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Unformatted text preview: Physical Chemistry Course Number: C362 5 The timedependent Schrodinger Equation h t ( x, t ) = H ( x, t ) (5.1) where, H is called the Hamiltonian operator. It is the operator in quantum me chanics that corresponds to the energy of the system. In quantum mechanics, every physically measurable quantity, has a corresponding operator. The operator H can be written as a sum of the kinetic and potential energy: H = K + V = p 2 2 m + V (5.2) Now if we substitute the momentum operator in Eq. ( 4.4 ), i.e. p = h x , we can write down the Hamiltonian operator as H = p 2 2 m + V = 1 2 m bracketleftBigg h x bracketrightBigg 2 + V = h 2 2 m 2 x 2 + V (5.3) where h 2 2 m 2 x 2 = 1 2 m bracketleftBig h x bracketrightBig 2 is the kinetic energy operator. The timedependent Schrodinger Equation ( 5.1 ) can be rationalized from the waveparticle duality. We will proceed to show this below. 1. As a result of the waveparticle duality, let us write ( x, t ) as a collection of waves. h ( x ) = integraldisplay dpf ( p ) exp braceleftBigg p h x bracerightBigg (5.4) Such a collection of waves, or packet of waves, is called a wavepacket. 2. Note further that waves exp { kx } are eigenstates of the momentum operator. 3. h ( x ) in Eq. ( 5.4 ) does not have a timedependence. So, we go ahead and mul tiply Eq. ( 5.4 ) by the quantity exp { t } = exp braceleftBig E h t bracerightBig so as to maintain the same waveform as in Eq. ( ?? ), ( x, t ) = integraldisplay integraldisplay dpdEf ( p ) g ( E ) exp braceleftBigg bracketleftBigg p h x E h t bracketrightBiggbracerightBigg (5.5) Why is this okay? 4. Go ahead substitute the right hand side of Eq. ( 5.5 ) into Eq. ( 5.1 ) to see what happens. (Forget about V for now.) Chemistry, Indiana University 23 c circlecopyrt 2011, Srinivasan S. Iyengar (instructor) Physical Chemistry Course Number: C362 5. Differentiating Eq. ( 5.5 ) twice with respect to x we obtain: h 2 2 m 2 x 2 ( x, t ) = h 2 2 m 2 x 2 integraldisplay dpdEf ( p ) g ( E ) exp braceleftBigg bracketleftBigg p h x E h t bracketrightBiggbracerightBigg = h 2 2 m integraldisplay integraldisplay dpdEf ( p ) g ( E ) bracketleftBigg p...
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 Winter '11
 AmarFlood

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