Tuesday 7 October 2014

Understand Sod ium pump and transmission of impulses

Polarization is established by maintaining an excess of sodium ions (Na +) on the outside and an excess of potassium ions (K +) on the inside. A certain amount of Na + and K + is always leaking across the membrane through leakage channels, but Na +/K + pumps in the membrane actively restore the ions to the appropriate side.

The main contribution to the resting membrane potential (a polarized nerve) is the difference in permeability of the resting membrane to potassium ions versus sodium ions. The resting membrane is much more permeable to potassium ions than to sodium ions resulting in slightly more net potassium ion diffusion (from the inside of the neuron to the outside) than sodium ion diffusion (from the outside of the neuron to the inside) causing the slight difference in polarity right along the membrane of the axon.

Other ions, such as large, negatively charged proteins and nucleic acids, reside within the cell. It is these large, negatively charged ions that contribute to the overall negative charge on the inside of the cell membrane as compared to the outside.

In addition to crossing the membrane through leakage channels, ions may cross through gated channels. Gated channels open in response to neurotransmitters, changes in membrane potential, or other stimuli.

The following events characterize the transmission of a nerve impulse (see Figure 1):

Resting potential. The resting potential describes the unstimulated, polarized state of a neuron (at about –70 millivolts).
Graded potential. A graded potential is a change in the resting potential of the plasma membrane in the response to a stimulus. A graded potential occurs when the stimulus causes Na + or K + gated channels to open. If Na + channels open, positive sodium ions enter, and the membrane depolarizes (becomes more positive). If the stimulus opens K + channels, then positive potassium ions exit across the membrane and the membranehyperpolarizes (becomes more negative). A graded potential is a local event that does not travel far from its origin. Graded potentials occur in cell bodies and dendrites. Light, heat, mechanical pressure, and chemicals, such as neurotransmitters, are examples of stimuli that may generate a graded potential (depending upon the neuron).
Figure 1.Events that characterize the transmission of a nerve impulse.

 figure
The following four steps describe the initiation of an impulse to the “resetting” of a neuron to prepare for a second stimulation:

Action potential. Unlike a graded potential, an action potential is capable of traveling long distances. If a depolarizing graded potential is sufficiently large, Na + channels in the trigger zone open. In response, Na + on the outside of the membrane becomes depolarized (as in a graded potential). If the stimulus is strong enough—that is, if it is above a certain threshold level—additional Na + gates open, increasing the flow of Na + even more, causing an action potential, or complete depolarization (from –70 to about +30 millivolts). This in turn stimulates neighboring Na + gates, farther down the axon, to open. In this manner, the action potential travels down the length of the axon as opened Na + gates stimulate neighboring Na + gates to open. The action potential is an all‐or‐nothing event: When the stimulus fails to produce depolarization that exceeds the threshold value, no action potential results, but when threshold potential is exceeded, complete depolarization occurs.
Repolarization. In response to the inflow of Na +, K + channels open, this time allowing K + on the inside to rush out of the cell. The movement of K + out of the cell causes repolarization by restoring the original membrane polarization. Unlike the resting potential, however, in repolarization the K + are on the outside and the Na + are on the inside. Soon after the K + gates open, the Na + gates close.
Hyperpolarization. By the time the K + channels close, more K + have moved out of the cell than is actually necessary to establish the original polarized potential. Thus, the membrane becomes hyperpolarized (about –80 millivolts).
Refractory period. With the passage of the action potential, the cell membrane is in an unusual state of affairs. The membrane is polarized, but the Na + and K + are on the wrong sides of the membrane. During this refractory period, the axon will not respond to a new stimulus. To reestablish the original distribution of these ions, the Na + and K + are returned to their resting potential location by Na +/K + pumps in the cell membrane. Once these ions are completely returned to their resting potential location, the neuron is ready for another stimulus.

What is an action potential/resting potential?

Information is transmitted through chemical messages called neurotransmitters, and these messages are triggered by action potentials. Every cell has a membrane voltage (difference in charge) called a membrane potential. The resting potential is the membrane potential when the neuron is not sending signals to other cells. In a human cell at resting potential, the concentration of potassium is greater inside the cell while the concentration of sodium is greater outside the cell. There are Na/K pumps inside the membrane that will transport 3 Na+ molecules outside of the cell and 2 K+ molecules into the cell. There are also many open K+ channels that allow K+ ions to flow out of the cell. Thus, the inside of the cellular membrane is negative in comparison to the positive charge outside the cell (more positive charges going out than coming in), resulting in a negative resting potential charge of about -70 mV.

An action potential is when Na+ ion channels open in response to stimuli allowing Na+ ions to flow into the cell, thus resulting in a depolarization (membrane potential becomes less negative). Once the membrane potential reaches the threshold (about -55 mV), there is a spike in membrane potential known as the action potential in which many Na+ ions are rushing into the cell. After this spike, most gated Na+ ion channels will close and K+ channels will open and the membrane potential will fall again (becoming more negative). The membrane potential will become even more negative than the resting membrane potential for a little bit (known as the undershoot, where gated K+ ion channels close) before returning back to the resting potential.

There is a refractory period in which a second activation potential cannot occur while one is already occurring because the Na+ ion channels close. Na+ ion channels will close after an activation potential passes, making sure that the activation potential travels in one direction and not backwards.

So those are the basics, sorry for the super long answer! Hope this helps. I suggest that you check out the website listed which is my professor's lecture on the membrane potentials, it includes some really nice diagrams of action potentials and neurons that help a lot. :)

How the Heart Works


The heart is responsible for circulating blood throughout the body. It is about the size of your clenched fist and sits in the chest cavity between your two lungs. Its walls are made up of muscle that can squeeze or pump blood out every time the heart "beats" or contracts. Fresh, oxygen-rich air is brought into the lungs every time you take a breath. The lungs are responsible for delivering oxygen to the blood, and the heart circulates the blood through the lungs and out to the different parts of the body.

The heart is divided into four chambers or "rooms". You can compare it to a duplex apartment that is made up of a right and a left unit, separated from each other by a partition wall known as a septum (pronounced SEP-tum).

Each "duplex" is subdivided into an upper and a lower chamber. The upper chamber is known as the atrium (pronounced AY-tree-yum) while the lower chamber is referred to as the ventricle (pronounced VEN-trickle). The right atrium (RA) sits on top of the right ventricle (RV) on the right side of the heart while the left atrium (LA) sits atop the left ventricle (LV) on the left side.

The right side of the heart (RA and RV) is responsible for pumping blood to the lungs, where the blood cells pick up fresh oxygen. This oxygenated blood is then returned to the left side of the heart (LA and LV). From here the oxygenated blood is pumped out to the rest of the body supplying the fuel that the body cells need to function. The cells of the body remove oxygen from the blood, and the oxygen-poor blood is returned to the RA, where the journey began. This round trip is known as the circulation of blood.

Do you wonder why each side of the heart has two pumping chambers (atrium and ventricle)? Why not just have a ventricle to receive blood and then pump it straight out? The reason is that the atrium serves as a "booster pump" that increases the filling of the ventricle. Filling a normal ventricle to capacity translates to more vigorous contraction or emptying. You can compare this to a strong spring. Within reasonable limits, the more you stretch a spring, the more vigorously will be its contraction or recoil. More complete filling of the ventricles thus translates into more vigorous ventricular contraction (a good thing).
The figure shown above is a section of the heart, as viewed from the front. It demonstrates the four chambers. You will also notice that there is an opening between the right atrium (RA) and the right ventricle (RV). This is actually a valve known as the tricuspid valve (pronounced try-CUS-pid). It is made of three flexible thin parts, known as leaflets, that open and shut. The figure below shows the tricuspid valve, as seen from above, in the open and shut position (the other valves pictured are discussed below).



When shut, the edges of the three tricuspid valve leaflets touch each other, preventing blood from going back into the RA when the RV squeezes. Thus, the tricuspid valve serves as a one-way door that allows blood to move only in one direction - from RA to RV. Similarly, the mitral valve (pronounced my-TRULL) allows blood to flow only in one direction from the LA to the LV. Unlike the tricuspid valve, the mitral valve has only two leaflets.

In the top diagram, you will also notice thin thread like structures attached to the edges of the mitral and tricuspid valves. These chords or strings are known as chordae tendineae (pronounced cord-EYE TEND-in-eye). They connect the edges of the tricuspid and mitral valves to muscle bands or papillary muscles (pronounced PAP-pill-larry). The papillary muscles keep the valve leaflets from flopping back into the atrium. The chords are designed to control the movement of the valve leaflets similar to ropes attached to the sail of a boat. Like ropes, they allow the sail to bulge outwards in the direction of the wind but prevents them from helplessly flapping in the breeze. In other words, they allow the valve to open and shut in a given direction but not beyond a certain point.

Lets now follow the circulation of blood more closely. Oxygen-poor blood from the head, neck and arms returns to the right atrium (RA) via the superior vena cava (pronounced VEE-nah CAVE-ah) or SVC. On the other hand, oxygen-poor blood from the lower portion of the body returns to the RA via the inferior vena cava or IVC.


When the RA is full, it contracts. This builds up pressure and pushes the tricuspid valve open. Blood now rushes from the RA into the right ventricle (RV). When the RV is filled, the walls of the ventricle begin to contract and the pressure within the RV rises. The increased pressure shuts the tricuspid valve and blood is pumped into the pulmonary artery (pronounced PULL-mun-narey) through the pulmonic valve (pronounced pull-MON-nick). The diagram below once again shows the four heart valves as viewed from the top of the heart, i.e., we are looking down at the two ventricles with the right atrium and left atrium removed.

The pulmonic valve is made up of three cusps or flexible cup-like structures, capable of holding blood. When the pressure in the right ventricle is low (as is the case when the RV is filling with blood) blood starts to move backward from the lungs toward the RV. The three cusps of the pulmonic valve fill with that blood and their sides touch each other, effectively shutting the valve. This prevents blood from leaking from the pulmonary artery into the right ventricle while the RV is filling. When the RV contracts to empty, the pressure within the RV rises above that of the pulmonary artery. This forces open the three cusps of the pulmonic valve and blood rushes through the pulmonary artery towards the lungs, where the red blood cells pick up oxygen.

The oxygenated blood from the lungs now returns to the left atrium (LA) via four tubes that are known as pulmonary veins (each draining a separate portion of the lungs). The pulmonary veins empty into the back portion of the LA. When the LA is completely filled it contracts. The mitral valve then opens, and blood is forced into the left ventricle (LV). When the LV is completely filled, it starts to empty its contents by contacting its walls. This increases pressure within the chamber, shuts the mitral valve and opens the aortic valve (AV, pronounced ey-OR-tick). The sequence is similar to that described for the RA, RV and pulmonic valve. The aortic valve also has three cusps.


The mitral and tricuspid valves open and the aortic and pulmonic valves shut while the ventricles fill with blood. In contrast, the mitral and tricuspid valves shut while the aortic and pulmonic valves open during ventricular contraction. This sequence ensures that the ventricles are filled to capacity before the ventricles start to pump blood and that the blood flows in only one direction.

After leaving the LV, blood now rushes through the aorta (pronounced a-OR-tah). The aorta is the main "highway" blood vessel that supplies blood to the head, neck, arms, legs, kidneys, etc. Blood is brought to these organs and limbs via branches that originate from the aorta. The cells within each part of the body pick up oxygen and nutrients from the blood. The oxygen-poor blood then returns to the RA, via the superior and inferior vena cava, and the beat goes on!!

Blood Pressure Measurement



Procedures
To begin blood pressure measurement, use a properly sized blood pressure cuff. The length of the cuff's bladder should be at least equal to 80% of the circumference of the upper arm.
Wrap the cuff around the upper arm with the cuff's lower edge one inch above the antecubital fossa.
Lightly press the stethoscope's bell over the brachial artery just below the cuff's edge. Some health care workers have difficulty using the bell in the antecubital fossa, so we suggest using the bell or the diaphragm to measure the blood pressure.
Rapidly inflate the cuff to 180mmHg. Release air from the cuff at a moderate rate (3mm/sec).
Listen with the stethoscope and simultaneously observe the sphygmomanometer. The first knocking sound (Korotkoff) is the subject's systolic pressure. When the knocking sound disappears, that is the diastolic pressure (such as 120/80).
Record the pressure in both arms and note the difference; also record the subject's position (supine), which arm was used, and the cuff size (small, standard or large adult cuff).
If the subject's pressure is elevated, measure blood pressure two additional times, waiting a few minutes between measurements.
A BLOOD PRESSURE OF 180/120mmHg OR MORE REQUIRES IMMEDIATE ATTENTION!

Monday 10 February 2014

DP Level Transmitter Calculation Using Diaphragm Seal

DP Level Transmitter Calculation Using Diaphragm Seal

Another installation method for level measurement using DP level transmitter is by utilizing diaphragm seal plus capillary tube. To determine the calibrated range for DP level transmitter in this installation, the fill fluid within the capillary shall be taken into account in calculation since the fill fluid also creates hydrostatic force exerting both DP level transmitter ports.
The density of fill fluid must be known, the information could be obtained from vendor catalog.
An example below describes the calculation in determining the calibrated range for DP level transmitter with capillary tube.

Given:
Process fluid density (ρP) = 950 kg/m3
Fill fluid density (ρF) = 1050 kg/m3
Maximum Level to be measured from process tap (h) = 4 m
Height Difference between two taps (h2) = 5 m
Gravitational acceleration = 9.81 m/s2
0 mA = dP at level min (left image)
∆P at min level
= P1 – P2
= Pv – (Pv + ρF . g . h2 )
= – ρF . g . h
= – 1050 . 9.81 . 5
= – 51502 Pa
= – 515 mbar
24mA = dP at level max (right image)
∆P at max level
= P1 – P2
= (Pv + ρP . g . h ) – (Pv + ρF . g . h2 )
= (ρP . g . h) -  (ρF . g . h2)
= (950 . 9.81 . 4) – (1050 . 9.81 . 5)
= – 14224 Pa
= – 142 mbar
Note that the transmitter mounting elevation can be disregard if both capillaries are filled with the same fill fluid. The transmitter elevation becomes a concern if only one leg is attached while the other port is exposed to atmosphere.

Friday 11 October 2013

Permanent Magnet Moving Coil Instruments

The permanent magnet moving coil instruments are most accurate type for direct current measurements. The action of these instruments is based on the motoring principle. When a current carrying coil is placed in the magnetic field produced by permanent magnet, the coil experiences a force and moves. As the coil is moving and the magnet is permanent, the instrument is called permanent magnet moving coil instrument. This basic principle is called D’Arsonval principle. The amount of force experienced by the coil is proportional to the current passing through the coil.

he moving coil is either rectangular or circular in shape. It has number of turns of fine wire. The coil is suspended so that it is free to turn about its vertical axis. The coil is placed in uniform, horizontal and radial magnetic field of a permanent magnet in the shape of a horse-shoe. The iron core is spherical if coil is circular and is cylindrical if the coil is rectangular. Due to iron core, the deflecting torque increase, increasing the sensitivity of the instrument.

The controlling torque is provided by two phosphor bronze hair springs.

The damping torque is provided by eddy current damping. It is obtained by movement of aluminum former, moving in the magnetic field of the permanent magnet.

The pointer is carried by the spindle and it moves over a graduated scale. The pointer has light weight so that it deflects rapidly. The mirror is placed below the pointer to get the accurate reading by removing the parallax. The weight of the instrument is normally counter balanced by the weights situated diametrically opposite and rapidly connected to it. The scale markings of the basic d.c PMMC instruments are usually linearly spaced as the deflecting torque and hence the pointer deflections are directly proportional to the current passing through the coil.

The top view of PMMC instrument is shown in the below image.


Advantages of PMMC

The various advantages of PMMC instruments are,

It has uniform scale.
With a powerful magnet, its torque to weight ratio is very high. So operating current of PMMC is small.
The sensitivity is high.
The eddy currents induced in the metallic former over which coil is wound, provide effective damping.
It consumes low power, of the order of 25 W to 200 mW.
It has high accuracy.
Instrument is free from hysteresis error.
Extension of instrument range is possible.
Not affected by external magnetic fields called stray magnetic fields.

Disadvantages of PMMC

The various disadvantages of PMMC instruments are ,

PMMC is Suitable for direct current measurement only.
Ageing of permanent magnet and the control springs introduces the errors.
The cost is high due to delicate construction and accurate machining.
The friction is due to jewel-pivot suspension.

U- Tube Manomerter | Theory, Explanation, Diagram, & Working Equations

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Construction of U-tube Manometer:

This manometer consists of a U shaped tube in which the manometeric liquid is filled. The manometer is used to measure the pressure which is unknown by the balancing gravity force and acceleration due to gravity, g = 9.81 m/sec2


The manometer consists of a steel, brass and aluminum material. It has a glass tube made up of pyralex glass. The graduations are made on the tube in terms of mm or in some condition it is graduated in kilo Pascal.

Working of U-tube Manometer:
The unknown pressure is applied in the one arm of the tube and the mercury in the tube or manometeric liquid filled in the tube moves in the tube or rises to the constant region and then the movement is stopped. The height of the liquid is measured and noted. The pressure is calculated by using the formula,

                                                                    P1-P2 = Pmhg

The above equation is arrived by 

P1 = Pthg = P2+Pmhg
P1-P2 = hg(Pt – Pm)

P1 = applied pressure
P2 = 0
Pt = specific gravity of the liquid or water
g = acceleration due to gravity.
P1 – P2 is approximately equal to Pmhg.


Advantages of U-tube Manometer:

Simple in construction
Low cost
Very accurate and sensitive
It can be used to measure other process variables.

Disadvantages of U-tube Manometer:

Fragile in construction.
Very sensitive to temperature changes.
Error can happen while measuring the h.

Characteristics of liquid used in U-tube Manometer:

Viscosity should be low.
Low surface tension is required.
The liquid should stick on the walls.
Should not get vaporized.