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Portable Optical Tweezers Kit
Chapter 7: Experiments
Page 72
MTN012639-D02
Here,
𝜂
𝑒𝑓𝑓
denotes the effective viscosity,
𝑅
is the radius of the PS-bead,
𝑇
is the
temperature of the sample in Kelvin (corresponds to room temperature), and
𝑘
𝐵
is the
Boltzmann constant, which is a natural constant and has a value of
1.38 ⋅ 10
−23 𝐽
𝐾
.
Exercise
Determine the effective viscosity
𝜂
𝑒𝑓𝑓
of the sample with the 3 µm polystyrene spheres, by
solving the equation (33) according to viscosity and using the gradient
𝑚
of the measured
curve from the previous exercise.
Solution
The equation for the calculation of the effective viscosity
𝜂
𝑒𝑓𝑓
is:
𝜂
𝑒𝑓𝑓
=
2𝑘
𝐵
𝑇
3𝜋𝑅𝑚
(34)
Here,
T
is the room temperature,
k
B
the Boltzmann constant,
a
the radius, and
m
the
previously determined gradient of the PS-beads used.
The determined effective viscosity should be in the range of a few
10
−3 𝑁𝑠
𝑚
2
Exercise
After which speed can the PS-bead no longer be held? Determine the maximum holding
force of the optical tweezers.
Solution
If the PS-bead is in the optical trap, two forces act on it. First of all, the frictional force
𝐹
𝑅
,
which is caused by the suspension in which the PS-bead is located, and thus works against
the other force, the holding force
𝐹
𝐻
of the optical trap. The following equation describes
the frictional force
𝐹
𝑅
:
𝐹
𝑅
= 6𝜋𝜂
𝑒𝑓𝑓
𝑅𝑣
(35)
Here,
𝜂
𝑒𝑓𝑓
is the effective viscosity of the suspension,
𝑅
is the radius of the bead, and
𝑣
is
the speed. The maximum holding force is said to have been reached precisely, when the
PS-bead at a certain speed
𝑣
𝑚𝑎𝑥
can just be held. This is the case when both forces are
in balance:
𝐹
𝑆𝑡𝑜𝑘𝑒𝑠
= 𝐹
𝐻,𝑚𝑎𝑥
= 6𝜋𝜂
𝑒𝑓𝑓
𝑅𝑣
𝑚𝑎𝑥
(36)
The holding force is in the range of a few pN.
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