Godwin Kessy said:
May anyone help me with these questions
1 why is a dipole neutral as it completely resembles a system of two charges
because the charges are equal and opposite ... actually, that is only the case for dipoles in electrically neutral systems ... there is no restriction that dipoles cannot be defined for electrically charged systems. To create a dipole, you just need a non-isotropic charge distribution.
2 i know probably its very advanced, but can anyone give me out a scope on wave function and its relation to energy of an orbital
Hmmm ... not sure what you are asking here. However, in general, the wavefunctions describing the characteristic states (eigenstates in QM parlance) of any quantum system is related to the energy is a very fundamental way, according to the time-independent Schrodinger equation, which says:
\hat{H}\psi=E\psi,
where "H" is the Hamiltonian operator. It's correct definition is indeed technical, but if you can stand a little math, for a simple 1-D system, the expanded version of this equation is:
\frac{\partial^{2}\psi\left(x\right)}{\partial x^{2}} + \frac{2m}{\hbar^2}\left[E-V\left(x\right)\right]\psi\left(x\right)=0
So it is just a simple 2nd-order differential equation, where m is that mass of the particle, E is the total energy, and V(x) is the potential energy, which can be a variable function of position. For a bound system (e.g. and electron orbiting an atom), there are only certain values of E that will satisfy this equation ... these are the characteristic energies (or energy eigenvalues). For each characteristic energy, there is also a characteristic wave-function \psi(x) (called an eigenfunction or eigenstate).
Does that help?
3 am not sure if this is the right forum to ask this question but why is dipole moment a vector quantity! Actualy how do we determine the nature of a quantity!
Dipole moment is a vector because both its direction and its magnitude are significant. Just imagine a simple diatomic molecule AB, which has a dipole moment, which we can understand in terms of partial charges on each of the atoms, one positive and an equally large negative partial charge. Now, the physical and chemical properties of that molecule will be different depending on whether the partial positive charge is on atom A, or on atom B.
More generally, if you consider a discrete collection of charges in space, the dipole moment is given by:
\vec{\mu}=\sum_{i}q_{i}\vec{r_{i}}
where q
i is the value of each point charge (positive or negative), and the vector quantity r
i defines the position of each charge relative to some common origin.
Clear?