Electrophoresis Flashcards
What are colloids
The are made of one phase dispersed into another phase (like liquid in liquid or solid in liquid)
We typically use liquid liquid, or solid in liquid (gel)
Explain colloid instability
Colloids in solution are not stable, they flocculate (clump together) then coagulate, then sediment out of solution
Or it can sediment (drop to bottom of container), flocculate, then coagulate
Not good
Whag influence colloid stability
Concentration: if higher, they more likely to interact with each other
Do they like to stick together
What solution it’s in
What are the two types of stabilization for colloids which are barriers to floculations
Steric stabilization (stick polymer chain on it that pushes away other molecule)
Electrostatic stabilization
Explain why flocculation is favourable to happen
Using hard sphere model
Van der walls forces pulls the molecules together at the lowest energy
The model says that if we leave the molecules together, they will start to stick together due to these attractive forces
This is the precursor to flocculation thencoagulation and precipitate
What are the sources of charge on surfaces
Ph change: making a solution basic give a net negative charge on the surface groups
Silica: the silica changes charge depending on the pH of the solution (can go either way) , like running KOH in glass (basic) so net negative silica charge of the surface. Giving acid makes it acidic
Ionization of surface groups: ions like AgI, can solvate one ion and leave the other on the surface
Surfactants: can be cationic or anionic surfactants (like SDS), sick to the surface and carry a charge with it
What is the equation for van der waals attractive force
Repulsive force
-A/12pir^2
On sheet
Explain the van der waal attractive force and repulsive force and the net energy in the one graph
attractive force which makes the line go down in energy as molecules get closer
Repulsive force which makes them go higher in energy as they get closer
Then net energy hump is in between them which shows how there is an energy hill the molecules need to climb so they can eventually attract and flocculate
Explain the flocculation curve
Particles far apart , no energy no interaction
Get close, start to have vander waals attractive forces, energy goes down
Then eventually you have repulsive force as they get too close, higher energy
If we get them close enough (for example higher concentration) Then they can cross over this high energy hump to follculate (crash out) and get closer together and to low energy
Eventually them stick together and turn into a clump that is incompressible
Explain the double layer model
Surface: You have a negative charge particle in solution
Stern layer: Surrounding it is the tight bound positive charged counterions that move with the particle
Diffuse layer: has less tightly bound ions, can be postive or negative because now the particle looks postive, it’s all the ions outward of the stern layer
Inside diffuse layer the is the slipping plane
Slipping plane: the part where ions stop moving with the particle as it moves through the solution
this plane is the boundary between ions that are still moving with the particle and ions that are not and just stay in the solution (some point in the diffuse layer)
Explain the double layer plot
P vs r plot for a positively charged particle
Surface potential: surface layer of the particle (0 r), the potential would be positive because it’s postive ion (
Stern potential: As we move outward from the surface and go to stern layer, the negative counterions start to drop the potential
Diffuse Layer: the potential decreases more due to shielding of the ions in the diffuse layer
Zeta potential: At some point in the diffuse layer we reach the slipping plane, potential measures here is the zeta potential
Then furthest away from the ion is close to zero because looks neutral
Why do we measure the zeta potential at ethe spliiping plane
If try to move particle through the fluid is act as if it has a size due to the ions surrounding it
Measuring the zeta potential at the slipping plane lets us measure the size of the particle because at this point you can see the end point of the ions that contribute to its size
40:04 idk
Why does the double layer plot go to zero at infinity
We’re so far away from the particle that there are a bunch of ions between where we measure and the particle
These in between ions position themselves around the particle based on what the charge on the particle looks like to them
This ultimately makes the potential neutralize and become zero
Do the surface and the zeta potential have the same sign
No the sign of the zeta potential doesn’t tell you what the surface of the particle is
The zeta potential depends on the solution that the particle is in
If more polar, more ions, can change what the zeta potential looks like
There are ions close to the surface of the molecule that aren’t exactly associating with it but their charge affects what the zeta potential is
Just like how PAH and PSS affect what the charge looks like on the molecule
What are the compounds that let you change the charge on the surface
PAH (postive charge)
PSS (negative charge)
If postive surface, add PSS, Makes surface negative
Can keep going with PAH to make it back to postive
What is the purpose of reversing charges using PSS or PAH
If the surface was one third negatively charged and the rest neutral
You can still add PAH to make it look uniformly negative since it big and will cover regions that are neutral
Can turn something that is weakly charged into something that has a highly negative or postive charge
At was potential is a particle /colloid stable
What does this mean
+/- 30mV
This mean if we measure the zeta and that is it’s value, there is enough of an energetic hump that the particles won’t easily flocculate and crash out
What is the effect of the pH on the zeta potential
low ph, zeta potential positive, stable
High pH, zeta potential negative, stable
At the isoelectric point, the zeta potential is zero and no net charge pushing the particles apart, unstable because now not +/- 30 mV
This means there will be flocculation since no charge repelling the ions
Can the isoelectric point of a particle be change and how
What could change shape of the zeta potential vs pH graph to start negative at low ph and get postive at high pH
Can be changed because of diff functional groups of the particle, can cause flocculation at lower ph or higher ph (so lower or higher isoelectric point)
Changing the sign at low ph would mean that having more h ions is causing the particle to be more negative , so not possible and weird
What is the Debye length
What does it mean
At what point does it end
Lambda D = 1/kappa
Describes the length of the diffuse layer and the amount shielding of the particle
How far you have to go before the potential of the particle is shielded by the many counter ions in the diffuse layer and the potential becomes zero
Since the diffuse layer has exponential decay (never goes to zero) we say that the diffuse layer ends at a potential 1/e of its original value
So 1/3 of the diffuse layers original potential value
If the diffuse layer drops has its exponential decay very quickly what does this mean
Very slow decay
Quick: say the diffuse layer is very thin, more ions, faster decrease because easier to drop the potential
Slow: diffuse layer very thick, less ions, , slower decrease because harder to drop the potential
What is the effect of higher ionic strength of the diffuse layer
More ions in the diffuse layer, shielding is going to be very thin because that’s all you need to drop the potential to 1/e
If less ions (for example just water and not na+), the diffuse layer is bigger since you need more of them to shield and drop the potential to 1/e
What is meant by shielding and why does it happen
If the particle is postive, the stern is negative, but ions in the diffuse layer look at that and try to make it more postive
Then the negative ions out look at, see a general postive charge, and configure themselves to make it more negative
This accumulation of opp charged ions makes it so that shielding of the particle happens and the potential looks to be neutral/zero very far away
When do we say something is fully shielded
When the potential reaches 1/e or 1/3 of the original potential value (at the surface)