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Quinacrine As a Fluorescent Label to Study Real-Time Exocytosis of Single Platelet Dense Granules J.M.H. Goudsmits July 2011 MBx 2011-xx Master’s Thesis Research Group Molecular Biosensors for Medical Diagnostics (MBx) Eindhoven University of Technology Department of Applied Physics Supervisors H.M. van Zijp A.M. de Jong

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Page 1: Quinacrine As a Fluorescent Label to Study Real-Time ...alexandria.tue.nl/extra1/afstversl/n/Goudsmits_2011.pdf · The arrowhead indicates a dense granule with a clear halo region

Quinacrine As a Fluorescent Label

to Study Real-Time Exocytosis of

Single Platelet Dense Granules

J.M.H. GoudsmitsJuly 2011

MBx 2011-xx

Master’s Thesis

Research Group

Molecular Biosensors for Medical Diagnostics (MBx)

Eindhoven University of Technology

Department of Applied Physics

Supervisors

H.M. van Zijp

A.M. de Jong

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Abstract

Platelets play a critical role in haemostasis. Their activation and aggregation

is facilitated by exocytosis of proteins and other small messenger molecules from

granules. The release dynamics of this process are rather unknown. In this study,

quinacrine, a fluorescent label for platelet dense granules, is explored as a tool to

measure real-time exocytosis of ATP stored in single dense granules.

A luciferase assay was used to assess quinacrine influence on platelet activa-

tion in bulk. No significant effect of quinacrine on platelet functioning was found.

The same assay was also used to investigate substrate-induced activation. These

studies revealed that BSA coated glass is the most suitable surface for platelet

immobilisation, which is needed for microscopy experiments. Real-time fluores-

cence microscopy studies on single platelets showed that quinacrine photoinduces

granule lysis, before exocytotic events can take place. Suggestions for an analyti-

cal approach to distinguish lysis from exocytosis are made, as well as proposals to

continue research on visualisation of single platelet activation.

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Contents

1 Introduction 3

1.1 Platelets . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3

1.1.1 Role in Haemostasis . . . . . . . . . . . . . . . . . . . . 3

1.1.2 Structure . . . . . . . . . . . . . . . . . . . . . . . . . . 3

1.1.3 Activation: Exocytosis and Shape Change . . . . . . . . . 4

1.2 Platelet Function Testing . . . . . . . . . . . . . . . . . . . . . . 6

1.2.1 Bulk Measurements . . . . . . . . . . . . . . . . . . . . . 6

1.2.2 Single Cell Measurements . . . . . . . . . . . . . . . . . 7

1.2.3 New Approach . . . . . . . . . . . . . . . . . . . . . . . 7

1.3 Thesis Overview . . . . . . . . . . . . . . . . . . . . . . . . . . . 8

2 Methods 9

2.1 Luciferase Assay for Bulk Activation . . . . . . . . . . . . . . . . 9

2.2 Substrate-Induced Activation Assay . . . . . . . . . . . . . . . . 9

2.3 Single Platelet Activation Assay: Visualising Dense Granule Exo-

cytosis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10

2.4 Materials and Setup . . . . . . . . . . . . . . . . . . . . . . . . . 12

2.4.1 Preparation of Washed Human Platelets . . . . . . . . . . 12

2.4.2 Measuring ATP with Luciferase . . . . . . . . . . . . . . 13

2.4.3 Substrate-Induced Activation . . . . . . . . . . . . . . . . 13

2.4.4 Imaging Labelled Granules . . . . . . . . . . . . . . . . . 14

2.4.5 Data Analysis . . . . . . . . . . . . . . . . . . . . . . . . 14

3 Results 17

3.1 Bulk Activation . . . . . . . . . . . . . . . . . . . . . . . . . . . 17

3.1.1 Quinacrine Does Not Influence TRAP-induced Platelet Ac-

tivation Significantly . . . . . . . . . . . . . . . . . . . . 17

3.1.2 Platelet Responsiveness Changes over Time . . . . . . . . 18

3.2 Substrate-Induced Activation . . . . . . . . . . . . . . . . . . . . 19

3.2.1 BSA Coated Surface Shows Least Induced Activation . . 19

3.2.2 Platelets Can Still Be Activated with TRAP After Incuba-

tion on Substrate . . . . . . . . . . . . . . . . . . . . . . 21

3.3 Fluorescent Imaging of Single Platelet Activation . . . . . . . . . 22

3.3.1 Types of Release Events . . . . . . . . . . . . . . . . . . 22

3.3.2 Granule Lysis Is Induced by Excitation Light . . . . . . . . 23

3.3.3 Discriminating Granule Lysis from Exocytosis . . . . . . . 24

1

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CONTENTS CONTENTS

4 Discussion & Conclusion 29

5 Acknowledgements 33

A Using Luciferase for a Single Platelet Assay 35

B Granule-OCS Exocytosis: Calculations and Simulations 37

B.1 Diffusion of Gaussian Profile in Free Space . . . . . . . . . . . . 37

B.2 Granular Content Diffusing Through Channel . . . . . . . . . . . 37

B.3 Granular Content Diffusing Through OCS . . . . . . . . . . . . . 39

Glossary 41

2

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Chapter 1

Introduction

Platelets, or thrombocytes, play an important role in haemostasis, the process

that stops bleedings caused by injured blood vessels. Blood loss should be stopped

quickly. Blood flow in intact vessels however should not be obstructed by unwanted

clot formation. The correct functioning of platelets is thus of vital importance.

1.1 Platelets

1.1.1 Role in Haemostasis

Haemostasis is a complex process that involves interactions between platelets,

blood vessels, numerous blood plasma proteins and several small molecules [1].

This process has a few steps. First, immediately following damage, vessels con-

strict, therefore lowering the blood flow. Second, platelets adhere to collagen that

is exposed at the damaged site. By adhesion, platelets are activated and release

proteins and other molecules that activate nearby platelets. As a result, platelets

interact and form a loose plug; this is called primary haemostasis. At the same

time, secondary haemostasis occurs: fibrin proteins are made that reinforce the

platelet plug by forming a fibre mesh. Finally, the vessel is repaired and the blood

clot is slowly dissolved by enzymes.

1.1.2 Structure

Human platelets, when in an unactivated resting state, are discoid-shaped cells

lacking a nucleus. The cells are 2 to 5 µm in diameter, 0.5 µm thick and have

a volume of 6 to 10 fl [2]. In healthy subjects, 150,000 to 300,000 platelets/µl

are present. Precursor cells called megakaryocytes form platelets and release them

into the bloodstream by fragmentation. Platelets contain organelles found in most

eukaryotes: endoplasmic reticulum, Golgi apparatus, mitochondria, glycosomes

and lysosomes. Two important types of secretory organelles that play a key role

in the function of platelets are present: alpha granules and dense granules (delta

granules).

Alpha granules are the most numerous of platelet organelles. Depending on

the platelet size, there are 40 to 80 granules. The round shaped organelles are 200

3

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1.1. Platelets

to 500 nm in diameter and contain many coagulation proteins. Dense granules

are smaller (100 nm diameter), fewer in number (4 to 8 per platelet), and are

irregular in form (Figure 1.1a). They contain small molecules: serotonin (65

mM), adenosine diphosphate (ADP, 653 mM), adenosine triphosphate (ATP, 436

mM) – both adenine nucleotide are non-metabolic, i.e. they are not involved in

energy pathways –, calcium-ions (2.2 M) and pyrophosphate (326 mM) [3]. As

observed from scanning electron microscope (SEM) images, in dense granules

there exist a so called halo region between the dense core and granular membrane

(Figure 1.1a). There is evidence that the halo contains serotonin taken up from

cytoplasm [4], and that the core consists of high molecular weight aggregates of

ATP and other molecules [5, 6].

(a) Dense granules (b) OCS

Figure 1.1: Scanning electron microscope (SEM) image of resting platelet. From [2]. (a)

Dense granules (visible as electron dense (black) regions) are irregular in form, 22,000x.

The arrowhead indicates a dense granule with a clear halo region. (b) Discoid platelet with

stained OCS and membrane surface, 22,000x. Arrowheads indicate surface invaginations.

1.1.3 Activation: Exocytosis and Shape Change

Upon activation, platelets degranulate. That is, they release the contents of both

types of granules into the extracellular space, normally the bloodstream, through

exocytosis. Exocytosis is a process that transports contents of vesicles out of the

cell membrane by fusion of the cell and vesicle membranes (lipid bilayers) (Figure

1.2). This process involves a few steps. First, the vesicle is transported towards

the cell membrane by motor proteins. Next, mediated by so-called SNARE proteins

[7], the vesicle docks to the cell membrane and both membranes fuse. A small

fusion pore is created through which diffusion of vesicle contents already starts.

Finally, the vesicle membrane is completely incorporated into the cell membrane

and its contents are completely released. Any proteins that were present in the

vesicle membrane itself are now incorporated in the cell membrane.

In human1 platelets, the products stored in granules are not discharged into

the extracellular space directly, but into the open canalicular system (OCS). The

1Not all platelets have an OCS, such as bovine and equine platelets.

4

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1.1. Platelets

Cell interior

Cell exterior

Cell membrane

Vesicle

Figure 1.2: Illustration of exocytosis (simplified). A vesicle approaches the cell membrane

(left image). Both membranes (vesicle and cell) are lipid bilayers. So-called SNARE proteins

(not displayed) mediate the docking of the vesicle to the membrane and the membrane

fusion (middle images). Finally, the vesicle membrane is completely incorporated into the

cell membrane and its contents are released (right image).

OCS is a tortuous network of membrane invaginations tunnelling through the

cytoplasm (Figure 1.1b). This tubular system increases the total surface area

exposed to plasma, providing a way for substances to quickly reach the innermost

of the cell. Alpha en dense granules fuse with the OCS membrane, which is cell

surface membrane. The OCS membrane also supplies the additional membrane

that is needed for spreading (see next paragraph).

Besides organelles described earlier, cell structures exist that shape the platelet.

Microtubules, situated as a circumferential coil, form the cytoskeletal support.

Microfilaments, or actomyosin filaments (contractile proteins also found in muscle

cells), are responsible for internal transformations and overall shape change upon

activation: platelets form pseudopods and spread, increasing surface area and

thus bind more strongly. The central body of the cell, incorporating most of the

organelles, remains visible as a bulge (Figure 1.3).

(a) Resting platelet (b) Activated platelet

Figure 1.3: SEM image of resting and activated platelet. From [2]. (a) Discoid-shaped

resting platelet, 30,000x. (b) Early spread platelet with pseudopods and central body visible,

11,000x.

Platelet activation is a complex process involving many intracellular pathways.

As mentioned earlier, platelets can be activated by collagen in damaged vessel

walls. Other platelet activators (agonists) are: ADP, ATP (both present in dense

5

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1.2. Platelet Function Testing

granules), epinephrine, thrombin (protein that cleaves fibrinogen into insoluble fib-

rin that leads to the formation of clots) and thrombin receptor activating peptide

(TRAP, synthetic peptide with strong activation response). Shear stress and low

temperatures can also trigger activation [8]. Both activation processes, degran-

ulation through exocytosis and shape change, are two separate processes that

describe the activation status. In other words, a shape change does not necessar-

ily mean that degranulation also takes place. Small structural deformations are

reversible [2], degranulation however marks irreversible platelet activation.

1.2 Platelet Function Testing

The clinical importance of diagnostic tests for abnormal platelet functioning is

evident. Moreover, research from the last years indicate that platelets are also

involved in inflammatory functions [9] and are critically involved in the onset of

atherosclerosis [10], therefore making platelet function analysis important in pre-

ventive healthcare.

Apart from clinical studies, research is needed to understand fundamental prop-

erties of platelet activation and granule release dynamics. In the following sections,

existing techniques for platelet function testing are summarised [11, 12].

1.2.1 Bulk Measurements

In general, the (bulk) responsiveness of platelets can be quantified by their steady

state activation as a function of agonist, presented in a dose-response curve (Fig-

ure 1.4). Deviations in reactivity, such as high-responsive platelets indicating

thrombotic risks or low-responsive platelets indicating bleeding disorders, result

in a curve change. Another method to describe responsiveness is to study the

temporal behaviour after stimulation.

b l ee d

i n g

n or m

a l

platel

et ac

tivatio

n

l o g [ a g o n i s t ]

t h ro m

b ot i c

Figure 1.4: Sketch of dose-response curves displaying platelet responsiveness for healthy

subjects and subjects with thrombotic and bleeding disorders.

The oldest in vivo technique to assess platelet functionality is bleeding time,

in which a cut with standardised width and depth is made. The time it takes for

the bleeding to stop is a quantitative measure for platelet functioning.

6

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1.2. Platelet Function Testing

Aggregometry is the most widely used platelet function test. Upon in vitro

stimulation of a blood sample with agonist, platelets start to aggregate and the

sample’s light transmission is increased. The light that is scattered, i.e. not

transmitted, as a function of agonist is a measure for platelet aggregation.

Another way to quantify activation is by measuring granule secretion. The

most used analytical assay to determine the dynamic (bulk) release of ATP from

dense granules is a luciferase bioluminescence assay [13, 14]. Another recent

study presents an electrochemical assay to measure real-time serotonin release

from platelets [15].

1.2.2 Single Cell Measurements

Whilst bulk techniques have benefits like speed and simplicity, they also manifest

shortcoming. Some rare events might be obscured and it is difficult to obtain

statistical distributions. Therefore, single cell measurements provide better under-

standing of fundamental properties.

Flow cytometry is an analytical technique to examine single cell functions, such

as platelet function. Before analysis, platelets are labelled with fluorescent anti-

bodies that bind specific membrane glycoproteins (GPs). For example, GP1b is

a platelet specific membrane marker and P-selectin2 (CD62P) is a protein that

is present on the surface of activated endothelial cells3 and activated platelets.

By measuring fluorescence and scattered light characteristics of single platelets

passing a laser beam, their level of activation can be quantified. Although flow cy-

tometry yields statistical distributions from a very low whole blood sample volume,

measurements require sample preparation, are slow and no dynamic information

can be obtained.

Other bioanalytical tools exist to study single platelet exocytosis [16]. One is an

electrochemical measurement of real-time serotonin (from dense granules) release

from activated platelets by placing a microelectrode above a single platelet. With

this method, quantitative serotonin detection on a sub-millisecond resolution can

be achieved [4, 17]. This technique lacks the ability to obtain spatial information

and to multiplex, i.e. address multiple platelets at once, though.

1.2.3 New Approach

In this research project, a new technique to visualise real-time single platelet ac-

tivation was examined. By fluorescent labelling of dense granule contents with

quinacrine, exocytosis is associated with loss of fluorescent intensity. As a re-

sult, spatial as well as temporal information can be obtained in parallel for tens of

platelets by fluorescent imaging. This multiplexed and spatiotemporal approach

gives new insights in the release dynamics of single platelets. The advantage of

using a fluorescent label is, that it can be combined with other techniques to mea-

sure or locally stimulate single platelets. For example, magnetic particles can be

attached to platelets [18]. An external magnetic field can then be used to apply

forces to the particles, activating the platelets.

2P-selectin is present on the alpha granule membrane. Upon degranulation, the protein is

expressed on the outer platelet surface.3Endothelial cells form a thin layer of cells lining the interior surface of blood vessels.

7

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1.3. Thesis Overview

1.3 Thesis Overview

Fluorescent imaging of dense granules labelled with quinacrine is investigated.

First, bulk measurements were performed to assess the effect of quinacrine on

platelet activation by means of a dose-response curve. Next, substrate induced

activation of immobilised (needed for microscopy experiments) platelets was stud-

ied. With this method, the most suitable substrate for imaging platelet activation

was determined. Then, surface immobilised platelets with stained granules were

imaged to visualise real-time degranulation. The effect of light and fluorescent

dye was studied.

8

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Chapter 2

Methods

Traditionally, bulk techniques like bleeding time and aggregometry are used to

evaluate platelet responsiveness. Another technique utilises a luciferase assay,

which measures ATP concentrations, to quantify platelet degranulation in bulk.

The latter method was first used to prove validity of the single cell measurements

using quinacrine. Finally, quinacrine was explored as a tool to visualise real-time

exocytosis of fluorescently labelled dense granules.

In this chapter, first the global principles of the assays are discussed together

with important characteristics of used substances. Next, the technical details of

the procedures are treated.

2.1 Luciferase Assay for Bulk Activation

Platelet reactivity was quantified by measuring the ATP release from dense gran-

ules with firefly luciferase. Firefly luciferase in combination with D-luciferin is

commonly used as a bioluminescence assay to measure ATP [19, 20]. The assay

has high sensitivity, broad range (pM to mM) and high specificity. D-luciferin is

oxidised while consuming ATP and producing light. The reaction, yielding one

photon per ATP molecule, is catalysed by luciferase, a 63 kDa protein:

ATP + D-luciferin ↽−−−−−−−−Luciferase, Mg2+

−−−−−−−−−−⇀ adenyl-luciferin + PPi,

adenyl-luciferin + O2 −−→ oxyluciferin + AMP + CO2 + light (560 nm).

ATP released from an activated platelet suspension was measured for a range of

TRAP concentrations (sub-µM to mM), i.e. a dose-response curve was measured.

This curve was determined for both untreated platelets and platelets incubated

with quinacrine to assess quinacrine influence on platelet activation.

2.2 Substrate-Induced Activation Assay

In order to determine a suitable substrate for fluorescent imaging of the platelets,

platelet activation induced by differently coated glass coverslips was measured. For

this purpose, glass coverslips were coated with the desired substance first. The

9

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2.3. Single Platelet Activation Assay: Visualising Dense Granule Exocytosis

substances tested were anti glycoprotein 1b (aGP1b, antibody that binds to GP1b,

a platelet surface membrane glycoprotein), mouse immunoglobulin G (IgG, general

antibody), poly-L-lysine (PLL, commonly used for cell adhesion) and bovine serum

albumin (BSA, blocking agent). After that, platelet suspension was added onto

the coated glass and incubated for 60 minutes: platelets sediment and interact

with the surface. Upon a strong enough stimulus, platelets activate and release

ATP (Figure 2.1). Next, supernatant was transferred into a well and the ATP

concentration was subsequently analysed with the luciferase assay.

60 min

Figure 2.1: Substrate-induced activation assay. A glass coverslip is coated with the de-

sired substance. After incubating platelets for 60 minutes, supernatant is transferred and

analysed with the luciferase assay.

2.3 Single Platelet Activation Assay: Visualising Dense

Granule Exocytosis

Single platelet activation was quantified by measuring real-time exocytosis of dense

granules. Exocytosis was visualised by labelling the granules with quinacrine.

Quinacrine (aka Mepacrine, Atabrine), an old antimalarial drug, is a fluorescent

label that binds adenine nucleotides like ATP [21]. Dense granules contain 436

mM ATP [3], which is high compared to other organelles. As a result, only dense

granules are stained with quinacrine [22]. Dense granule staining was used before

in flow cytometry measurements [23], as bulk fluorescence assay [24], or it was

used to obtain the number of dense granules by counting flashes on prolonged

irradiation [25, 26]. As already shown in mast cells [27], pancreatic B-cells [28]

and astrocytes [29], the release of secretory granule contents is associated with

the decrease or loss of quinacrine fluorescence. Accordingly, platelet degranulation

can be visualised real-time by observing changes in quinacrine fluorescence.

Quinacrine Characteristics

Quinacrine fluorescence excitation (absorbance) ranges roughly from 350 to 475

nm, emission ranges from 440 to 600 nm (Figure 2.2a) [30]. The dye is a base

with different absorption spectra for multiply1 charged cations (Figure 2.2b) [31].

Around the physiological pH of 7, there is an equilibrium mainly between singly

and doubly charged cations. For lower pH, the equilibrium shifts towards the

doubly charged cation, conversely for higher pH the equilibrium shifts towards the

singly charged cation and neutral molecule. Giving the fact that quinacrine is

1The degree of protonation depends on pH.

10

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2.3. Single Platelet Activation Assay: Visualising Dense Granule Exocytosis

excited between 450 and 490 nm (cf. Section 2.4.4), the absorption (and hence

fluorescence) is stronger at lower pH.

3 5 0 4 0 0 4 5 0 5 0 0 5 5 0 6 0 0

norm

alised

excita

tion /

emiss

ion

w a v e l e n g t h ( n m )

e x c i t a t i o n e m i s s i o n

(a) Excitation / emission

3 2 0 3 4 0 3 6 0 3 8 0 4 0 0 4 2 0 4 4 0 4 6 0 4 8 0 5 0 0 5 2 00 . 0 0

0 . 0 5

0 . 1 0

0 . 1 5

0 . 2 0

0 . 2 5

0 . 3 0

0 . 3 5

0 . 4 0

M & N

abso

rbanc

ew a v e l e n g t h ( n m )

D

(b) Protonation dependent absorbance

Figure 2.2: Quinacrine fluorescence characteristics. (a) As measured at pH 5.5, fluores-

cence excitation ranges from 350 to 475 nm, emission ranges from 440 to 600 nm. Both

curves are normalised. From [30]. (b) Absorption spectra of the dication (D), monocation

(M) and neutral molecule (N). From [31].

Quantitative bulk measurements of quinacrine in a closed fluid cell (cf. Section

2.4.4) were performed to determine the pH dependent fluorescence (Figure 2.3a).

Phosphate buffer was used because of its simplicity to fix pH. As the reference point

shows, phosphate buffer has no significant influence compared to Hepes buffer,

which is normally used. From pH 5.5, the results show a decreasing fluorescent

intensity for increasing pH, up to a factor of 2 at pH 8.0. These results are in

agreement with what is expected from absorbance graphs (Figure 2.2b). Dense

granules are slightly acidic at pH 6.1 [32]. When granules secrete their contents

in the extragranular space2 at a pH around 7 - 7.4, intensity drops by 15 to 20%

(only considering the pH effect).

Other bulk measurements of quinacrine in Hepes buffer pH 7.3 show that

quinacrine fluorescence depends on dye concentration (Figure 2.3b). Fluorescent

intensity is strongly non-linear for high concentrations. At concentrations above 10

mM a strong quenching effect is visible. The implication is that when quinacrine

concentration drops (e.g. by exocytosis), dequenching can occur for initally high

quinacrine concentrations. This will result in an increase in fluorescent intensity.

The exact nature of quinacrine quenching remains unclear, however it strongly

depends on its environment, such as calcium concentration [33]. The quenching

strength, i.e. the ratio between maximum intensity and minimum intensity at

saturating dye concentration, might be of the order of one to ten or even more

[34, 35].

2Extragranular space can be platelet cytoplasm or platelet exterior.

11

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2.4. Materials and Setup

5 . 5 6 . 0 6 . 5 7 . 0 7 . 5 8 . 00

3 0 0

3 5 0

4 0 0

4 5 0

5 0 0

5 5 0

6 0 0

6 5 0

p h o s p h a t e b u f f e r H e p e s b u f f e r , p H 7 . 4

inten

sity (a

.u.)

p H(a) pH dependence

1 E - 4 1 E - 3 0 . 0 1 0 . 11 0

1 0 0

1 0 0 0

inten

sity (a

.u.)

[ q u i n a c r i n e ] ( M )(b) Quenching

Figure 2.3: Quinacrine fluorescence depends on pH and dye concentration. In both plots,

error bars represent the spread between different positions in the closed fluid cell. (a)

Increasing pH (from 5.5) decreases fluorescent intensity up to a factor of 2 at pH 8.0. (b)

At concentrations above 1 mM fluorescence starts to level off. At concentrations above 10

mM a strong quenching effect is visible. The red line indicates a linear behaviour.

Certain dyes (e.g. acridine orange) are strong at photo-induced production of

reactive oxygen, others (e.g. FITC-dextran) are poor [36]. This reactive oxygen

can cause oxidation of co-factors, proteins and desaturated fatty acids in lipids

(lipid peroxidation). When a fluorescent dye, that is loaded into vesicles, produces

reactive oxygen, lipid peroxidation causes membrane degradation. This can even-

tually result in vesicle lysis: disintegration by rupture of the membrane [37, 38].

For vesicles loaded with fluorescent dye, both lysis (a physical effect) and real exo-

cytosis (a biological effect) result in a decrease of dye concentration. Hence, lysis

can lead to false positive exocytotic events, which is highly undesirable. From liter-

ature it is unknown if quinacrine stained dense granules induce granular membrane

degradation or granule lysis under fluorescent excitation.

2.4 Materials and Setup

2.4.1 Preparation of Washed Human Platelets

Blood was drawn from healthy donors (free of aspirin for 10 days) and anti-

coagulated with 3.2% sodium citrate. Within one hour from collection, the

whole blood sample was centrifuged at 250g for 20 minutes at room temper-

ature. Platelet rich plasma (PRP) with volume VPRP was transferred and anti-

coagulated with citrate dextrose (ACD, 0.25% citrate, 0.15% citric acid and 0.2%

D-glucose). Next, the PRP was centrifuged at 520g for 16 minutes at room tem-

perature to pellet the platelets. The pellet (supernatant was disposed) was then

resuspended in Hepes buffer (10 mM HEPES, 150 mM NaCl, 5 mM KCl, 0.3

mM NaH2PO4.H2O, 10 mM MgSO4.7H2O, 50 mM D-glucose, pH 6.5) with 100

ng/ml carbaprostacyclin (cPGI2, Cayman Chemical)3 to a final volume of VPRP .

3Carbaprostacyclin prevents platelet activation caused by e.g. resuspending. It is a stable

analog of prostacyclin (PGI2, having a lifetime of 3 minutes), which is an inhibitor for platelet

secretion and aggregation [2]. PGI2 is released by healthy endothelial cells.

12

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2.4. Materials and Setup

Again, the platelets were pelleted by centrifuging at 520g for 16 minutes at room

temperature. The pellet was finally resuspended in Hepes buffer, pH 7.3 to the

desired volume – about the original whole blood volume. Before using the washed

platelets (WP), the WP suspension was kept at room temperature for 30 min-

utes. This allows platelets that are in a reversible activation state to return to

their resting state.

2.4.2 Measuring ATP with Luciferase

A 96-well plate was coated with bovine serum albumin (BSA) to minimise substrate-

induced platelet activation. Therefor, 3% BSA in phosphate buffered saline (PBS,

10 mM phosphate buffer, 2.7 mM potassium chloride, 137 mM sodium chloride,

pH 7.4) was incubated in the wells for 1 hour and then washed with PBS. 50 to

100 µl of solution (based on Hepes buffer pH 7.3) with unknown ATP concen-

tration was added to the wells. In case TRAP (Bachem) was used to activate

platelet suspension in the well, it was added from a 10x solution approximately 5

minutes prior to the next step. Firefly luciferase (Sigma-Aldrich, 20 µg/ml final

concentration) and D-luciferin (Tebu-Bio, 50 µg/ml final concentration) were pre-

mixed in Hepes buffer pH 7.3 and then added as 10 µl to the wells just before the

measurement4. Dynamic luminescence was measured by a well plate reader using

1-second integration time per point per well for at least 1 hour. A few samples

of ATP with known concentration were used for calibration in each measurement

series. Luminescent signal intensity typically showed a slight increase in the first

30 minutes, followed by a slight decrease. The maximum intensity was used for

data analyses.

2.4.3 Substrate-Induced Activation

Glass coverslips (24 mm x 36 mm) were thoroughly washed in detergent (solved in

deionised water), deionised water and isopropanol respectively and blow-dried with

air. The desired primary coating was applied by incubation at room temperature.

After washing with 1% BSA in PBS, a secondary BSA coating (3% BSA in PBS,

2 hours incubation at room temperature) was applied in order to block the surface.

Then, coverslips were washed with Hepes buffer pH 7.3 and gently blow-dried.

100 µl of WP was added on top of the coverslip and incubated for one hour

at room temperature in a sealed petri dish5. After incubation, 50 to 75 µl of

supernatant was transferred into a well to determine the ATP concentration with

the luciferase reaction (Section 2.4.2). Although incubation took place in a sealed

petri dish, results were corrected for evaporation, which is of the order of 10%.

Results were compared with ATP concentrations in untreated WP and ac-

tivated WP (activated with 400 µM TRAP for at least 5 minutes prior to the

measurement).

4Protocol adapted from Van Holten, Department of Clinical Chemistry and Haematology,

University Medical Centre Utrecht5From microscope images it was concluded that in one hour most of the platelets sediment

and interact with the substrate.

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2.4. Materials and Setup

2.4.4 Imaging Labelled Granules

Glass coverslips were thoroughly washed (Section 2.4.3). The surface was coated

with BSA (3% BSA in PBS, 2 hours at room temperature). After incubation,

the coverslips were washed with Hepes buffer pH 7.3. 0.5 µl of WP was added

per 1 mm2 of surface area, followed by 20 µM quinacrine (final concentration,

added from 10x stock). WP and quinacrine were incubated for 30 minutes at room

temperature, allowing the platelets to sediment onto the coated surface. Unbound

platelets and excess quinacrine were washed out with Hepes buffer. Unless stated

otherwise, biocompatible imaging spacers (9 mm well diameter, 0.12 mm height)

were used to create a closed fluid cell filled with Hepes buffer (Figure 2.4).

BSA-coated coverslipincubated with WP

coverslip

double-sidedbiocompatible tape

Figure 2.4: Fluid cell construction, exploded view. Biocompatible double-sided tape (9 mm

well diameter, 0.12 mm height) is sandwiched between a BSA-coated coverslip incubated

with washed platelets and a clear coverslip.

Labelled platelets on the bottom of a fluid cell were imaged with a inverted

microscope (Leica DMI5000 B) and a 40x objective lens. The fluorescence light,

provided by a metal halide bulb (Leica EL6000), excites fluorophores in a ∼ 500

x 500 µm2 area. A filter cube with excitation filter (bandpass, 450 - 490 nm),

dichroic mirror (510 nm) and suppression filter (lowpass 515 nm) (Leica I3) was

used.

Stained granules were imaged by a high sensitivity camera (Hamamatsu C10600-

10B (ORCA-R2)) at 2 or 5 Hz. At 40x one pixel covers 0.25 x 0.25 µm2, the total

imaging area is approximately 330 x 250 µm2. Bright field images were taken prior

and/or posterior to fluorescence movies to identify the position of the platelets.

2.4.5 Data Analysis

Movie files were analysed by home-brew software. Granules were pinpointed man-

ually6. Next, the software analyses a 5 x 5 pixel region (which is approximately the

size of the point spread function of the microscope objective) around the centre,

i.e. the brightest pixel, of the granule (Figure 2.5a). The average intensity, cor-

rected for photobleaching and other fluctuations with background intensity from a

nearby platelet-free area, is plotted over time. From the curve, parameters such as

release delay, release duration, initial intensity and final or remaining intensity can

be extracted (Figure 2.5b). Intensity parameters were fitted by horizontal lines,

the release duration is approximated by a straight best-fit line. The time t = 0

6An automated granule recognition algorithm needs careful approach, due to the irregular

nature of granules and the high density in some regions.

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2.4. Materials and Setup

can be defined by a special event, such as the addition of agonist or the onset of

fluorescent light.

(a) Fluorescence image

0 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 00

2 0

4 0

6 0

8 0

1 0 0

1 2 0

1 4 0

r e l e a s e d u r a t i o n

r e l e a s e d e l a yf i n a l / r e m a i n i n gi n t e n s i t y

light in

tensity

(a.u.

)

t i m e ( s )

i n i t i a l i n t e n s i t y

(b) Granule intensity over time

Figure 2.5: Data analysis. (a) Fluorescence image of platelet showing two granules. The

marked area indicates a 5 x 5 pixel (= 1.25 x 1.25 µm2) region around the centre of the

granule used for analysis. (b) Granule intensity over time. Release delay, release duration,

initial intensity and final or remaining intensity can be extracted.

15

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Chapter 3

Results

Platelet activation in bulk and substrate-induced activation was first investigated

with the luciferase assay. Those result were used for an optimal single platelet

activation assay using quinacrine.

3.1 Bulk Activation

3.1.1 Quinacrine Does Not Influence TRAP-induced Platelet

Activation Significantly

A dose-response of TRAP-stimulated platelets was measured with the luciferase

assay for both unlabelled washed platelets (WP) and WP (same donor) incubated

with 20 µM quinacrine (Figure 3.1). ATP concentrations represent the degree of

degranulation, i.e. the level of activation. A sigmoid curve fit is applied to the

data (Table 3.1):

s(c) = s0 +s1 − s0

1 + (c0/c)p. (3.1)

Here, c denotes the concentration of TRAP, c0 the concentration which induces

a response s halfway between the baseline s0 and maximum response s1 and p is

a measure for the slope at c0. The response (ATP concentration) was calibrated

with samples of known ATP concentrations. Measurements without WP, but

with fixed concentrations of ATP (not shown) indicate that quinacrine and TRAP

have no significant effect on the luciferase reaction for the ATP range typical in

experiments with platelets (10 µM and below).

With a platelet concentration of 89200 platelets/µl (counted with a flow cy-

tometer), fully activated WP release 4.83 nmol ATP/108 platelets, which is in

agreement with values found in literature [39].

It can be concluded that quinacrine does not effect platelet activation by TRAP

significantly: there is no notable difference in c0. A decreased level of maximum

activation of about 15% for WP incubated with quinacrine is observed, however

platelets can still be activated with TRAP. The effect of quinacrine on processes

other than dense granule release through TRAP remains unknown.

17

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3.1. Bulk Activation

0 . 1 1 1 0 1 0 0 1 0 0 00

1

2

3

4

5

W P W P + Q u i n a c r i n e

[ATP]

(µM)

[ T R A P ] ( µM )

Figure 3.1: Dose-response curve of TRAP-stimulated washed platelets (WP), either incu-

bated with 20 µM quinacrine or without. Each point was only sampled once.

Table 3.1: Fitting parameters for dose response curve of unlabelled washed platelets (WP)

and WP incubated with 20 µM quinacrine.

WP WP + Quinacrine

s0 (µM ATP) 0.38 ± 0.14 0.33 ± 0.09

s1 (µM ATP) 4.31 ± 0.16 3.55 ± 0.13

c0 11.5 ± 1.2 15.8 ± 1.7

3.1.2 Platelet Responsiveness Changes over Time

In order to evaluate platelet activation over the course of time, a flow cytome-

try study is performed by Loes van Zijp (for technical details, see [18]). In this

experiment, P-selectin expression on the outer membrane, a quantity for platelet

activation, is measured over time (Figure 3.2). Two batches of WP from the

same donor were analysed to investigate the best storage method. Batch 1 was

prepared approximately 30 minutes after blood was collected from a donor, batch

2 was prepared ∼350 minutes later (whole blood was kept at room temperature).

Baseline and maximum response (cf. Section 3.1.1) were measured. The time

t = 0 is 30 minutes after the last washing step (cf. Section 2.4.1). Actual mea-

surements took place 30 minutes after the indicated time: samples were incubated

for 20 minutes with 800 µM TRAP and fixed with 0.2 % formaldehyde solution

for 10 minutes1.

Neglecting outliers2, results show a clear trend of decreasing responsiveness

(maximum response). In four hours, responsiveness is reduced by 35%. The

data points for batch 1 and batch 2 overlap remarkably well. Therefore it can be

concluded that storing platelets in whole blood does not result in higher respon-

siveness compared to storing WP in buffer. The decrease in maximum response

is not compensated by an increase in baseline response (non-activated WP). The

1Fixation, i.e. termination of any ongoing biochemical reactions, is needed for flow cytometry

measurements. Formaldehyde does so by cross-linking proteins.2Outliers from the trend currently cannot be explained since procedural errors cannot be

excluded completely.

18

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3.2. Substrate-Induced Activation

0 1 0 0 2 0 0 3 0 0 4 0 0 5 0 00

1 0

2 0

3 0

4 0

5 0

6 0

7 0

n o t a c t i v a t e d

b a t c h 1b a t c h 2

P-Sele

ctin ex

pressi

on (a

.u.)

t i m e ( m i n )

a c t i v a t e d ( 8 0 0 µM T R A P )

Figure 3.2: Platelet responsiveness as measured by P-selectin expression over time. Two

batches of WP (originating from the same sample of whole blood) were measured; batch

2 was prepared ∼350 minutes after batch 1. The dashed line is merely a visual indication

to separate activated and non-activated WP.

exact nature of this behaviour and its implications for fluorescent labelling are

unknown.

In conclusion, older platelets are less sensitive to activation by TRAP and there

is no increase in pre-activation.

3.2 Substrate-Induced Activation

3.2.1 BSA Coated Surface Shows Least Induced Activation

Different surface coatings were applied to glass coverslips (Table 3.2) to immobilise

platelets. Washed platelets (WP, same donor) were incubated on the coated glass

for one hour. Next, the ATP concentration of supernatant was analysed with

the luciferase assay (Figure 3.3a). As a reference, ATP concentrations of both

untreated WP and WP incubated with 200 µM TRAP, i.e. baseline en maximum

response (cf. Section 3.1.1), are shown. BSA clearly induces the least activation.

The analysed supernatant only contained few platelets3, demonstrating that most

of the platelets interacted with the surface.

It is unclear from these results if the interactions between substances and

platelet (receptors) are responsible for activation. For example, from flow cy-

tometry studies it is known that platelets labelled with aGP1b in solution are not

activated completely. Moreover, there is no evidence in literature that BSA induces

direct platelet activation. From these observations, it is deduced that binding to a

surface leads to activation, rather than the interactions themselves. The strength

of the (nonspecific) surface bonds might determine the degree of activation.

3In a different measurement, supernatant from a BSA coated surface was incubated with

200 µM TRAP, i.e. any remaining platelets were activated. Results were compared to pure (i.e.

non-treated) supernatant. ATP concentrations relative to bulk activated WP were respectively

0.38 and 0.25. This indicates supernatant contained only few platelets.

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3.2. Substrate-Induced Activation

Table 3.2: Different glass coating procedures.

coating (primary) wash coating (secondary)

aGP1b1% BSA in PBS 3% BSA in PBS (∼2h)

(10 µg/ml in PBS, ∼20h)

mouse IgG1% BSA in PBS 3% BSA in PBS (∼2h)

(200 µg/ml in PBS, ∼20h)

PLLPBS 3% BSA in PBS (∼2h)

(1 mg/ml in H2O, ∼20h)

BSA

(3% in PBS, ∼2h)

0 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

1 . 2

1 . 4

1 . 6

1 . 8 s u p e r n a t a n t p l a t e l e t s u s p e n s i o n

aGP1

b

mous

e IgG

WP +

TRAP

BSA

WP

glass

(unco

ated)

norm

alised

[ATP

]

PLL

(a)

0 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

1 . 2

1 . 4

1 . 6

1 . 8

mous

e IgG

(high

)

aGP1

b / Fc

R bl

mous

e IgG

(high

) / Fc

R bl

mous

e IgG

(low)

mous

e IgG

(low)

/ FcR

bl

WP

WP +

TRAP

norm

alised

[ATP

]

aGB1

b

(b)

Figure 3.3: Substrate-Induced Activation. Measurements in (a) and (b) are from two

different donors. In both figures, ATP concentrations are normalised to the ATP concen-

tration found in activated washed platelet suspension. Each value is the average of three

samples, error bars represent the spread. (a) Different surface coatings induce dissimilar

platelet activation. BSA induces the least activation. (b) Platelets incubated with Fc re-

ceptor blocker (FcR bl) show reduced substrate-induced activation. Two concentrations

were used for mouse IgG surface incubation: 200 µg/ml (high) and 10 µg/ml (low).

On the outer surface of platelets, Fc receptors (FcR) are present. These

proteins bind to the Fc region of antibodies. Experiments were conducted where

WP were incubated with Fc receptor (FcR) blocker (Miltenyi Biotech, 10 times

diluted from stock) for ten minutes at room temperature preceding incubation on

coated glass. FcR blocker prevents binding of platelets with antibodies via the

Fc region4. The results show that substrate-induced platelet activation is lowered

when WP were incubated with FcR blocker (Figure 3.3b). This demonstrates that

when no blocker is used, Fc bonds that induce surface activation are present.

The difference in relative activation by antibody between the two measurements

series can be attributed to donor variance. The latter is clear from the ratio

baseline to maximum for bulk WP, i.e. the ratio of green bars (Figure 3.3).

To sum up: among other coatings, BSA is the most suitable coating for platelet

immobilisation. The binding of platelets to the surface rather than the interaction

with BSA causes activation.

4It is unknown how the antibodies like aGP1b and mouse IgG are oriented on the surface. It is

assumed that part of the antibodies are oriented such that the Fc region is available to platelets.

20

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3.2. Substrate-Induced Activation

3.2.2 Platelets Can Still Be Activated with TRAP After Incu-

bation on Substrate

Previous results show that platelets immobilised on a BSA substrate are activated

by approximately 30%. Next, experiments were carried out to prove that those

bound platelets can still reach a higher level of activation by adding TRAP.

As before, primary supernatant was removed from the surface, following a 60 or

120 minutes platelet incubation (Figure 3.4). Next, coverslips were gently washed

in Hepes buffer pH 7.3. After that, Hepes buffer with or without 200 µM TRAP

was added and incubated for 15 minutes. In this way, immobilised platelets can

be completely activated. Then, secondary supernatant was removed and analysed

with the luciferase assay.

Secondary supernatant with TRAP shows that adhered platelets can still be

activated, even when platelets were incubated for two hours on the substrate

(Figure 3.5). A negative control series with merely Hepes buffer added after

the washing step shows that platelets were barely activated by this buffer. This

observation confirms that TRAP causes the activation and not the procedure

or the buffer itself. Summing the relative ATP concentrations of primary and

secondary supernatant does not yield 1. The washing step, removing some (non-

activated) platelets and remaining supernatant, is most likely the reason.

60/120 min

primary secondary

wash, add Hepes (+/- TRAP)

Figure 3.4: Two-step substrate-induced activation assay. After primary supernatant is

transferred and analysed with the luciferase assay, the coverslip is gently washed and incu-

bated for 15 minutes with Hepes buffer pH 7.3 with or without TRAP. Then, secondary

supernatant is removed and analysed.

0 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

1 . 2

1 . 4

1 . 6 s u p e r n a t a n t p l a t e l e t s u s p e n s i o n

seco

ndary

supe

rnatan

t, Hep

es

2h1h seco

ndary

supe

rnatan

t, TRA

P

prima

ry su

perna

tant

WP

WP +

TRAP

norm

alised

[ATP

]

2h1h

1h 2h

Figure 3.5: Two-step substrate-induced activation. Two series for 60 and 120 minute

platelet incubation are displayed. Secondary supernatant with TRAP shows that adhered

platelets can still be activated.

21

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3.3. Fluorescent Imaging of Single Platelet Activation

3.3 Fluorescent Imaging of Single Platelet Activa-

tion

Previous measurements show that platelets immobilised on a BSA coated glass

substrate are suitable for fluorescence microscopy with quinacrine labelled dense

granules. The BSA surface already induces degranulation, however, adding TRAP

should result in additional release events visible as decrease or loss of fluorescence

intensity.

3.3.1 Types of Release Events

Without discussing the origin yet, several exocytotic-like events were visible when

imaging washed platelets incubated with 20 µM quinacrine on a BSA substrate.

Events were analysed by plotting granular fluorescent intensity versus time. Some

events show a monotonically decreasing intensity (Figure 2.5b), whereas others

show a spike prior to decrease (Figure 3.6a) which is visible as a flash in the

movie. Movements along the z-direction, i.e. movements in or out of the focal

plane, contribute to an intensity change of at most 10% for shifts of ∼1 µm.

As a result, flashing phenomena are not caused by drifts in or out of the focal

plane, but are attributed to quenching (or actually dequenching) of quinacrine

(Section 2.3). Due to high background levels of the order of 100 light intensity

units, the actual increase in intensity is a factor of two. Although exact quenching

interactions are unknown, this factor matches the expected factor from quinacrine

quenching solely based on concentration (Figure 2.3b). The high background

intensity combined with strong quenching also obscures some granules; only flashes

(dequenching) signal the presence of granules (Figure 3.6b). The background

signal is mainly caused by bulk fluorescence of the fluid with low concentrations

of leaked quinacrine. This was measured by varying fluid cell height: background

intensity was proportional to cell height.

0 2 0 4 0 6 0 8 0 1 0 00

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

light in

tensity

(a.u.

)

t i m e ( s )

(a)

0 2 0 4 0 6 0 8 0 1 0 00

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

light in

tensity

(a.u.

)

t i m e ( s )

(b)

0 2 0 4 0 6 0 8 0 1 0 00

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

light in

tensity

(a.u.

)

t i m e ( s )

(c)

Figure 3.6: Some release events from a single measurement. Background intensity is of the

order of 100 light intensity units. (a) A spike, or flash, prior to decrease in signal intensity

is attributed to quenching of quinacrine. (b) High background intensity combined with

strong quenching obscures some granules, only flashes (dequenching) signal the presence

of granules. (c) A visually apparent single granule shows well-separated events in time,

indicating the presence of two granules. The two first peaks (at 5 and 25 seconds) originate

from neighbour granules.

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3.3. Fluorescent Imaging of Single Platelet Activation

The point spread function of ∼1 µm leads to visual overlap in granules. With

the current hardware, it is impossible to visually separate granules distanced less

than 500 nm. Moreover, the irregular shape of dense granules makes it even harder

to discriminate between two granules. However, if a visually apparent single granule

shows well-separated (release) events in time (Figure 3.6c), it can be concluded

that more granules contribute to the intensity graph5.

Heuristic observations indicate a strong sample to sample variation from the

same donor. Within one fluid cell, there is even a notable spot to spot difference,

making it inherently challenging to compare results. Also a time dependence needs

to be taken into account, as already measured before (Section 3.1.2).

3.3.2 Granule Lysis Is Induced by Excitation Light

To investigate if excitation light in combination with quinacrine can lead to vesi-

cle lysis, the number of events were analysed as a function of time (Figure 3.7).

Washed platelets were incubated with 20 µM quinacrine on a BSA substrate.

No agonist was used, which means that any observed event is either caused by

substrate-induced activation or by granule lysis. Two measurements on the same

sample were performed. First one with low excitation intensity during one minute,

after which intensity is increased by a factor of four. A second spot was analysed

with constant low light intensity (Figure 3.7a). With intenser excitation, an in-

creased number of events per time unit is clearly visible, indicating light induced

events. Another sample (same preparation) was analysed, now t = 0 is defined

as the onset of excitation light (first exposure) (Figure 3.7b). The first event was

recorded at 16 seconds and a reduced event rate is observed in the first minute.

Again, this indicates light induced events: if merely substrate induced events were

recorded, a concave graph is expected (i.e. the slope of the graph would not

increase in time).

In order to evaluate if the photo-induced observed events are truly lysed gran-

ules – and not photo-induced exocytosis (i.e. photo activation of platelets) –

proteins were disabled by fixation with formaldehyde (cf. Section 3.1.2). As a

consequence, platelets are unable to deform and release granules, both processes

mediated by proteins (cf. Section 1.1.3).

After platelet incubation on the substrate and washing, a closed fluid cell was

filled with 0.2% formaldehyde instead of Hepes buffer. Samples were incubated at

room temperature for 1 hour prior to fluorescent imaging. Recordings clearly show

events (decrease or loss of fluorescence) (Section 3.3.3). This indicates that the

observed events are the result of physical rather than biological processes. Ergo,

excitation light induces granule lysis. The next section deals with characteristics

of the observed events.

5It is assumed granular fusion is an all-or-none event.

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3.3. Fluorescent Imaging of Single Platelet Activation

0 5 0 1 0 0 1 5 0 2 0 00

5 0

1 0 0

1 5 0

2 0 0

2 5 0

3 0 0

3 5 0

cu

mulat

ive co

unt (a

.u.)

t i m e ( s )

v a r i a b l e l i g h t i n t e n s i t y c o n s t a n t l i g h t i n t e n s i t y

l i g h t i n t e n s i t y i n c r e a s e d

(a)

0 2 5 5 0 7 5 1 0 0 1 2 5 1 5 0 1 7 50

2 5

5 0

7 5

1 0 0

1 2 5

1 5 0

1 7 5

l i g h t i n t e n s i t y i n c r e a s e d

cumu

lative

coun

t (a.u.

)

t i m e ( s )(b)

Figure 3.7: Granule lysis induced by excitation light. The vertical axis denotes the cumula-

tive count of events. (a) Increasing excitation light intensity clearly results in an increased

number of events per time unit. Both graphs are normalised, such that for 0 < t < 60

seconds they overlap. The onset of light is at t < 0. (b) A reduced rate of events during

the first minute after the onset of excitation light (t = 0, first exposure) indicates light

induced events.

3.3.3 Discriminating Granule Lysis from Exocytosis

From bulk measurements it is known that platelets can still be activated with

TRAP after incubation on a BSA substrate. Although excitation light induces false

positive exocytotic events, platelets should show degranulation upon activation

with TRAP. Non-activated platelets were compared with activated platelets to

investigate differences in events. An attempt is made to discriminate granule lysis

from exocytosis.

Washed platelets (WP) were incubated on a BSA coated glass substrate as be-

fore. No cover glass is used to close the cell, the spacer remains in place. The open

well was then filled with 20 µl of Hepes buffer and positioned on the microscope

stage. 2.5 µl of 10 mM TRAP (yielding a final concentration of ∼1 mM) was care-

fully pipetted into the open fluid cell. Prior to addition and immediately following

addition, data was recorded at different spots for two minutes. The average num-

ber of exocytotic-like events per platelet is equal prior to and following addition of

TRAP for two samples (Figure 3.8). Thus, addition of TRAP does not result in

extra events. From these results, it is unclear whether real exocytotic events are

present or absent in the pool of all events. Hence, the features of the events were

analysed, such as duration and intensity. Measurements on formaldehyde-fixed

platelets were compared to post-TRAP events. Fixed platelets were chosen to be

absolutely positive that all events are identified as vesicle lysis.

24

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3.3. Fluorescent Imaging of Single Platelet Activation

0 . 0 0

0 . 0 5

0 . 1 0

0 . 1 5

0 . 2 0

0 . 2 5

0 . 3 0

s a m p l e 1

s a m p l e 2

p r e T R A P p o s t T R A P

# eve

nts / #

plate

lets

Figure 3.8: Average number of (release) events per platelet prior to and immediately follow-

ing addition of TRAP are equal for two samples. Events were recorded during approximately

one minute. The difference between samples, both incubated at the same time and mea-

sured only 15 minutes apart, might be the result of time.

0 4 8 1 2 1 6 2 00 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

coun

t

d u r a t i o n ( s )

N = 4 8

(a) post-TRAP

0 4 8 1 2 1 6 2 00 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

coun

t

d u r a t i o n ( s )

N = 5 5

(b) Formaldehyde-fixed

Figure 3.9: Histogram of event durations for events posterior to addition of TRAP (a) and

when platelets were fixed with formaldehyde (b). Counts are normalised to the second and

highest bin between 2 and 4 seconds. Each data set is composed of two samples from the

same donor. Different donor material is used in TRAP and formaldehyde experiments.

Calculations and simulations demonstrate that exocytosis of a granule through

the OCS takes well below 1 second, more specifically of the order of 10 ms (Ap-

pendix B). In these calculations, it is assumed that quinacrine and ATP diffuse

freely through the OCS and that both substances are non-bound in the gran-

ule, i.e. they can freely diffuse out of the granule. Events in measurements on

formaldehyde-fixed platelets manifest a typical time scale of a few seconds (Figure

3.9b). This confirms that these events are not exocytotic. Measured time scales

match time scales as measured for photo-induced vesicle lysis in astrocyte cells

[36].

Event durations of fixed platelets were compared to event durations from ex-

periments with addition of TRAP (Figure 3.9a). A small increase in short duration

events is visible for measurements with TRAP. This difference can be caused by

real exocytotic events or by natural sample variations. Therefore, those relatively

fast events are analysed further by investigation of cytosolic fluorescence.

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3.3. Fluorescent Imaging of Single Platelet Activation

When granules lyse, their contents diffuse through the entire cell cytosol.

Seemingly, quinacrine diffuses slowly through the outer cell membrane, and an in-

creased cytosolic fluorescence might be visible for several seconds (Figure 3.10a).

In fact, this cytosolic fluorescence sometimes causes an apparent event duration

of several seconds, while the actual event (lysis) might take shorter. The cy-

tosolic light is clearly not from light scattered (scattering is a linear effect) from

the vesicle. Data (not shown) indicate that granule intensity sometimes does not

increase, while cytosolic intensity does in those cases. It is highly unlike that cy-

tosolic fluorescence can be attributed to quinacrine fluorescence inside the OCS,

since calculations show that once inside the OCS, quinacrine diffuses out rapidly

(of the order of a few milliseconds).

(a) Bright field image and fluorescence movie showing cytosolic fluorescence

0 1 0 2 0 3 0 4 0 5 00

1 0 0 0

1 2 0 0

1 4 0 0

1 6 0 0

1 8 0 0

2 0 0 0

c y t o s o l i c i n t e n s i t y g r a n u l e i n t e n s i t y

light in

tensity

(a.u.

)

t i m e ( s )(b) Cytosolic vs. granule intensity

Figure 3.10: (a) Left image: bright field image of platelet, outlined with a red dotted

line. Other five images: fluorescence movie of release event. Cytosolic fluorescence can be

observed, indicating the contents of lysed granules diffuses slowly out of the platelet. Images

are shown for every 0.5 second, increasing in time from left to right. Image dimension are

10 µm x 10 µm. (b) Cytosolic intensity (black line, averaged per pixel, area in between the

two squares (15 x 15 pixels and 5 x 5 pixels) (a)) and granule intensity (red line, averaged

per pixel, small square (5 x 5 pixels)) are plotted versus time. In the graph that is shown,

the ratio of peak cytosolic intensity and peak granule intensity equals 0.72.

The cytosolic fluorescence can be used as a parameter to identify vesicle lysis.

In order to make a quantitative analysis, the ratio of peak cytosolic intensity and

peak granule intensity is examined (Figure 3.10b). The granule intensity is as

defined before: the average (per pixel) intensity of a 5 x 5 pixels area around

the granule centre. The cytosolic intensity is defined as the average intensity of

the area between a 15 x 15 pixels square centred around the granule and the 5 x

5 pixels square (Figure 3.10a). The distribution of ratios for formaldehyde-fixed

platelets is plotted to characterise vesicle lysis (Figure 3.11). All events, including

those that do not show a clearly visible cytosolic fluorescence, are included. Ratios

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3.3. Fluorescent Imaging of Single Platelet Activation

are typically 0.7 and higher. For exocytotic events, ratios are expected below 0.6

(this number is limited by the background intensity).

The three fastest events, around 0.6 seconds or 3 frames, from the post-

TRAP measurement (Figure 3.9a) are candidates to be identified as exocytosis.

For these events, the ratios peak cytosolic intensity to granule intensity lie between

0.67 and 0.78. Comparing with the distribution for formaldehyde-fixed platelets,

the selected events cannot be identified as exocytosis.

It can be concluded that for experiments performed in this work, no physiologi-

cal events can be recognised with analysis based on event duration and fluorescent

intensity.

0 . 6 0 . 7 0 . 8 0 . 9 1 . 0 1 . 1 1 . 2 1 . 3 1 . 40

5

1 0

1 5

2 0

coun

t

p e a k c y t o s o l i c i n t e n s i t y / p e a k g r a n u l e i n t e n s i t y

N = 5 5

Figure 3.11: Distribution of the ratio peak cytosolic intensity and granule intensity (cf.

Figure 3.10b) for formaldehyde-fixed platelets. This distribution characterises vesicle lysis.

Background intensity typically limits the ratio to around 0.6.

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Chapter 4

Discussion & Conclusion

Platelets play a crucial role in haemostasis. Upon activation, platelets release small

messenger molecules from their granules to facilitate platelet aggregation. Single

cell techniques are required to measure fundamental properties of this release.

Prior to the study presented in this work, the luciferase assay was reviewed for

measuring single platelet activation. This assay can be used to visualise exogenous

ATP secreted from dense granules in bulk (cf. Section 2.1). Previous studies show

that luciferase immobilised on beads [40] or on the platelet surface [41] can be

used to measure local ATP concentrations at the platelet surface. However, these

immobilisation methods were only used in bulk. Estimations based on diffusion

theory show that detection of ATP released by a single platelet is highly challenging

(Appendix A). From experiments (not shown in this work), it can be concluded

that using luciferase for a single platelet assay is not feasible with the current

hardware.

In this study, fluorescent labelling of dense granules with quinacrine, which

binds ATP, was explored to obtain spatial and temporal characteristics of the

dense granule release.

Bulk measurements showed that quinacrine clearly has an effect on platelets.

Activation by TRAP, studied by means of ATP release from dense granules, is

approximately 15% less for platelets incubated with quinacrine. However, since

platelets can still be activated and the halfway response of the dose response

curve does not change for quinacrine, it is assumed that the fluorescent label

does not influence release characteristics considerably. The effect of quinacrine on

other platelet activation processes, such as membrane receptor sensitivity for other

molecules than TRAP, alpha granule release or shape change, remains unknown.

Platelet immobilisation needed for fluorescence microscopy is a challenging ob-

jective. Any surface other than endothelial cells (cells that line the inner blood

vessel wall) will activate platelets. Endothelial cells release prostacyclin, an in-

hibitor for platelet secretion and aggregation, making them not suitable as sub-

strate. BSA coated glass was found suitable for immobilisation. Although the

surface induces partial activation – from fluorescence images with quinacrine it is

believed that part of the dense granules in a single platelet is released, however

further studies need to be conducted – adding TRAP will activate platelets more.

Exact time scales on which the agonist activates platelets are unknown. The lu-

29

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ciferase assay is rather slow to investigate this, so a better procedure needs to be

explored. This can be done by e.g. electrochemical measurements [15]. However,

TRAP is known to be a strong agonist [2], and other agonists like thrombin have a

activation delay of the order of seconds [15]. Therefore it is assumed that TRAP

is appropriate for real-time single cell microscopy, which requires a fast-acting

agonist.

Quinacrine is not very suitable for studying real-time granule release. Events

were undoubtedly related to photo-induced processes. Experiments with formal-

dehyde-fixed platelets confirm that the events do not result from light-induced

activation, but are merely a physical process. Like with other dyes as acridine

orange [38], it is thought that under excitation light it produces reactive oxygen

which causes peroxidation of (granular) membrane lipids eventually leading to lysis.

A lower concentration of quinacrine would reduce the amount of lysis events and

would also increase the time delay before initiation of events, as found for acridine

orange [36]. In order to decrease the quinacrine concentration or light intensity

and still have sufficient signal, the fluorescent background should be reduced. This

can be achieved for example by reducing the height of the fluid cell or using a flow

cell with continuous supply of non-fluorescent buffer. Another option is to use

total internal reflection fluorescence microscopy (TIRFM), that has an intrinsic

high signal to background ratio. Low dye concentration (which is also present

in the cell cytosol, but at lower concentration than in granules) or reduction of

excitation light intensity will still lead to production of reactive oxygen. Though

possibly not resulting in granule lysis, the radicals might still alter cell behaviour.

Scavengers for (reactive) oxygen might be used to prevent granule lysis. However,

such agents may alter cell physiology. The same bulk techniques that were used

to study quinacrine influence can be used to address the effect of these oxygen

scavengers.

An attempt was made to resolve granule lysis from exocytosis. When com-

pared to non-treated resting platelets, addition of TRAP did not change the av-

erage number of events per platelet. Therefore, the duration of events was anal-

ysed. Calculations show that granules fusing with the membrane release their

contents in a period of the order of 10 ms, which matches release times of sero-

tonin (also a dense granule substance) [4]. Events, both for formaldehyde-fixed

platelets and for platelets treated with TRAP, last for several seconds, suggesting

non-exocytotic events. The long duration events can be explained in two ways.

First, membrane degradation may results in a perforated membrane, leading to

slow diffusion of quinacrine. Second, some platelets show long duration cytosolic

fluorescence, which may mask the true (lysis) event. Some short-duration events

(around 0.6 seconds) were recorded for TRAP-treated platelets, while not present

in formaldehyde-fixed platelets. This difference is present due to sample variations:

the events still showed a cytosolic fluorescence, marking them as lysis. No exocy-

totic events can be recognised for TRAP-treated platelets with analysis based on

event duration and fluorescent intensity. This can be caused by the effect of reac-

tive oxygen, which might alter the TRAP-induced response. Bulk measurements

in combination with quinacrine and excitation light can be used to evaluate this

effect.

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In conclusion, quinacrine is a marker that induces unwanted effects such as

granule lysis. Current measurements make it impossible to discriminate vesicle

lysis from exocytosis. Future work can focus on the reduction of unwanted effects

by reducing quinacrine concentration and excitation power after increasing the

signal to noise ratio or on the use of oxygen scavengers. Another option is to

abandon quinacrine and use other endogenous dyes, such as Ca dyes, to visualise

platelet activation. Also exogenous markers can be used, though losing direct and

spatial information.

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Chapter 5

Acknowledgements

The author would like to thank Loes van Zijp and Arthur de Jong for supervising

this research project. They and also Holger Kress are acknowledged for helpful

discussions. I would like to thank all fellow students in the student room for their

company and discussions, and again Loes for providing some 2D fishes to make

the view in the room more bearable. Finally, my thanks go to all other members

of the MBx group for the help in the labs, (lunch) talks, board game nights, and

many other things I do not mention here.

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Appendix A

Using Luciferase for a SinglePlatelet Assay

Here, the feasibility of using luciferase for visualising ATP released from a single

granule will be discussed. For that purpose, diffusion theory is used to estimate the

number of ATP molecules available for the luciferase reaction (cf. Section 2.1).

This number is compared to the number of photons that are eventually collected

and detected by the camera.

For simplicity, the shape of a platelet is modelled as a sphere with radius R.

In first approximation, the ATP is released homogeneously distributed over the

entire cell surface 1. The solution of the steady state diffusion equation, ∇2c = 02, where c denotes the (molar) concentration, is for spherical symmetry

c(r) = cR ·R

r, (A.1)

with cR the concentration at the surface. From Fick’s first law of diffusion, j =

−D · ∇c , the ATP diffusion flux at the surface jR can now be acquired:

cR = jR ·R

D, (A.2)

Here, D is the diffusion coefficient of the ATP molecules. The flux can be esti-

mated by

jR =nATP∆t · A, (A.3)

where nATP denotes the number of moles ATP in a single granule, ∆t the release

duration and A the platelet surface area.

As a next step, the number of ATP molecules N present in the focal volume

of a single pixel, Vpix , can be estimated using Avagrado’s number NA:

N =1

α

Vpix∫c · NA dV. (A.4)

1ATP from dense granules is released through the OCS, which has surface invaginations

spread over the outer membrane. A correction for this is applied later.2Again for the sake of simplicity, steady state is assumed and consumption of ATP molecules

by the luciferase reaction is neglected. Therefore, the obtained result should rather be interpreted

as an upper limit than an expected value.

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The factor 1α (α < 1) is present to correct for the fact that ATP is only released

from surface invaginations of the OCS. As a consequence, the effective concentra-

tion becomes higher. It is assumed that the focal area of a single pixel Apix (0.25 x

0.25 µm2, parallel to the membrane) is much larger than the opening of the OCS.

Furthermore, it is assumed that Vpix only covers zero or one openings. Then, α is

defined as the ratio of number of pixels that cover a surface invagination to the

total number of pixels that cover the platelet. That is, α = Nopening/ (A/Apix),

with Nopening the total number of surface invaginations.

Combining equations (A.1) through (A.4) and filling in the corresponding num-

bers (Table A.1), the expected number of ATP molecules in a focal volume is

N = 1 · 105. The value is comparable to the number of ATP molecules available

per opening: nATP · NA/Nopening ≈ 5 · 105

Table A.1: Typical values for quantities involved in granule release.

Quantity Value

R 1 µm [2]

D 300 µm2/s [42]

nATP 8 ·10−18 mole [3, 39, 43]

∆t 10 msec (Appendix B)

Nopening 10 [2, 44]

Vpix 0.25 x 0.25 x 1.0 µm3 (w x d x h)

To arrive at the number of collected photons on the camera, one needs to

take a few factors into consideration. First, the concentration of luciferase is

limiting the number of produced photons, since the molar ratio of luciferase 3 to

ATP is 2 to 1. This effect is estimated to reduce efficiency by a factor of ten.

Second, collection efficiency, that is the relative number of photons that enter

the objective, reduces the photon count be a factor of ten 4. Third, the camera

quantum efficiency around the 500 nm wavelength is about 50%, lowering the

number of counts even more. In the end, the number of detected photons is

around 500. The pixel noise of the camera is of the same order of magnitude.

In conclusion, it is highly challenging to observe light, produced by the luciferase

reaction, originating from a single granule.

3Luciferase and luciferin where used at (near) maximum soluble concentrations of 0.3 mM

and 10 mM respectively.4Calculated from the numerical aperture and refractive index of the objective.

36

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Appendix B

Granule-OCS Exocytosis:Calculations and Simulations

Platelet granules (both alpha and dense) fuse with the OCS to release their con-

tents through exocytosis [2]. In the following calculations and simulations, typical

release times are estimated for different geometries. Therefor, solutions of the

diffusion equation ∂c(~r ,t)∂t −D∇

2c(~r , t) – where c denotes the concentration, D the

diffusion coefficient, ~r position and t time – are studied. Any convective effects

are neglected.

B.1 Diffusion of Gaussian Profile in Free Space

For spherical symmetry, the solution of the diffusion equation with an initial gaus-

sian profile is

c(r, t) = c0

(t ′

t + t ′

) 32

exp

(−

r2

4D (t + t ′)

). (B.1)

Here, r is the radial position, and the following relation holds between the full

width at half maximum w and t ′:

w = 4√

ln (2)√D(t + t ′). (B.2)

In other words, t ′ can be defined by the initial (at t = 0) full width at half maximum

w0: t ′ ≈ w02/(11D).

Filling in numbers gives an idea about the time it takes for a granule-sized profile

to diffuse in free space. For w0 ∼ 0.1 µm (granule diameter) and D ∼ 100 µm2/s

(Appendix A), the centre concentration, i.e. c(0, t), drops by a factor of 1000 in

1 millisecond.

B.2 Granular Content Diffusing Through Channel

Imagine a granule, with constant volume V and spatially constant concentration

of a molecule c0, connected to a channel of length L and cross section A(x) as a

function of the position inside the channel x (Figure B.1). For small and smooth

37

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B.2. Granular Content Diffusing Through Channel

changes in A(x), diffusion is only in the x-direction. As a result, the molecular

concentration inside the channel c(x, t) is independent of the radial position.

A(x)x

Cell interior Cell exteriorGranule

L

VC!

Figure B.1: Sketch of a granule, with spatially constant concentration c0 and constant

volume V , releasing its contents through a channel of length L and cross section A(x).

Next, the discharge Q is independent of the position:

−d(c0V )

dt= Q = A(x)j(x) = A(x)D

∂c

∂x. (B.3)

Note however that the equation only holds when the concentration profile has fully

developed. This assumption will be validated later on. The concentration in the

channel can be described by:

c0(t)−L∫

0

∂c

∂xdx = αc0(t), (B.4)

where αc0 is the concentration outside the channel and can be approximated by

0 (cf. Section B.1) 1. Combining equation (B.3) and (B.4) yields:

dc0

dt= −

c0

τ, τ =

V

(1− α)D

L∫0

dx

A(x). (B.5)

Table B.1 shows two approximated timescales τ : one for a granule docked

to the membrane (diffusion through a small pore) (Figure 1.2) and one for ATP

passing a long channel mimicking the OCS. Note that the transport of ATP is

completely driven by diffusion, no shape or volume change is taken into account.

A vesicle fusing with the cell membrane (or OCS) however decreases in size (cf.

Section 1.1.3), thus reducing release times.

Table B.1: Estimated order of magnitude of release times for diffusion through a small pore

in a membrane-docked granule and diffusion through a long channel, mimicking the OCS.

V (µm3) D (µm2/s) L (µm) A (µm2) (avg.) τ ; τ ′ (ms)

0.13 1000.010 (membrane) 1 · 10−5 10; 2.5e-4

1 (platelet dim.) 1 · 10−3 (from [2]) 10; 2.5

1Typical approximated release time scales appear to be much larger then time scales of free

diffusion in open space.

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B.3. Granular Content Diffusing Through OCS

Finally, the assumption of a fully developed concentration profile needs to be

addressed. Therefore, the diffusion equation is solved with boundaries conditions

c(0, t) = c0 (kept constant in time) for all t and c(x, 0) = 0 for x > 0, i.e. the

initial profile is a step function. The solution of the diffusion equations is:

c(x, t) = c0 erfc

(−

x

2√Dt

). (B.6)

The quantity 2√Dt is the length over which to profile has developed. The time it

takes for the front to reach the channel end, that is the settling time τ ′ (2√Dτ ′ =

L) is also displayed in Table B.1. It can be concluded that the settling time does

not play a major role.

In the above calculations, the volume ratio of the channel versus the granule

is not taken into consideration. That is, the effect of a channel that is approxi-

mately equal or larger in volume than the granule is neglected. This could have

implications for the settling time. Though, simulations in the following section

show that this effect only plays a minor role.

B.3 Granular Content Diffusing Through OCS

The OCS is a complex tortuous system that can be modelled as a network with long

channels and dead-end branches (Figure B.2). In order to investigate the diffusion

properties of such a system, the diffusion equation will be solved numerically.

Furthermore, the estimations on which equation (B.5) is based will be verified.

nL

A

VC!

A

L’

Cell exterior

Cell interior

Granule

Figure B.2: Left: Sketch of a granule (initial concentration c0, constant volume V ) releasing

its contents through a single channel (length L, cross section A, cf. Figure B.1). Right:

Granule releasing its contents through the OCS, modelled as a channel with n dead-end

branches of length L′ and cross section A.

The code, plain c, to solve the 2D (planar) or 3D (cylindrical symmetry) partial

differential equation uses the straightforward finite forward difference method. As

a grid size and time resolution, respectively 5 nm and 0.01 ms is taken. Above the

opening of the channel, i.e. the cell exterior, an open (initially zero concentration)

space is simulated that is the same height L as the channel.

For a single channel, the simulated release time (solving the diffusion equation

in 3D) matches the time obtained from estimations (Section B.2) (Figure B.3a).

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B.3. Granular Content Diffusing Through OCS

The initial stronger drop in the simulation is due to the (fast) development of the

concentration profile. Simulations comparing (in 2D 2) a single channel with an

OCS-like geometry (Figure B.2) – L = L′ = 1µm, A = 0.032 µm2, V = 0.13 µm3

3, n = 10 – show that there is no significant difference in release time (Figure

B.3b). The geometry with 10 dead-end branches, which introduces an increased

effective channel volume, leads to a larger initial slope.

0 2 0 4 0 6 0 8 0 1 0 00 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

s i m u l a t i o n a p p r o x i m a t i o n

avera

ge gr

anula

r con

centr

ation

(a.u.

)

t i m e ( m s )(a) Single channel

0 2 0 4 0 6 0 8 0 1 0 00 . 0

0 . 2

0 . 4

0 . 6

0 . 8

1 . 0

0 b r a n c h e s 1 0 b r a n c h e s

avera

ge gr

anula

r con

centr

ation

(a.u.

)

t i m e ( m s )(b) Dead-end branches

Figure B.3: Solving the diffusion equation numerically for a specific geometry. Vertical

axes represent the normalised granular concentration. (a) Simulated release times match

the analytically approximated times. (b) Dead-end branches do not impose a significant

change in release time.

22D is used because of simplicity and speed.3Since the simulation is in 2D, actual parameters are: granule dimension 0.175 x 0.175 µm2,

channel width 0.030 µm. In that way, the ratio granule size to channel size is equal for 2D and

3D parameters.

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Glossary

agonist Substance that initiates a physiological response when combined with a

receptor. 5, 6, 15

alpha granule Secretory organelle that contains growth factors and other proteins

involved in coagulation. 3, 7, 29

coagulation Process of blood clotting. 4

dense granule (aka δ-granule or dense body) Secretory organelle that contains

small molecules (ADP, ATP, serotonin, ionized calcium. 3, 5, 7, 8, 10, 22,

23, 29, 35

exocytosis Process that transports contents of vesicles out of the cell membrane

by membrane fusion. 4, 10, 37

Fc receptor Protein on the cell surface that binds the Fc region – a constant

region, in contrast to two variable Fab regions that bind specific antigens –

of antibodies. 20

glycoprotein Protein that is covalently linked as a side-chain to a polysaccharide

chain. 7

haemostasis Process that stops bleedings caused by injured blood vessels. 3, 29

lysis Disintegration of a cell or vesicle by rupture of the membrane. 12, 23, 24

OCS Open Canalicular System, tortuous network of membrane invaginations tun-

nelling through the cytoplasm. 4, 25, 26, 35–40

photobleaching Phenomenon that a fluorophore loses the ability to fluoresce due

to photon-induced chemical damage. 14

quenching Process such as energy transfer or complex formation that decreases

fluorescence intensity. 11, 22

TRAP Thrombin Receptor Activation Peptide, synthetic peptide that evokes a

very strong activation response, without the complications of clot formation.

9, 13, 17–19, 21, 22, 24, 29

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