Derivations
Understanding Schrödinger’s Time Independent Equation!!! Corner-stone equation of quantum-mechanics....!!!
Till now we were discussing only the
theoretical part of the quantum mechanics…. But now it's time to understand the
maths behind all this drama in a simple way.
All starts with the classical wave
equations. It is the root cause of all the thought process regarding the
derivation of Schrödinger’s equations….
∂^2y/∂t^2 = v^2∂^2y/∂x^2
So, can we convert the classical wave
equation and modify it in such a way by which we can accommodate the
characteristics of quantum matter waves???
The simple answer is no. Strings
exhibit wave phenomenon as a whole; y and v in the above equation refer to
amplitude and speed respectively.
Erwin Schrödinger |
Schrödinger took assumptions that the
quantum wave equation should have two properties. As we have seen in classical
wave equation that the wave equation should have a linear and second-order
differential equation and the success of Bohr’s model argued for retaining the
concept of energy conservation.
In classical physics, the conservation
of mechanical energy is expressed by,
E= p^2/2m +V(x) ……….. (1)
Remember, when we were discussing about
harmonic motion in elementary physics texts, we often encounters solutions of
the wave equation of the form
y= Asin (kx-wt) …...……. (2)
Now,
one more equation we need to establish the relation between the classical wave
to quantum-mechanical matter waves, and that is the de Broglie relation,
λ=h/p
…………..(3)
Also, we know from wave mechanics that,
k=2π/ λ
.………… (4)
from equation 2,3 and 4,
y=A sin {(p/ ħ)x – wt}
Now, double differentiating it with respect to x,
p^2= - ħ^2/y(∂^2y/∂x^2) ……………(5)
p^2= - ħ^2/y(∂^2y/∂x^2) ……………(5)
Now, putting equation 5 in equation 1,
- ħ^2/2m(∂^2y/∂x^2) + V(x)y=E y …………….(6)
Now, we can see that this equation is a non-relativistic,
one-dimentional, time-independent Schrödinger’s
equation which is also known as Schrödinger’s Wave
equation. Here, if you observe carefully then you can see that here there is no
mention about the wavefunction.
This equation works fine for a pulse travelling on a string but when you
are taking about atoms and molecules then you should mention about 3-D space.
So, what Schrödinger did actually
to solve this problem????
By intuition equation 6 can be represented in a 3-D form by adding second
partial derivatives of the wave pattern with respect to y and z to the left
side.
So, finally we get the 3-D form of Schrödinger’s
Time Independent Equation,
- ħ/2m(∂^2Ψ
/∂x^2+∂^2Ψ /∂y^2+∂^2Ψ
/∂z^2) + V Ψ =E Ψ
But, here story doesn’t end…..
Anyone who knows the basic aspects of
physics must have noticed following curious aspects from the final equation:-
1) Classical Wave equation was in fact never
used. It only used as a prototype
wavefunction.
2) Nowhere the concept of quantization
built into development. It only can be
seen by solving the equation for a set of values of V(x, y, z) and set
of boundary conditions
3) The total energy E appears explicitly
in the final equation which is unusual for
classical physics as in Newton’s second law i.e. F=ma, there is no
mention of E.
We can calculate that by providing boundary conditions like ignition position
and speed of the particle involved after solving the differential equation.
For a given set of V(x, y, z) and set
of boundary conditions there exist certain values of Ψ(x, y, z) that satisfy the equation and each
values gives a particular value of E. This set of values of E represent the
quantized energy states of the system.
In my next
articles on quantum-verse, I am going to explain the need of time-dependent
equation of Schrödinger and also going to derive it. So, don’t forget to subscribe to our website and follow me on social media for updates…..
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Thanks for reading.....
See you next time!!!
-Ratnadeep Das Choudhury
Founder and Writer of The Dynamic Frequency
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