This lecture focuses on how proteins bind ligands, how to interpret the dissociation constant (KD), and why ligands eventually dissociate even when binding occurs.
One of the key questions in protein biophysics is:
When is a proteināligand interaction considered strong or weak?
The answer depends on the dissociation constant (KD).
KD describes the affinity between a protein and a ligand.
K_D = rac{k_}{k_}
Where:
Interpretation:
| KD Range | Binding Strength |
|---|---|
| mM (10ā»Ā³ M) | Weak binding |
| µM (10ā»ā¶ M) | Moderate binding |
| sub-µM (<10ā»ā¶ M) | Strong binding |
| nM or sub-nM | Very strong binding |
Important note:
ā ļø These boundaries are not strict rules. They are approximate classifications used in biochemistry.
In the lecture example, a millimolar KD was measured for an alginate oligomer binding to a protein, which indicates weak binding.
Even when binding occurs, ligands may leave the protein quickly.
Example given in the lecture:
If:
k_ = 10^7 ; M^{-1}s^{-1}
and
K_D = 1 mu M
Then:
k_ = 10 s^{-1}
Meaning:
rac{1}{k_} = 0.1 s
So the ligand stays bound only about 100 milliseconds.
Even though binding occurs, the ligand dissociates frequently, meaning the interaction is not very stable.
A truly strong interaction would keep the ligand bound for much longer times.
Binding strength can also be expressed as binding free energy (ĪG).
Typical value discussed:
Delta G approx -35 ; kJ/mol
This corresponds roughly to micromolar binding affinity.
Even though ā35 kJ/mol sounds like a lot, it still only stabilizes the interaction for fractions of a second.
To maintain very stable complexes, the binding energy must be much stronger.
A key conceptual point in the lecture:
Binding interactions are dynamic, not static.
Proteins and ligands are constantly moving due to thermal motion.
In solution:
Because of this motion:
Eventually, enough interactions break simultaneously, allowing the ligand to escape.
This is a statistical process driven by thermal energy.
Proteināligand binding typically relies on non-covalent interactions, including:
Attraction between opposite charges.
Example:
Directional interactions between:
Weak contacts caused by temporary dipoles between atoms.
Because these interactions are individually weak, the ligand can escape when:
The lecture showed a simulation of an alginate trimer binding to a protein module.
Key observations:
Timescale:
ā±ļø Dissociation events occur within microseconds.
If the measured KD is millimolar, dissociation can happen extremely frequently.
Example:
10^4 ext{ dissociation events per second}
Meaning:
Unlike association, dissociation does NOT depend on concentration.
Reason:
Dissociation is governed purely by internal molecular energy fluctuations.
Lower KD = stronger binding.
Weak binding leads to rapid dissociation.
Interactions constantly break and reform.
Thermal motion eventually breaks enough interactions for the ligand to escape.
Examples include:
ā Core idea of the lecture:
Proteināligand binding is not a rigid lock-and-key system. It is a dynamic equilibrium where molecules constantly bind and unbind due to thermal motion.