot in the wave. This is what happens in destructive interference, the “electron” car is knocked out of orbit. However, certain stable configurations are possible, as is illustrated below; the wave ends up in phase with the original wave after one complete revolution, and constructive interference results. Such a pattern would result in a stable orbit. These types of wave are called a standing wave, and are common in other contexts; for example, they can be established on a string attached to a wall if the string is moved up and down at exactly the right speed (such a wave would appear not to be moving, which is why it's called a standing wave). HOWEVER Imagine a rollercoaster ride again; this time the operators leave the rollercoaster cars on the rollercoaster. This is like the stable wave orbit, it will return to the same spot in the wave. The “electron” car will follow the orbit – the electron stays in the energy level (on the ladder rung). Now back to Quantum Numbers. Schrödinger’s Quantum Numbers 1. Principal (shell) quantum number - n • Describes the energy level within the atom. • Energy levels are 1 to 7 • Maximum number of electrons in n is 2 n2 Schrödinger’s Quantum #’s Principal: the higher the n value the higher the energy; and the lower in the periodic table the element is. For example if n=3 the element’s highest energy is more than an element with n=2 2. Momentum (subshell) quantum number - l • Describes the sublevel in n Sublevels in the atoms of the known elements are s - p - d - f Each energy level has n sublevels. Sublevels of different energy levels may have overlapping energies. • The momentum quantum number also describes the shape of the orbital. Orbitals have shapes that are best described as spherical (l = 0), polar (l = 1), or cloverleaf (l = 2). Orbitals take on even more complex shapes as the value of the angular quantum number becomes larger. Momentum quantum number: l States the shape of “subshells” The number of “subshells” is equal to the energy level (The Principal Quantum # - n) The subshells are: s (l=0); p (l=1); d (l=2); f (l=3) Subshells describe the shape of the orbitals The d and f orbitals are complex 3. Magnetic quantum number - m Describes the orbital within a sublevel s has 1 orbital d has 5 orbitals p has 3 orbitals f has 7 orbitals Orbitals contain 0, 1, or 2 electrons, never more. m also describes the direction, or orientation in space for the orbital. This diagram shows the three possible orientations of a p orbital - px, py, pz. Atomic orbitals are studied in more detail in college. 4. Spin quantum number - s This fourth quantum number describes the spin of the electron. • Electrons in the same orbital must have opposite spins. • Possible spins are clockwise or counterclockwise. • The spin number is arbitrarily assigned the numbers + ½ and – ½ # of Sublevel orbitals s (l=0) p (l=1) d (l=2) “m” values 1 3 5 7 0 -1, 0, 1 -2, -1, 0, 1, 2 -3, -2, -1, 0, f (l=3) 1, 2, 3 9 -4, -3, -2, -1, g (l=4) 0, 1, 2, 3, 4 Orbitals contain 0, 1, or 2 electrons # of Max # of orbitals electrons Sublevel s (l=0) 1 2 p (l=1) 3 6 d (l=2) 5 10 f (l=3) 7 14 g (l=4) 9 18 spin number + ½ called up spin spin number – ½ called down spin In Conclusion: The first three quantum numbers: the principal quantum (n), the angular quantum number (l) and the magnetic quantum number (m) are integers. The principal quantum number (n) cannot be zero: n must be 1, 2, 3, etc. The angular quantum number (l) can be any integer between 0 and (n – 1). For n = 3, l can be 0, 1, or 2. (only one of these values) The magnetic quantum number (m) can be any integer between -l and +l. For l = 2, m can be – 2, – 1, 0, +1, or +2. The spin quantum number (s) is arbitrarily assigned the numbers + ½ or – ½