In order to provide sense and meaning to the probability approach, Schrödinger in1926 derived on equation known after his name as Schrödinger's wave equation. This equation is the basic of wave mechanics and is based upon the idea of the electron as standing wave around the nucleus. If the electron has wave like nature, it should obey the same equation of motion as all other known type of wave. On the basis of simple idea Schrödinger derived an equation which describes the wave motion of an electron wave along of the three axis x, y, z called Schrödinger wave equation.
Schrödinger's wave equation correlates the wave property of the electron with its energy. During the derivation of this equation, he took the following under consideration.
1. de-Broglie's wave particle duality equation
2. Heisenberg's uncertainty principle
3. Bohr's concept of quantized energy levels.
The equation for the standing wave comparable with that of a stretched string is
Where,. (sigh) = amplitude at displacement x and is wave function
A = constant
x = displacement direction
l = wavelength.
Differentiating eq (i) twice with respect to x we get,
As total energy (E) = KE + PE
Again
According to de-Broglie's equation
Putting the value of v2 from eq (iii) on eq (iv) we get,
Putting the value of eq (v) on eq (ii) we get
Equation (vi) is a Schrödinger wave equation for the wave motion in one dimension only ie x-axis. For electron moving in a three dimension space it is modified as:
Where Ñ2 (del-square)[Laplacian operator] =
Equation (vii) and (viii) are Schrödinger wave equation expressions.
The valid values of are called Eigen functions, and the values of E corresponding to this Eigen functions are called Eigen values. The Eigen values are found to be more or less the same energy values given by Bohr's in different orbit.
For to be valid it should satisfy following conditions:
i. must be finite and continuous
ii. It should be single valued
iii. must be continuous functions of x, y, and z coordinates respectively.
represent the three dimensional amplitude of electron wave at various points surrounding the nucleus, and is called orbital. However, 2, gives the probability of finding electron of certain energy at a space inside the atom.
The value of may be real or imaginary. If is real, 2 also is real. Thus 2 gives the probability of finding electron.
But if is imaginary * gives the probability of finding electron wave
let = a + ib (imaginary quantity)
* = (a+ib) (a–ib) = a2+b2 (real)
Note: The probability should always be real and positive.
How can you take sigh(symbol) independent of time, as you have assumed sigh(symbol) as amplitude of standing wave at a point which also depends on the time
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