The Octahedral Setup
Imagine you are looking at the heart of the [Ti(H2O)6]3+ complex. Titanium, with an atomic number of 22, normally has the electronic configuration [Ar]3d24s2. However, in this complex, it exists in a +3 oxidation state. Losing three electrons leaves it with just a single electron in its 3d subshell, making it a d1 system.
When the six water molecules approach the central titanium ion to form an octahedral complex, their electron clouds repel the d-orbitals of titanium. Because of the spatial orientation of these orbitals, they don't all experience the same repulsion. The five degenerate d-orbitals split into two distinct energy levels: a lower energy set of three orbitals called t2g, and a higher energy set of two orbitals called eg. Our lone electron naturally occupies the lowest available energy state, settling comfortably into one of the t2g orbitals.
The Quantum Leap
Now, what happens when light shines on this complex? If a photon of light possesses exactly the right amount of energy, the electron in the t2g level can absorb it and make a quantum leap to the higher eg level. This phenomenon is known as a d−d transition, and it is the primary reason why many transition metal complexes exhibit beautiful, vibrant colors!
The energy required for this transition is exactly equal to the energy gap between the t2g and eg levels. We call this gap the octahedral crystal field splitting energy, denoted by Δo.
According to Planck's quantum theory, the energy of a photon is directly proportional to its frequency, or inversely proportional to its wavelength. The master equation connecting these concepts is:
Here, h is Planck's constant, c is the speed of light, and λ is the wavelength of the absorbed light.
Crunching the Numbers
The problem provides us with all the necessary pieces of the puzzle. We are given the wavelength of the absorbed light, λ=498 nm. Before we plug this into our equation, we must ensure all our units are consistent. We convert nanometers to meters by multiplying by 10−9, giving us λ=498×10−9 m.
We also have the standard constants:
h=6.626×10−34 Js
c=3×108 ms−1
Substituting these values into our master equation, we get:
Δo=498×10−96.626×10−34×3×108
Let's break down the calculation to avoid any silly mistakes. First, we multiply the numerical coefficients in the numerator:
Next, we handle the powers of 10 in the numerator:
So, our expression simplifies to:
Δo=498×10−919.878×10−26
Now, we divide the numbers and subtract the exponent in the denominator from the exponent in the numerator:
Δo=(49819.878)×10−26−(−9)
To express this in standard scientific notation, we shift the decimal point two places to the right, which decreases the exponent by 2:
The Final Verdict
We have successfully calculated the octahedral splitting energy! The question asks us to find the value that fills in the blank for ⋯×10−19 J, and to round it off to the nearest integer.
Looking at our result, 3.9915 is incredibly close to 4. Therefore, rounding off to the nearest integer gives us our final answer:
Final Answer = 4
This problem beautifully illustrates how macroscopic properties like the color of a solution are intimately connected to the microscopic quantum world of electron transitions and orbital splitting!