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The latest Messages 4
2021-08-21 21:49:58
JEE Main 2021 Session 4 admit card released Check now jeemain.nta.nic.in
@physicswallah8
10.8K viewsedited 18:49
2021-08-21 21:23:48
Exceptions of Conclusions of Mendel
Incomplete Dominance
(1) When neither of the alleles of a character is completely dominant over the other and the F1 hybrid is intermediate between the two parents, the phenomenon is called incomplete dominance.
(2) Incomplete dominance was first discovered by Correns in Mirabilis jalapa. The plant is called as 4’O clock plant or ‘Gul-e-Bans’. Homozygous red (RR) flowered variety of the plant was crossed with white (rr) flowered variety. F1 offspring had pink flowers (Rr). This is called incomplete dominance.
(3) Incomplete dominance is also known to occur in snapdragon. The phenotypic ratio and genotypic ratio in F2 generation in case of incomplete dominance is 1:2:1.
Co-dominance
(1) In co-dominance both the gene expressed for a particular character in F1 hybrid progeny. There is no blending of characters, whereas both the characters are expressed equally.
(2) Co-dominance is seen in animals for coat colour. When a black parent is crossed with white parent, a roan color in F1 progeny is produced.
Sex determination
(1) Fixing the sex of an individual as it begins life is called sex determination. The various genetically controlled sex-determination mechanisms have been classified into following categories
(2) Chromosomal theory of sex determination: The X-chromosome was first observed by German biologist, Henking in 1891 during the spermatogenesis in male bug and was described as X-body. The chromosome theory of sex determination was worked out by E.B. Wilson and Stevens (1902-1905).
(3) They named the X and Y chromosomes as sex-chromosomes or allosomes and other chromosomes of the cell as autosomes.
(4) Sex chromosomes carry genes for sex. X-chromosomes carries female determining genes and Y-chromosomes has male determining genes.
(5) The number of X and Y chromosomes determines the female or male sex of the individual, Autosomes carry genes for the somatic characters. These do not have any relation with the sex.
Sex Determination by chromosomes:
Those chromosomes which are involved in the determination of sex of an individual are called sex chromosomes while the other chromosomes are called autosomes.
1) XX – XY type: In most insects including fruit fly Drosophila and mammals including human beings the females possess two homomorphic sex chromosomes, named XX. The males contain two heteromorphic sex chromosomes, i.e., XY. Hence the males produce two types of gametes / sperms, either with X-chromosome or with Y-chromosome, so they are called Heterogamety.
2) ZZ – ZW type: In birds and some reptiles, the males are represented as ZZ (homogamety) and females are ZW (heterogamety).
3) XX – XO type: In round worms and some insects, the females have two sex chromosomes, XX, while the males have only one sex chromosomes X. There is no second sex chromosome. Therefore, the males are designated as XO. The females are homogametic because they produce only one type of eggs. The males are heterogametic with half the male gametes carrying X-chromosome while the other half being devoid of it.
11.2K views18:23
2021-08-21 19:39:23
We have prepared a one single video that will help your whole JEE mains & advanced promotions and NEET preparations in just 15 minutes.
11.2K viewsedited 16:39
2021-08-20 12:21:20
Notes on Special Theory of Relativity:-
Frame of reference:- A system of coordinates whose axes can be suitably chosen is said to be a frame of reference.
Inertial frame:- A frame of reference either at rest or moving with a uniform velocity (zero acceleration) is known as inertial frame.
Non-inertial or accelerated frame:- It is a frame of reference which is either having a uniform linear acceleration or is being rotated with a uniform speed.
Galilean transformation:-
(a) Transformation of position:-
x' = x – vt
y' = y
z' = z
t' = t
Inverse transformation,
x = x'+ vt '
y = y'
z = z'
t = t'
(b) Transformation of distance:-
l ' = l
Here, l = x2-x1 is the length of rod as observed in frame S.
Anything which remains unchanged when observed from the two Galilean frames of reference is known as Galilean invariant.
(c) Transformation of velocity:-
u'= u– v
Inverse transformation:- u = u'+ v
(d) Transformation of acceleration:-
a' = a
Thus, the acceleration of body, as observed by two observers siting in two inertial frames, is same. Hence, acceleration is said to be Galilean invariant.
Law of conservation of momentum:-
It states that the total momentum of an isolated system (no external force) always remains constant.
In S frame:- m1u1 + m2u2 = m1v1 + m2v2
In S ' frame:- m1u'1 + m2 u'2 = m1 v'1 + m2 v'2
Thus, the law of conservation of momentum is valid in S ' also, indicating that the law is Galilean invariant.
Ether and velocity of light:- c' = c ±v
Postulates of special theory of relativity:-
(a) The laws of physical phenomenon are same when stated in terms of two systems of reference in uniform translator motion relative to each other.
(b) The velocity of light in vacuum is constant, independent not only of the direction of propagation but also of the relative velocity of the source and the observer.
Lorentz transformation equations:-
x' = [x - vt]/√[1- v2/c2]
y'= y
z'= z
t' = [t – [(v/c 2) x]]/√[1- v2/c2]
Lorentz inverse transformation equations:-
x= [x' + vt] /√[1- v2/c2]
y = y'
z= z'
t= [t' + [(v/c 2) x']]/√[1- v2/c2]
Length contraction:-
l = l0√[1- v2/c2]
So, l
Here, l0 is the proper or original length in S frame and l is the relativistic length in S' frame.
Time Dilation:-
??t = ??t0/√ [1-v2/c2]
So, ?t > ??t0
Here, ??t0 is the proper or original time in S frame and ?t is the relativistic time in S' frame.
?Thus, the time interval as observed by the moving observer appears to be lengthened.
Frequency:- If f 0 is the natural frequency of a process in frame S, then the frequency f as observed from S ' given by,
f = f0√[1- v2/c2]
Relativistic velocity addition theorem:-
ux' = [ux – v]/[1- [(v/c2)ux]]
uy' = [uy√[1- v2/c2]]/[1- [(v/c2)ux]]
uz' = [uz√[1- v2/c2]]/[1- [(v/c2)ux]]
Relativistic variation of mass:-
m= m0/√[1-v2/c2]
Rest mass energy:-
E0 = m0c2
Total energy (Mass-Energy Equivalence):-
E= mc2 = [m0/√[1-v2/c2]] c2
Kinetic energy:-
EK= E - E0 = (m - m0) c2
Here c is the speed of light, m0 is the rest mass and m is the relativistic mass.
Relativistic momentum:-
p= mv
= [m0/√[1-v2/c2]] v
20.4K views09:21
2021-08-20 10:52:43
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17.7K views07:52
2021-08-18 10:34:35
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