View
214
Download
0
Embed Size (px)
Citation preview
Page 1
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
BMS 631 - LECTURE 7Flow Cytometry: TheoryJ. Paul RobinsonProfessor of Immunopharmacology& Biomedical EngineeringPurdue University
Hansen Hall, B050Purdue UniversityOffice: 494 0757Fax 494 0517email: [email protected]
WEB http://www.cyto.purdue.edu
Detectors & Fluidics
3rd Ed. Shapiro 127-133
Notes:1. Material is taken from the course text: Howard M.
Shapiro, Practical Flow Cytometry, 3nd edition (1994), Wiley-Liss, New York.
2. RFM =Slides taken from Dr. Robert Murphy3. MLM – Material taken from Melamed, et al, Flow
Cytometry & Sorting, Wiley-Liss, 2nd Ed.
Page 2
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Detectors
• Light must be converted from photons into volts to be measured
• We must select the correct detector system according to how many photons we have available
• In general, we use photodiodes for forward scatter and absorption and PMTs for fluorescence and side scatter
Page 3
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Silicon photodiodes• A silicon photodiode produces current when photons
impinge upon it (example are solar cells)• Does not require an external power source to operate• Peak sensitivity is about 900 nm• At 900 nm the responsivity is about 0.5
amperes/watt, at 500 nm it is 0.28 A/W• Are usually operated in the photovoltaic mode (no
external voltage) (alternative is photoconductive mode with a bias voltage)
• Have no gain so must have external amps• quantum efficiency ()% = 100 x (electrons out/(photons in)
Page 4
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
PMT• Produce current at their anodes when photons impinge upon
their light-sensitive cathodes• Require external powersource• Their gain is as high as 107 electrons out per photon in• Noise can be generated from thermionic emission of electrons
- this is called “dark current”• If very low levels of signal are available, PMTs are often cooled
to reduce heat effects• Spectral response of PMTs is determined by the composition of
the photocathode• Bi-alkali PMTs have peak sensitivity at 400 nm• Multialkali PMTs extend to 750 nm • Gallium Arsenide (GaAs) cathodes operate from 300-850 nm
(very costly and have lower gain)
Page 5
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Signal Detection - PMTs
Cathode Anode
Dynodes
Photons in
AmplifiedSignal Out
EndWindow
• Requires Current on dynodes• Is light sensitive• Sensitive to specific wavelengths• Can be end`(shown) or side window PMTs
Secondary emission
Page 6
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Photomultiplier tubes (PMT’s)
The PMTs in an Elite. 3 PMTs are shown, the other 2 have been removed to show their positions. A diode detector is used for forward scatter and a PMT for side scatter.
The Bio-Rad Bryte cytometer uses PMTs for forward and wide angle light scatter as well as fluorescence
Page 7
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
PMTs• High voltage regulation is critical because the
relationship between the high voltage and the PMT gain is non-linear (almost logarithmic)
• PMTs must be shielded from stray light and magnetic fields
• Room light will destroy a PMT if connected to a power supply
• There are side-window and end-window PMTs• While photodiodes are efficient, they produce
too small a signal to be useful for fluorescence
Page 8
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Diode Vs PMT• Scatter detectors are frequently diode
detectors
Back of Elite forward scatter detector showing the preamp
Front view of Elite forward scatter detector showing the beam-dump and video camera signal collector (laser beam and sample sheath are superimposed)
Sample stream
Page 9
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Types of PMTs
Side Window
High voltage in
Signal out
Page 10
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
High Voltage on PMTs• The voltage on the PMT is applied to the dynodes• This increases the “sensitivity” of the PMT• A low signal will require higher voltages on the
PMT to measure the signal• When the voltage is applied, the PMT is very
sensitive and if exposed to light will be destroyed• Background noise on PMTs is termed “dark
noise”• PMTs generally have a voltage range from 1-
2000 volts• Changing the gain on a PMT should be linear
over the gain range• Changing the voltage on the PMT is NOT a linear
function of response
Page 11
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Avalanche Photodiodes (APD’s)
• Combines the best features of PMTs and photodiodes• High quantum efficiency, good gain• Gain is 102-103 (much less than PMTs)• Problem with high dark current
Image From: http://micro.magnet.fsu.edu/primer/java/photomicrography/avalanche/
Page 12
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
CCDs
• Charge Coupled devices (CCD) usually in our video cameras (also called charged transfer devices)
• light causes accumulation of electric charge in individual elements which release the charge at regular intervals
• Useful in imaging because they can integrate over time
• Not fast enough for flow cytometry application in general
Page 13
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Summary so far….• Photodiodes can operate in two modes - photovoltaic
and photoconductive• PMTs are usually used for fluorescence measurements• Photodiodes are usually used for scatter• PMTS are sensitive to different wavelengths according
to the construction of the photocathode• PMTs are subject to dark current• Voltages and gain are not linear• Photodiodes are more sensitive than PMTs but because
of their low gain, they are not as useful for low level signals (too much noise)
Page 14
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Flow Systems and Hydrodynamics
Getting the cells in the right place (at the right time)! (Shapiro, pp 133-143 - 3rd ed)
Page 15
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Basics of Flow Cytometry
•cells in suspension
•flow in single-file through
•an illuminated volume where they
•scatter light and emit fluorescence
•that is collected, filtered and
•converted to digital values
•that are stored on a computer
Fluidics
Optics
Electronics
[RFM]
Page 16
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Flow Cytometry:
The use of focused light (lasers) to interrogate cells delivered by a
hydrodynamically focused fluidics system.
Flow CellFlow Cell
FluorescenceFluorescencesignalssignals
Focused laserFocused laserbeambeam
Sheath fluid
Fluidics - Differential Pressure System
From C. Göttlinger, B. Mechtold, and A. Radbruch[RFM]
Page 18
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics SystemsPositive Pressure Systems
• Based upon differential pressure between sample and sheath fluid. • Require balanced positive pressure via either air or nitrogen• Flow rate varies between 6-10 ms-1
+ + ++ + ++ + +
Positive Displacement Syringe Systems
• 1-2 ms-1 flow rate• Fixed volume (50 l or 100 l)• Absolute number calculations possible• Usually fully enclosed flow cells
100 l
Sample loop
Sample Waste
Flowcell3-way valve
Syringe
Page 20
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamics and Fluid Systems
• Cells are always in suspension • The usual fluid for cells is saline• The sheath fluid can be saline or
water• The sheath must be saline for sorting• Samples are driven either by
syringes or by pressure systems
Page 21
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics
• Need to have cells in suspension flow in single file through an illuminated volume
• In most instruments, accomplished by injecting sample into a sheath fluid as it passes through a small (50-300 µm) orifice
[RFM]
Page 22
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics
• When conditions are right, sample fluid flows in a central core that does not mix with the sheath fluid
• This is termed Laminar flow
[RFM]
Page 23
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
• Whether flow will be laminar can be determined from the Reynolds number
• When Re < 2300, flow is always laminar
• When Re > 2300, flow can be turbulent
Fluidics - Laminar Flow
Re d v
whered tube diameter
density of fluidv mean velocity of fluid
viscosity of fluid
[RFM]
Page 24
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics
• The introduction of a large volume into a small volume in such a way that it becomes “focused” along an axis is called Hydrodynamic Focusing
[RFM]
FluidicsThe figure shows the mapping between the flow lines outside and inside of a narrow tube as fluid undergoes laminar flow (from left to right). The fluid passing through cross section A outside the tube is focused to cross section a inside.
From V. Kachel, H. Fellner-Feldegg & E. Menke - MLM Chapt. 3[RFM]
V. Kachel, H. Fellner-Feldegg & E. Menke - MLM Chapt. 3
Notice how the ink is focused into a tight stream as it is drawn into the tube under laminar flow conditions.
Notice also how the position of the inner ink stream is influenced by the position of the ink source.
[RFM]
Fluidics
Page 27
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics
• How do we accomplish sample injection and regulate sample flow rate?– Differential pressure– Volumetric injection
[RFM]
Page 28
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Differential Pressure System
• Use air (or other gas) to pressurize sample and sheath containers
• Use pressure regulators to control pressure on each container separately
[RFM]
Page 29
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Differential Pressure System
• Sheath pressure will set the sheath volume flow rate (assuming sample flow is negligible)
• Difference in pressure between sample and sheath will control sample volume flow rate
• Control is not absolute - changes in friction cause changes in sample volume flow rate
[RFM]
Page 30
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Volumetric Injection System
• Use air (or other gas) pressure to set sheath volume flow rate
• Use syringe pump (motor connected to piston of syringe) to inject sample
• Sample volume flow rate can be changed by changing speed of motor
• Control is absolute (under normal conditions)
[RFM]
Page 31
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Syringe systems
• Bryte HS Cytometer
3 way valve
Syringe
Fluidics - Volumetric Injection System
H.B. Steen - MLM Chapt. 2
Page 33© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamic Systems
MicroscopeMicroscopeObjectiveObjective
WasteWasteFlowFlowCellCell CoverslipCoverslip
SignalsSignals
MicroscopeObjective
Waste
FlowCell Coverslip
SignalsSignals
Page 34
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Particle Orientation and Deformation
• As cells (or other particles) are hydrodynamically focused, they experience different shear stresses on different points on their surfaces (an in different locations in the stream)
• These cause cells to orient with their long axis (if any) along the axis of flow
[RFM]
Page 35
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Particle Orientation and
Deformation• The shear stresses can also cause
cells to deform (e.g., become more cigar-shaped)
[RFM]
Fluidics - Particle Orientation and Deformation
“a: Native human erythrocytes near the margin of the core stream of a short tube (orifice). The cells are uniformly oriented and elongated by the hydrodynamic forces of the inlet flow.
b: In the turbulent flow near the tube wall, the cells are deformed and disoriented in a very individual way. v>3 m/s.”
Image fromV. Kachel, et al. – Melamed Chapt. 3[RFM]
Page 37
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Flow Chambers
• The flow chamber– defines the axis and dimensions of
sheath and sample flow– defines the point of optimal
hydrodynamic focusing– can also serve as the interrogation
point (the illumination volume)
[RFM]
Page 38
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Closed flow cells
Laser direction
Page 39
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Coulter XL
Sample tubeSheath and waste system
Page 40
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluidics - Flow Chambers
• Four basic flow chamber types– Jet-in-air
• best for sorting, inferior optical properties
– Flow-through cuvette• excellent optical properties, can be used for
sorting
– Closed cross flow• best optical properties, can’t sort
– Open flow across surface• best optical properties, can’t sort
[RFM]
Fluidics - Flow Chambers
H.B. Steen - MLM Chapt. 2
Flow through cuvette (sense in quartz)
[RFM]
Fluidics - Flow Chambers
H.B. Steen - MLM Chapt. 2
Closed cross flow chamber
[RFM]
Page 43© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamic Systems
Sample inSheath
Sheath in
Laser beam
Piezoelectriccrystal oscillator
FluorescenceSensors
Scatter Sensor
Core
Sheath
Page 44
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamically focused fluidics
Page 45
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamically focused fluidics
•Increase Pressure:•Widen Core•Increase turbulence
Signal
Page 46© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Hydrodynamic Systems
Flow Cell
Injector Tip
Fluorescencesignals
Focused laserFocused laserbeambeam
Sheath fluid
Page 47
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
What happens when the channel is blocked?
Page 48
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Flow chamber blockage
A human hair blocks the flow cell channel. Complete disruption of the flow results.
Page 49
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Bryte Fluidic Systems Detectors
• Sample Collection and hydrodynamics
Bryteb.mpg
Page 50
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fluorescence Detectors and Optical TrainBrytec.mpg
Shown above is the Bryte HS optical train - demonstrating how the microscope-like optics using an arc lamp operates as a flow detection system. First are the scatter detectors (left side) followed by the central area where the excitation dichroic can be removed and replaced as necessary. Behind the dichroic block is the arc lamp. To the right will be the fluorescence detectors.
Page 51
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Flow CellFlow Cell
Injector Tip
FluorescenceFluorescencesignalssignals
Focused laserFocused laserbeambeam
Sheath fluid
Page 52
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Sheath and waste systemsEpics Elite
Sheath Filter UnitLow PressureSheath and Waste bottles
Page 53
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Fromlaser
Fluorescence collection lens, optical filters, dichroic filter, band pass filter
Beam shaping lens
reflector
J.Paul RobinsonProfessor of ImmunopharmacologySchool of Veterinary Medicine, Purdue University
Page 54
© 1990-2002 J.Paul Robinson, Purdue University BMS 631 – LECTURE007.PPT
Lecture Summary
• Detection systems in flow cytometry• Critical aspects of flow systems• Flow must be laminar (appropriate Reynolds #)
– When Re < 2300, flow is always laminar• Samples can be injected or flow via differential
pressure• There are many types of flow cells• Blockages must be properly cleared to obtain high
precision
WEB http://www.cyto.purdue.edu