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INTRODUCTION TO HYPERTENSION: AN OVERVIEW TO THE ANATOMY AND PHYSIOLOGY TO THE HEART

An Overview Hey readers!! I am Sarang More an Edublogger and student. So in today’s video we are going to discuss about the PATHOPHYSIOLOGY of Hypertension. But, but, but before jumping into the actual concept it is very essential to know about the organ or the system in which the actual hypertension will be causing i.e. in heart obviously but more specifically in the arteries or the blood vessels. So in this article we are going to study about the CARDIOLOGY. Coming to the heart, it is relatively small, conical in shape and roughly as the size of one’s fist (not always possible). It is 12cm in length and 9cm in breath and 6cm thick. It weighs 250gm in adult females while in males it weighs about 300gm . The heart rest on diaphragm, near the midline of thoracic cavity known as mediastinum. Actually, the heart is slightly tilted towards left so it is said that heart is positioned to the left side. One more astounding fact about the heart is it is placed inverted in position,

Suspensions in pharmacy

 Dear readers, I am Sarang Morea former pharmacy student. Here is my first blog. It is a knowledgeable ride of one of the important topic i. e. Suspension. 

Here we go....... 


               A pharmaceutical suspension is a coarse dispersion in which internal phase is dispersed uniformly through the external phase. The internal phase consisting of insoluble solid particles having a specific range of size which is maintained uniformly throughout the suspending vehicle with the aid if single or combination of suspending agent. 


Classification :-


 ๐˜ฝ๐™–๐™จ๐™š๐™™ ๐™ค๐™ฃ ๐™œ๐™š๐™ฃ๐™š๐™ง๐™–๐™ก ๐™˜๐™ก๐™–๐™จ๐™จ๐™š๐™จ:-

Eg- Oral suspension

Externally applied suspension

Parental suspension


๐˜ฝ๐™–๐™จ๐™š๐™™ ๐™ค๐™ฃ ๐™œ๐™š๐™ฃ๐™š๐™ง๐™–๐™ก ๐™ฅ๐™ง๐™ค๐™ฅ๐™ค๐™ง๐™ฉ๐™ž๐™ค๐™ฃ ๐™ค๐™› ๐™จ๐™ค๐™ก๐™ž๐™™ ๐™ฅ๐™–๐™ง๐™ฉ๐™ž๐™˜๐™ก๐™š๐™จ:-

Eg- Dilute (2-10%v/w) suspension

Concentrated (50% v/w) suspension

๐—ฏ๐—ฎ๐˜€๐—ฒ๐—ฑ ๐—ผ๐—ป ๐—ฒ๐—น๐—ฒ๐—ฐ๐˜๐—ฟ๐—ผ๐—ธ๐—ถ๐—ป๐—ฒ๐˜๐—ถ๐—ฐ ๐—ป๐—ฎ๐˜๐˜‚๐—ฟ๐—ฒ ๐—ผ๐—ณ ๐˜€๐—ผ๐—น๐—ถ๐—ฑ ๐—ฝ๐—ฎ๐—ฟ๐˜๐—ถ๐—ฐ๐—น๐—ฒ๐˜€:-

Eg:-particles suspension

Flocculated suspension

Deflocculated suspension


๐—ฏ๐—ฎ๐˜€๐—ฒ๐—ฑ ๐—ผ๐—ป ๐˜€๐—ถ๐˜‡๐—ฒ ๐—ผ๐—ณ ๐—ฝ๐—ฎ๐—ฟ๐˜๐—ถ๐—ฐ๐—น๐—ฒ:-

Eg:colloidal suspension

Coarse suspension

Nano ๐˜€๐˜‚๐˜€๐—ฝ๐—ฒ๐—ป๐˜€๐—ถ๐—ผ๐—ป



๐˜๐—ต๐—ฒ๐—ผ๐—ฟ๐˜† ๐—ผ๐—ณ ๐—ฝ๐—ต๐—ฎ๐—ฟ๐—บ๐—ฎ๐—ฐ๐—ฒ๐˜‚๐˜๐—ถ๐—ฐ๐—ฎ๐—น ๐˜€๐˜‚๐˜€๐—ฝ๐—ฒ๐—ป๐˜€๐—ถ๐—ผ๐—ป:-


Sedimentation behaviour:-

In simple word, sedimentation behaviour can be explained as the floccules settle under the influence of gravitational force, After possessing  the stability for longer time.

According to thermodynamics, In large system the influence of gravity as correspondence to mass is negligible but due to change in medium and thermodynamically small system the influence of gravity play the huge role. 
Lets derive a small derivation For simple understanding and for your convenience. 

Let this sedimentation be “S” and surface area of floccules be “A” and viscosity be “V”.
Then,

 
         S=๐—ž๐—”

Where K is proportionality constant. 

๐—ฆ๐˜๐—ผ๐—ธ๐—ฒ'๐˜€ ๐—น๐—ฎ๐˜„:-

Velocity of sedimentation is expressed as, 

Vsed= d2 (ps-p0) g/18n
         =2[(ps-p0) g/9n]

Where, 
V= sedimentation velocity
d=diameter of particle
r= radius
Ps= density of disperse phase
Po= density of disperse medium
g= acceleration due to gravity
no= viscosity in disperse medium in poise. 

๐—ณ๐—ฎ๐—ฐ๐˜๐—ผ๐—ฟ๐˜€ ๐—ฎ๐—ณ๐—ณ๐—ฒ๐—ฐ๐˜๐—ถ๐—ป๐—ด ๐˜€๐—ฒ๐—ฑ๐—ถ๐—บ๐—ฒ๐—ป๐˜๐—ฎ๐˜๐—ถ๐—ผ๐—ป:-

๐Ÿญ. Particle size diameter. 

๐Ÿฎ. Density difference between disperse phase and disperse media
๐Ÿฏ. Viscosity of dispersion medium. 

๐Ÿฐ Sedimentation volume flocculated suspension :-

Sedimentation volume can be explained in the simple word is the difference in the formation of the cake in its active mode as well as a stable mode. 
Sedimentation volume is the ratio of final volume of sediment to original volume of sediment. 
F= Vu/Vo.

Sedimentation velocity:-

The velocity dx/dtof the particle in the unit centrifugal force can be expressed in the terms of svedberg coefficients ‘S'.


Sedimentation behaviour of flocculated and deflocculated suspension:-

Flocculated suspension-
The flocc will cause increase in sedimentation rate due to increase size of sediment in particle. 

Sedimentation depends on size of flock and porosity of flock. 

Due to formation of loose structure it entraps up appreciable amount of liquid it can be easily redispersed by agitation. 

Deflocculated suspension-

In this suspension the individual particles settle slowly as they are whole entity the sedimentation rate is low. 

The force of attraction between individual particle is high so it forms a cake at the bottom known as claying. 

The large particles settle down forming cake but small particles remain dispersed at the Superatent liquid  so it appears to be cloudy. 

As in case of flocculated suspension due to viods between big particles the small particles settle over there and super Nant liquid appears clear. 

The density and porosity of dispersed phase also plays important role.
 
๐—ฏ๐—ฟ๐—ผ๐˜„๐—ป๐—ถ๐—ฎ๐—ป ๐—บ๐—ผ๐˜ƒ๐—ฒ๐—บ๐—ฒ๐—ป๐˜ (๐—ฑ๐—ฟ๐˜‚๐—ป๐—ธ๐—ฒ๐—ป ๐˜„๐—ฎ๐—น๐—ธ) :-

Let us recall the kinetic theory of gas that we had studied earlier. 

According to kinetic theory of gas , a gas molecule remains in constant motion in its surrounding spontaneously in multi direction.

In that, the gas molecule will either bombard with another same gas molecule or the boundary between the system and surrounding.

Take that idea and apply it in the case of suspension. 

In the suspension the particle will bombard either with another gas  molecule or container which will always recharge up it’s kinetic energy. 

Hence the particle will never sediment to form a cake if particle size is between 2 to 5 mm density of particles and viscosity of medium. 

The equation for brownian movement is, 

Di2= RTt/N3ฯ€nr

Where, 
R= gas constant
T= temperatures in kelvin
N= Avogadro number
n=viscosity of medium
t= time
r= radius of particle. 

Here we can explain the NSD i. e. No sedimentation diameter. It refers to diameter of suspended particle where no sedimentation occurs in suspending system. The NSD values depend upon density and viscosity of system. 




It's my first blog . Please forgive me for any mistake. Thank you very much for giving your most precious time. 

Comments

  1. Very useful info...thanks alot

    ReplyDelete
  2. Thank you for your positive compliment. Please stay tuned with us for more educational content.

    ReplyDelete
  3. Excellent..very useful and knowledgeable keep it up

    ReplyDelete

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