The quantum mechanical model of the hydrogen atom requires that if the principal quantum number is 4, the number of different permitted orbital quantum numbers will be:
Four
The quantum mechanical model provides a detailed description of the behavior of electrons within atoms, including the simplest atom, hydrogen. This model uses a set of quantum numbers to precisely define the state and properties of an electron. Understanding these quantum numbers is fundamental to comprehending atomic structure.
Let's focus on the two main quantum numbers relevant to this question:
The question asks for the number of different permitted orbital quantum numbers when the principal quantum number for the hydrogen atom is 4.
We are given:
According to the rules of the quantum mechanical model, the allowed values for the orbital quantum number (l) are calculated using the formula:
\(l = 0, 1, 2, ..., (n-1)\)
Substituting the given value of \(n=4\) into this formula, we get:
\(l = 0, 1, 2, ..., (4-1)\)
\(l = 0, 1, 2, 3\)
These are the distinct values that the orbital quantum number can take when the principal quantum number is 4. Each of these 'l' values corresponds to a specific type of subshell:
The relationship between the principal quantum number (n) and the permitted orbital quantum numbers (l) can be summarized in the following table:
| Principal Quantum Number (n) | Permitted Orbital Quantum Numbers (l) | Number of Different 'l' Values | Corresponding Subshell Types |
|---|---|---|---|
| 1 | 0 | 1 | s |
| 2 | 0, 1 | 2 | s, p |
| 3 | 0, 1, 2 | 3 | s, p, d |
| 4 | 0, 1, 2, 3 | 4 | s, p, d, f |
Therefore, for the hydrogen atom, when the principal quantum number is 4, the number of different permitted orbital quantum numbers is the count of the values {0, 1, 2, 3}, which is four.
_______ specifies the preferred orientation in the orbital space of the given energy and size.
After completing the gold foil experiment, Rutherford concluded that the size of the nucleus is very small compared to the size of the atom. This is because:
Which of the following was not observed by Rutherford using the scattering of α-rays?
1. Most of the α-particles get slightly deflected from their path.
2. Fewer α-particles get deflected at greater angles.
Suppose that an alpha particle of 4.50 MeV approaches head-on a uranium nucleus (Z = 92). Assuming that the uranium nucleus remains at rest and the alpha particle momentarily comes to rest and reverses its direction at a distance much more than the radius of the uranium nucleus, the distance of its closest approach is close to: