Sunday 9 June 2013

CELL DIVISION

MEIOSIS
It is a reduced type of cell division taking place in germ cells that results in the formation of 4 haploid daughter cells or gametes.

STAGES OF MEIOSIS:




  • MEIOSIS I : RESULTS IN THE FORMATION OF 2 HAPLOID CELLS
  • MEIOSIS II :RESULTS IN THE FORMATION OF 4 DAUGHTER CELLS WITH HAPLOID CHROMOSOMAL NUMBER MAINTAINED.

MEIOSIS I:


Consists of 4 phases:

  1. PROPHASE I
  2. METAPHASE I 
  3. ANAPHASE I
  4. TELOPHASE I
Figure 7-18. Early primary spermatocytes of the mouse. Left to right: leptotene,
zygotene, early pachytene, midpachytene. Sudan Black squash (x1200).

PROPHASE 1:

It is the longest phase of the cycle and consists of the following substages.

  • Leptotene (lepto-Greek thin , -tene -Greek ribbon)
In this first substage of prophase I, the chromosomes have appeared within the nuclear envelope but are not yet fully condensed.  Each is a thin thread of DNA along which clearly defined beads of local coiling (chromomeres) can be seen. The chromosomes, while they have this threadlike form, are called chromatonemata .The chromosomes appear single because the sister chromatids are still so tightly bound to each other that they cannot be separately seen.


  • Zygotene (zygonema) (zygo- is Greek for union, fusing)



During zygotene homologs begin to unite (synapse) by coming into approximate alignment .Synapsis ,the process of fusion that occurs between homologs begins at various points along the chromosome and extends outward, zipper-fashion, until complete. When synapsis is finished, the fused homologs look like single chromosome under the light microscope, but that are actually double.
 The interface where two homologs unite is called a synaptonemal complex, which can be seen under an electron microcope.

In the  early zygotene , some  regions of paternal and maternal homologs have fused while In the  late zygotene, both homolog pairs have fused over their entire lengths .

Tetrads: Once the homolog pairs synapse they are called tetrads (each has four chromatids; tetra is Greek for four) or bivalents.Bivalent is the preferred term.


  • Pachytene (pachynema). (pachy- is Greek for thick). 


During pachytene the two sister chromatids of each chromosome separate from each other. This makes the chromosomes look thicker .Homologs are still paired at this point.

Each chromosome splits into two chromatids and thus each pair will have four chromatids two paternal and two maternal. They are now called tetrads.

CROSSING OVER:
The non-sister chromatids of the paternal and maternal chromosomes overlap each other. They appear to be joined at several regions along their length. These points are called Chiasmata. Each chiasma is the site of an exchange of genetic material between the two chromatids.

A kind of localized breakage of the DNA occurs, which is followed by exchange of DNA between them. This process is called crossing over or genetic recombination .Crossing over produces "cross-over chromatids," each composed of distinct blocks of DNA, some blocks derived from the mother, others from the father.



  • Diplotene OR Diplonema:

At the beginning of this stage each chromatid of each chromosome is still fused to a chromatid of that chromosome's homolog (recall that sister chromatids are already separate at this point).

As diplotene progresses, these initially fused non-sister chromatids begin to separate from each other. However, they cannot separate completely because they are still connected by two strands of DNA at each of the points where exchanges took place.At each such cross-over site, the two strands form an x-shaped structure called a chiasma (pl. chiasmata).



TERMINALIZATION:
Chiasmata then begin moving toward the ends of the chromatids. This process of sliding toward the ends is known as terminalization. 

DICTYOTENE IN OOCYTES:
In oocytes, a special, extremely prolonged form of diplotene occurs called dictyotene. The primary oocyte undergoes the first three of the substages of prophase I (leptotene, zygotene, and pachytene) during late fetal life. The process is then suspended during diplotene until puberty or thereafter. Therefore, in dictyotene (and consequently prophase I) can last months or even years, depending on the type of organism in question.

  • Diakinesis

During this, the last stage of Prophase I, the nucleolus disappears, terminalization reaches completion, and the chromosomes coil tightly, and so become shorter and thicker. The nuclear envelope begins to disappear. The centrosomes reach the poles.




LASER



LASERS--NO LONGER RESTRICTED TO CRIME-THRILLERS


A laser is a device that emits light (electromagnetic radiation) through a process of optical amplification based on the stimulated emission of photons.
The term "laser" originated as an acronym for "Light Amplification by Stimulated Emission of Radiation".
The emitted laser light is notable for its high degree of spatial and temporal coherence.

CHARACTERISTICS OF LASER LIGHT:
Laser light is very different from normal light.

  • The light released is monochromatic.
  •  It contains one specific wavelength of light (one specific color).
  •  The light released is coherent. It is “organized” -- each photon moves in step with the others.
  •  The light is very directional. A laser light has a very tight beam and is very strong and concentrated.

BOHR'S ATOMIC THEORY:


  • When an electron absorbs energy either from light (photons) or heat (phonons), it receives that incident quantum of energy. But transitions are only allowed in between discrete energy levels such as the two shown above. This leads to emission lines and absorption lines.



  • When an electron is excited from a lower to a higher energy level, it will not stay that way forever. An electron in an excited state may decay to a lower energy state which is not occupied, according to a particular time constant characterizing that transition. 
When such an electron decays without external influence, emitting a photon, that is called "spontaneous emission".


  • These excited state electrons can return to their resting state by emitting energy in the form of photons.The photon emitted has a very specific wavelength (color) that depends on the state of the electron's energy when the photon is released. Two identical atoms with electrons in identical states will release photons with identical wavelengths.


Working of a laser:
In order to produce the light rays associated with a laser thrre principles must be followed in the following order.

METASTABILITY:


STATE 1 IS METASTABLE  WHILE STATE 3 IS THE MOST STABLE

 Upon receiving certain quanta of energy ,electrons transit to another energy state (say E1 to E3).Since the stability of E3 is of the order 10ex-8 sec hence the electron soon decays to a lower energy level (say E2).However E2 is a metastable state since its life time is of the order 30ex-3 sec.

POPULATION INVERSION:


A number of problems limit the effectiveness of this approach. The central problem occurs because the lower laser level is the ground level, which is the normal state for most atoms or molecules. In order to produce the population inversion, a majority of ground state electrons must be promoted to the highly excited energy level, requiring a significant input of external energy. In addition, the population inversion is difficult to sustain for an appreciable time, and therefore, three-level lasers must be operated in pulsed mode rather than continuously.

As a result of metastability of E2 energy level,there are far more electrons in the E2 than in the E1 level.This is called population inversion as the rate of flow of electrons from E3 to E1 is greater than from E2 to E1.
This is achieved by very intense flashes of light or electrical discharges.

STIMULATED EMISSION:
Now that the electrons are in high energy levels the  stimulated emission must occur.In the process,an incoming photon stimulates an excited atom to give up its stored energy in the form of a photon that is identical in wavelength, direction, polarization, and phase to the stimulus photon.
If the excited atom is unable to produce a photon that matches the incoming photon, then stimulated emission cannot take place.
                                                                                         
As a photon passes through the collection of excited atoms, it can stimulate the generation of many trillions of photons, or more, creating an avalanche of light.

SUSTAINING STIMULATED EMISSION:
Two mirrors at either end of the lasing medium reflect these photons facilitating the light gain.The active medium can thus be regarded as an amplifier that takes in a small signal (one photon, say) and delivers a large signal (many photons, all identical to the first) at the output.


ASSEMBLY OF MIRRORS .ONE IS PARTIALLY AND THE OTHER FULLY SILVERED.
Monochromatic, single-phase, columnated light leaves the laser through the half-silvered mirror -- laser light!


PONT PHYSIQUE 

bridge circuit is a type of electrical circuit in which two circuit branches (usually in parallel with each other) are "bridged" by a third branch connected between the first two branches at some intermediate point along them

Wheatstone Bridge
The Wheatstone bridge is an electrical circuit for the precise comparison of resistances.It was invented by Samuel Hunter Christie in 1833 and improved and popularized by Sir Charles Wheatstone

CONSTRUCTION:


The Wheatstone bridge is an electrical bridge circuit used to measure resistance. It consists of

  1. a common source of electrical current (such as a battery) 
  2. a galvanometer that connects two parallel branches, containing four resistors,of which two are known R_1and R_3.One of the parallel branches contains one adjustable resistor R_2 and an unknown R_X.

 WORKING:

BALANCING THE BRIDGE:


If the bridge is unbalanced, the direction of the current indicates whether R_2 is too high or too low. R_2 is varied until there is no current through the galvanometer, which then reads zero.

If the ratio of the two resistances in the known leg (R_2 / R_1) is equal to the ratio of the two in the unknown leg (R_x / R_3), then the voltage between the two midpoints (B and D) will be zero and no current will flow through the galvanometer V_g.Such a bridge is called BALANCED.

Detecting zero current with a galvanometer can be done to extremely high accuracy. Therefore, if R_1, R_2 and R_3 are known to high precision, then R_x can be measured to high precision. Very small changes in R_x disrupt the balance and are readily detected.

At the point of balance, the ratio of R1 to R2 is equal to R3 and R4.

METER BRIDGE
It consists of a meter long wire of high resistance and low temperature co-efficient.

CONSTRUCTION:


  • It consists of a wire AB of 1 meter length and uniform cross section.
  • A battery of emf ' e ' , a plug key 'K' are connected between the two terminals A and B.
  • A graduated meter scale S is fixed by the side of the wire for taking the lengths of the wire from the +ve terminal i.e A. 
  • Three strips C1 ,C2 ,C3 of copper or bronze with negligible resistances are also stretched on the board with gaps in between them. 

  • A resistance box 'RB' is connected in the gap 'G1' . Resistance in RB = P 
  • The unknown resistance 'X' is connected in gap 'G2' .
  • In between the centre C of strip C2 , a galvanometer G and a high resistance 'H.R' are connected in series . 

The other end of the galvanometer is connected to a ‘jockey’ which is essentially a metallic rod whose one end has a knife-edge which can slide over the wire to make electrical connection.


  • When the jockey is at a point 'D' on the wire , it divides the wire into two parts AD and DB of lengths L1 and L2.
  • Resistance of AD length of wire =R = L1 [sigma] 
  • Resistance of DB length of wire = S = L2 [sigma]  

where [sigma] is the resistance per unit length of the wire.

Now , the circuit is exactly similar to a Wheatstone bridge.

WORKING:

The jockey is now pressed at various points one the wire from 'A' to towards 'B' , until we get near null deflection in the galvanometer . 

At this stage , the high resistance is shunted and the exact balance point giving null deflection at D is obtained . 

CALCULATIONS:

The length l1 from A to D is noted . The unknown resistance X can be calculated from the following equation.
When the bridge is balanced , we have

     [(P)/(X)]   =  [(R)/(S)]   =  [(l1)/(l2)]

But in a meter bridge l2 = ( 100 - l1 ) . So the balanced condition of a meter bridge is

[(P)/(X)]   =  [(l1)/(100-l1)]

USES:

The meter bridge can be conveniently used to

  •  determine an unknown resistance
  •     compare two resistance
  •     determine the specific resistance of the material of a wire .