1. Please read:
7 tips to solve physics faster in MHT-CET
September 19, 2010 By Prof. Rohan Shenoy40 Comments
1. Play chess or any other mild puzzle for improving basic logical, analytic and reasoning skills.
2. By-heart logarithm tables of common nos (Ex: 0 – 9) for faster calculation.
3. Wherever you are dealing with fractional nos, always eliminate the decimal and spin it into a
power of 10. Example: (5.1/17) should be solved as [(51/17)*10-1]. Eliminating fractions will
improve the accuracy exponentially. In MHT-CET physics paper, many times the only
difference in options is their decimal place. Ex: a) 1.3 b) 0.13 c) 0.013 d) 0.0013
4. Learn inter-conversion of units in various systems such as MKS and CGS.
5. While solving numerical MCQs from any book, such as P.S. Bangui, start solving from the last
question to first question, i.e in reverse order. The difficult questions are usually given in the
last. If reverse order is too difficult, you can solve alternate questions in serial order.
6. Use common sense, and do not be nervous or anxious while approaching questions. Most of
the questions are straight forward formula based. Students blow it up because they are weak
on calculation parts, or are not prepared fully.
7. Instead of “reading” formulas, practice them in the form of numericals. This will give dual
benefit of learning the formula as well math speed.
For your information:
Atleast 45 out of 50 questions in physics paper are numerical questions. It is foolish on the
part of any student to appear for CET without having practiced numeric
a personal appeal from
Wikipedia founder Jimmy Wales Read now
Laws of thermodynamicsFrom Wikipedia, the free encyclopediaJump to: navigation, search
Thermodynamics
The classical Carnot heat engine
Branches[show]Classical · Statistical · Chemical
Equilibrium / Non-equilibrium

2. Laws[hide]Zeroth · First · Second · Third
Systems[show]State:
Equation of state
Ideal gas · Real gas
Phase of matter · Equilibrium
Control volume · Instruments
--------------------------------------------------------------------------------
Processes:
Isobaric · Isochoric · Isothermal
Adiabatic · Isentropic · Isenthalpic
Quasistatic · Polytropic
Free expansion
Reversibility · Irreversibility
Endoreversibility
--------------------------------------------------------------------------------
Cycles:
Heat engines · Heat pumps
Thermal efficiency
System properties[show]Property diagrams
Intensive and extensive properties
--------------------------------------------------------------------------------
Functions of state:
Temperature / Entropy (intro.) †
Pressure / Volume †
Chemical potential / Particle no. †

3. († Conjugate variables)
Vapor quality
Reduced properties
--------------------------------------------------------------------------------
Process functions:
Work · Heat
Material properties[show]Specific heat capacity
Compressibility
Thermal expansion
Property database
Equations[show]Carnot's theorem · Clausius theorem · Fundamental relation · Ideal gas law · Maxwell
relations · Onsager reciprocal relations
--------------------------------------------------------------------------------
Table of thermodynamic equations
Potentials[show]Free energy · Free entropy
--------------------------------------------------------------------------------
Internal energy
Enthalpy
Helmholtz free energy
Gibbs free energy

4. History and culture[show]Philosophy:
Entropy and time · Entropy and life
Brownian ratchet
Maxwell's demon
Heat death paradox
Loschmidt's paradox
Synergetics
--------------------------------------------------------------------------------
History:
General · Heat · Entropy · Gas laws
Perpetual motion
Theories:
Caloric theory · Vis viva
Theory of heat
Mechanical equivalent of heat
Motive power
Publications:
"An Experimental Enquiry Concerning ... Heat"
"On the Equilibrium of Heterogeneous Substances"
"Reflections on the
Motive Power of Fire"
--------------------------------------------------------------------------------
Timelines of:
Thermodynamics · Heat engines

5. --------------------------------------------------------------------------------
Art:
Maxwell's thermodynamic surface
--------------------------------------------------------------------------------
Education:
Entropy as energy dispersal
Scientists[show]Bernoulli · Carnot · Clapeyron · Clausius · von Helmholtz · Carathéodory · Pierre
Duhem · Gibbs · Joule · Maxwell · von Mayer · Onsager · Rankine · Smeaton · Stahl · Thompson · Kelvin
· Waterson
v ·t ·e
The four laws of thermodynamics define fundamental physical quantities (temperature, energy, and
entropy) that characterize thermodynamic systems. The laws describe how these quantities behave
under various circumstances, and forbid certain phenomena (such as perpetual motion).
The four laws of thermodynamics are:[1][2][3][4][5][6]
Zeroth law of thermodynamics: If two systems are in thermal equilibrium with a third system, they
must be in thermal equilibrium with each other. This law helps define the notion of temperature.
First law of thermodynamics: Heat and work are forms of energy transfer. Energy is invariably
conserved but the internal energy of a closed system changes as heat and work are transferred in or
out of it. Equivalently, perpetual motion machines of the first kind are impossible.
Second law of thermodynamics: The entropy of any isolated system not in thermal equilibrium almost
always increases. Isolated systems spontaneously evolve towards thermal equilibrium—the state of
maximum entropy of the system—in a process known as "thermalization". Equivalently, perpetual
motion machines of the second kind are impossible.
Third law of thermodynamics: The entropy of a system approaches a constant value as the
temperature approaches zero. The entropy of a system at absolute zero is typically zero, and in all
cases is determined only by the number of different ground states it has. Specifically, the entropy of a
pure crystalline substance at absolute zero temperature is zero.

6. Classical thermodynamics describes the exchange of work and heat between systems. It has a special
interest in systems that are individually in states of thermodynamic equilibrium. Thermodynamic
equilibrium is a condition of systems which are adequately described by only macroscopic variables.
Every physical system, however, when microscopically examined, shows apparently random
microscopic statistical fluctuations in its thermodynamic variables of state (entropy, temperature,
pressure, etc.). These microscopic fluctuations are negligible for systems which are nearly in
thermodynamic equilibrium and which are only macroscopically examined. They become important,
however, for systems which are nearly in thermodynamic equilibrium when they are microscopically
examined, and, exceptionally, for macroscopically examined systems that are in critical states[7], and
for macroscopically examined systems that are far from thermodynamic equilibrium.
There have been suggestions of additional laws, but none of them achieve the generality of the four
accepted laws, and they are not mentioned in standard textbooks.[1][2][3][4][5][8][9]
The laws of thermodynamics are important fundamental laws in physics and they are applicable in
other natural sciences.
Contents [hide]
1 Zeroth law
2 First law
3 Second law
4 Third law
5 History
6 See also
7 References
8 Further reading
[edit] Zeroth lawThe zeroth law of thermodynamics may be stated as follows:

7. If system A and system B are individually in thermal equilibrium with system C, then system A is in
thermal equilibrium with system B
The zeroth law implies that thermal equilibrium, viewed as a binary relation, is a Euclidean relation. If
we assume that the binary relationship is also reflexive, then it follows that thermal equilibrium is an
equivalence relation. Equivalence relations are also transitive and symmetric. The symmetric
relationship allows one to speak of two systems being "in thermal equilibrium with each other",
which gives rise to a simpler statement of the zeroth law:
If two systems are in thermal equilibrium with a third, they are in thermal equilibrium with each other
However, this statement requires the implicit assumption of both symmetry and reflexivity, rather
than reflexivity alone.
The law is also a statement about measurability. To this effect the law allows the establishment of an
empirical parameter, the temperature, as a property of a system such that systems in equilibrium
with each other have the same temperature. The notion of transitivity permits a system, for example
a gas thermometer, to be used as a device to measure the temperature of another system.
Although the concept of thermodynamic equilibrium is fundamental to thermodynamics and was
clearly stated in the nineteenth century, the desire to label its statement explicitly as a law was not
widely felt until Fowler and Planck stated it in the 1930s, long after the first, second, and third law
were already widely understood and recognized. Hence it was numbered the zeroth law. The
importance of the law as a foundation to the earlier laws is that it allows the definition of
temperature in a non-circular way without reference to entropy, its conjugate variable.
[edit] First lawThe first law of thermodynamics may be stated thus:
Increase in internal energy of a body = heat supplied to the body - work done by the body. U = Q - W
For a thermodynamic cycle, the net heat supplied to the system equals the net work done by the
system.
More specifically, the First Law encompasses several principles:

8. The law of conservation of energy.
This states that energy can be neither created nor destroyed. However, energy can change forms, and
energy can flow from one place to another. The total energy of an isolated system remains the same.
The concept of internal energy and its relationship to temperature.
If a system, for example a rock, has a definite temperature, then its total energy has three
distinguishable components. If the rock is flying through the air, it has kinetic energy. If it is high
above the ground, it has gravitational potential energy. In addition to these, it has internal energy
which is the sum of the kinetic energy of vibrations of the atoms in the rock, and other sorts of
microscopic motion, and of the potential energy of interactions between the atoms within the rock.
Other things being equal, the internal energy increases as the rock's temperature increases. The
concept of internal energy is the characteristic distinguishing feature of the first law of
thermodynamics.
The flow of heat is a form of energy transfer.
In other words, a quantity of heat that flows from a hot body to a cold one can be expressed as an
amount of energy being transferred from the hot body to the cold one.
Performing work is a form of energy transfer.
For example, when a machine lifts a heavy object upwards, some energy is transferred from the
machine to the object. The object acquires its energy in the form of gravitational potential energy in
this example.
Combining these principles leads to one traditional statement of the first law of thermodynamics: it is
not possible to constuct a perpetual motion machine which will continuously do work without
consuming energy.
[edit] Second lawThe second law of thermodynamics asserts the existence of a quantity called the
entropy of a system and further states that
When two isolated systems in separate but nearby regions of space, each in thermodynamic
equilibrium in itself (but not necessarily in equilibrium with each other at first) are at some time
allowed to interact, breaking the isolation that separates the two systems, allowing them to exchange
matter or energy, they will eventually reach a mutual thermodynamic equilibrium. The sum of the
entropies of the initial, isolated systems is less than or equal to the entropy of the final combination
of exchanging systems. In the process of reaching a new thermodynamic equilibrium, total entropy
has increased, or at least has not decreased.

9. It follows that the entropy of an isolated macroscopic system never decreases. The second law states
that spontaneous natural processes increase entropy overall, or in another formulation that heat can
spontaneously be conducted or radiated only from a higher-temperature region to a lower-
temperature region, but not the other way around.
The second law refers to a wide variety of processes, reversible and irreversible. Its main import is to
tell about irreversibility.
The prime example of irreversibility is in the transfer of heat by conduction or radiation. It was known
long before the discovery of the notion of entropy that when two bodies of different temperatures
are connected with each other by purely thermal connection, conductive or radiative, then heat
always flows from the hotter body to the colder one. This fact is part of the basic idea of heat, and is
related also to the so-called zeroth law, though the textbooks' statements of the zeroth law are
usually reticent about that, because they have been influenced by Carathéodory's basing his
axiomatics on the law of conservation of energy and trying to make heat seem a theoretically
derivative concept instead of an axiomatically accepted one. Šilahvý (1997) notes that Carathéodory's
approach does not work for the description of irreversible processes that involve both heat
conduction and conversion of kinetic energy into internal energy by viscosity (which is another prime
example of irreversibility), because "the mechanical power and the rate of heating are not expressible
as differential forms in the 'external parameters'".[10]
The second law tells also about kinds of irreversibility other than heat transfer, and the notion of
entropy is needed to provide that wider scope of the law.
According to the second law of thermodynamics, in a reversible heat transfer, an element of heat
transferred, δQ, is the product of the temperature (T), both of the system and of the sources or
destination of the heat, with the increment (dS) of the system's conjugate variable, its entropy (S)
[1]
The second law defines entropy, which may be viewed not only as a macroscopic variable of classical
thermodynamics, but may also be viewed as a measure of deficiency of physical information about
the microscopic details of the motion and configuration of the system, given only predictable
experimental reproducibility of bulk or macroscopic behavior as specified by macroscopic variables
that allow the distinction to be made between heat and work. More exactly, the law asserts that for

10. two given macroscopically specified states of a system, there is a quantity called the difference of
entropy between them. The entropy difference tells how much additional microscopic physical
information is needed to specify one of the macroscopically specified states, given the macroscopic
specification of the other , which is often a conveniently chosen reference state. It is often convenient
to presuppose the reference state and not to explicitly state it. A final condition of a natural process
always contains microscopically specifiable effects which are not fully and exactly predictable from
the macroscopic specification of the initial condition of the process. This is why entropy increases in
natural processes. The entropy increase tells how much extra microscopic information is needed to
tell the final macroscopically specified state from the initial macroscopically specified state.[11]
[edit] Third lawThe third law of thermodynamics is sometimes stated as follows:
The entropy of a perfect crystal at absolute zero is exactly equal to zero.
At zero temperature the system must be in a state with the minimum thermal energy. This statement
holds true if the perfect crystal has only one state with minimum energy. Entropy is related to the
number of possible microstates according to S = kBln(Ω), where S is the entropy of the system, kB
Boltzmann's constant, and Ω the number of microstates (e.g. possible configurations of atoms). At
absolute zero there is only 1 microstate possible (Ω=1) and ln(1) = 0.
A more general form of the third law that applies to systems such as glasses that may have more than
one minimum energy state:
The entropy of a system approaches a constant value as the temperature approaches zero.
The constant value (not necessarily zero) is called the residual entropy of the system.
[edit] HistorySee also: Philosophy of thermal and statistical physics
Count Rumford (born Benjamin Thompson) showed, about 1797, that mechanical action can generate
indefinitely large amounts of heat, so challenging the caloric theory. The historically first established
thermodynamic principle which eventually became the second law of thermodynamics was
formulated by Sadi Carnot during 1824. By 1860, as formalized in the works of those such as Rudolf
Clausius and William Thomson, two established principles of thermodynamics had evolved, the first
principle and the second principle, later restated as thermodynamic laws. By 1873, for example,
thermodynamicist Josiah Willard Gibbs, in his memoir Graphical Methods in the Thermodynamics of

11. Fluids, clearly stated the first two absolute laws of thermodynamics. Some textbooks throughout the
20th century have numbered the laws differently. In some fields removed from chemistry, the second
law was considered to deal with the efficiency of heat engines only, whereas what was called the
third law dealt with entropy increases. Directly defining zero points for entropy calculations was not
considered to be a law. Gradually, this separation was combined into the second law and the modern
third law was widely adopted.
Date: 21 Feb 2013 (Thursday)
Paper: (Marathi / Gujarati / Kannada / Sindi / Malyalam / Tamil / Telugu / Punjabi / Bengali
Time: 11.00 am to 2.00 pm
Date: 22 Feb 2013 (Friday)
Paper: Hindi
Time: 11.00 am to 2.00 pm
Paper: German / Andhramagadhi / Persian
Time: 3.00 am to 6.00 pm
Date: 23 Feb 2013 (Saturday)
Paper: English
Time: 11.00 am to 2.00 pm
Date: 25 Feb 2013 (Monday)
Paper: Physics
Time: 11.00 am to 2.00 pm
Date: 27 Feb 2013 (Wednesday)

12. Paper: Chemistry
Time: 11.00 am to 2.00 pm
Date: 1 March 2013 (Friday)
Paper: Mathematics & Statistics Paper
Time: 11.00 am to 2.00 pm
Date: 4 March 2013 (Monday)
Paper: Biology
Time: 11.00 am to 2.00 pm
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13. Home>Time Table -
Maharashtra Board HSC Time Table
Maharashtra Board HSC Time Table 2013, Maharashtra
HSC Time Table 2013: -
The MSBSHSE is a state education board of Maharashtra state. The MSBSHSE board is known
as the Maharashtra State Board of Secondary and Higher Secondary Education. The board is
providing education facilities to the students of Maharashtra state. The MSBSHSE board was
established on the 1st January of 1966 year. The MSBSHE board was established under the act of
the Legislative Assembly of Maharashtra education board. The main headquarters of the board is
the Pune district of the Maharashtra state. Some other offices are also located in the Mumbai,
Nagpur districts. The board is providing education in the local state language and in the English
language.
Maharashtra Board HSC Time Table 2013:-
The board is providing higher secondary education in different subjects in the different
departments. Mainly board is providing higher secondary education in the science, arts and
commerce stream with different combinations of subjects. The MSBSHSE board is conducting
exams at the end of every annual session. The board conducts class 12th board exams in the
march month after the end of the session. The Maharashtra Board HSC Time Table is very
important for all the appearing students in the 12th class examination.
The board exams of class 12th are important for the students and for this education board. The
students work hard in the class 12th from the start of the session to get a good percentage of
marks. The Maharashtra board announced Maharashtra Board HSC Time Table 2013 mention
as below: -
FIRST HALF SECOND HALF
SUBJECT WITH INDEX SUBJECT WITH
DATE/DAY TIME TIME
NUMBER INDEX NUMBER
Marathi (02)
Thursday Gujarati (03) Urdu (05) French (13)
Kannada (06) Pali (35)
3:00 pm
21st 11:00 am to Tamil (09)
to 6:00
February, 2:00 pm Telugu (10)
pm
Malayalam (08)
2013 Sindhi (07)
Bengali (12)
Punjabi (11)

14. German (14)
Friday
11:00 am to
3:00 pm Ardhamagadhi (16)
22nd 2:00
Hindi (04) to 6:00
February, pm11:00 am
pm Persian (37)
to 1:00 pm
2013
Avesta – Pahalavi (87)
Saturday
11:00 am to
23th English (01)
2:00pm
February,
2013
Secretarial Practice (C) (52)
11:00 am to
2:00 PM
Monday
3:00 pm
11:00 am to Political Science (A)
25th Physics (S) (54) to 6:00
2:00 pm (42)
February, pm
2013
11:00 am to
1:00 pm
Physics Paper 1st (S) (54)
Tuesday 11.00 a.m.
Physics Paper – II (S) (54)
26th to
( For Repeater Candidates
February,
Only)
2013 1.00 p.m.
11.00 a.m.
to Book Keeping & Accountancy
(A/C) (50)
Wednesday 2.00 p.m.
Chemistry (S) (55) 3:00 pm
27th, to 6:00 Philosophy (A) (46)
February Chemistry Paper – I (S) (55) pm
2013 11.00 a.m.
( For Repeater Candidates
to Only)
1.00 p.m.
Thursday
Chemistry Paper – II (S) (55)
11:00 am to
28th
1:00 pm ( For Repeater Candidates
February,
Only)
2013
Friday 11:00 am to Mathematics & Statistics Paper 3:00 pm Sociology (A/S) (45)

15. 2:00 pm (A/S) (40) to 6:00
01st March, pm
2013
11.00 a.m. Mathematics & Statistics
paper-I (A/S) (40)
to
( For Repeater Candidates
1.00 p.m. Only)
Mathematics & Statistics Paper
– I (C) (88)
Mathematics &
Statistics Paper – II
(A/S) (40)
3.00 p.m.
Saturday
( For Repeater
to
02nd March, Candidates Only)
2013
5.00 p.m.
Mathematics &
Statistics Paper – II
(C) (88)
11.00 a.m.
Biology (S) (56)
to
2. 00 p.m. 3.00 p.m.
Monday
Economics (A/S/C)
to
04th March, (49)
2013 Biology Paper – I (S) (56)
11.00 a.m. 6.00 p.m.
( For Repeater Candidates
to
Only)
1. 00 p.m.
Tuesday 11.00 a.m. Biology Paper – II (S) (56)
05th March, to ( For Repeater Candidates
2013 Only)
1.00 p.m.
Wednesday 11.00 a.m. Organisation of Commerce & 3.00 p.m. History (A) (38)
06th March, to Management (C) (51) to
2013
2.00 p.m. 6.00 p.m.

16. Friday VOCATIONAL COURSES- 3.00 p.m. Education (A/S) (78)
PAPER – I
08th March, to
2013 (TECHNICAL GROUP)
11:00 am to 6.00 p.m.
2:00 pm General Civil Engineering (A4)
——————
11.00 a.m. Electrical Maintenance (A1)
to Mechanical Maintenance (A2)
1.30 p.m. Scooter and Motor Cycle
Servicing (A3)
Electronics (C2)
11.00 a.m.
Computer Science (D9)
to
2.00 p.m.
COMMERCE GROUP PAPER
–I
Banking (A5) Office
Management (A7) Marketing
11.00 a.m. & Salesmanship (A8) Small
Industries & Self Employment
to (A9)
2.00 p.m.
FISHERY GROUP PAPER – I
Fish Processing Technology
(B9) Fresh Water Fish Culture
11.00 a.m. (C1)
to
2.00 p.m AGRICULTURAL GROUP
PAPER – I

17. Animal Science & Dairying
(B2), Crop Science (B4),
Horticulture (B5)
11.00 a.m.
to
2.00 p.m
Monday VOCATIONAL COURSES- 3.00 p.m. OCCUPATIONAL
PAPER – II ORIENTATION
11th March, to
2013 (TECHNICAL GROUP) Library & Information
11:00 am to 5.00 p.m. Science (A/C) (85)
2:00 pm General Civil Engineering (A4)
——————
3.00 p.m. Historical &
11:00 am to Electrical Maintenance (A1) Development of
1:30 pm to
Mechanical Maintenance (A2) Indian classical Dance
6.00 p.m. (A) (91)
Scooter and Motor Cycle
Servicing (A3)
11:00 am to Electronics (C2)
2:00 pm
Computer Science (D9)
COMMERCE GROUP PAPER
11:00 am to – II
2:00 pm
Banking (A5) Office
Management (A7) Marketing
& Salesmanship (A8) Small
Industries & Self Employment
(A9)
11:00 am to
2:00 pm FISHERY GROUP PAPER –

18. II
Fish Processing Technology
(B9) Fresh Water Fish Culture
11:00 am to (C1)
1:00 pm
AGRICULTURAL GROUP
PAPER – II
Animal Science & Dairying
(B2), Crop Science (B4),
Horticulture (B5)
3.00 p.m.
Wednesday
to Logic (A) (47)
12th March,
2013
6.00 p.m.
11.00 a.m.
Wednesday
to Co-operation (A/C) (53)
13th March,
2013
2.00 p.m.
3.00p.m.
to
European Music (A)
11.00 a.m.
Friday (73)
4.00p.m
to Geography (A/S/C) (39)
15th
3.00p.m.
March,2013
2.00 p.m.
Japanese (21)
to
6.00p.m
Russian (20) Child Development
11.00 a.m. 3.00 p.m.
(A/S) (43)
Sanskrit (33)
to to
Saturday
Arabic (36)
2.00 p.m. 5.30 p.m.
Agriculture Science &
16th
Technology
March,2013
General Knowledge (32) Paper-I (75), Animal
11.00 a.m. 3.00 p.m.
Science & Technology
(For Military School’s only)

19. to to Paper-I (76)
2.00 p.m 5.00 p.m.
11.00 a.m. 3.00 p.m.
Agriculture Science &
Geology Paper – I (S) (41)
Technology
to to
Paper-II (75), Animal
1.00 p.m. 5.00 p.m.
Monday Science & Technology
18th Paper-II (76)
History & Appreciation of Arts
march,2013
11.00 a.m. (A) 3.00 p.m.
to (Painting, Sculpture & to
Defense Studies
Architecture) (60)
(A/S/C) (77)
2.00 p.m. 5.30 p.m.
11.00 a.m.
Tuesday
to Textile (A/S) (44)
19th
march,2013
1.30 p.m.
3.00p.m
to
Geology Paper – II (S)
11.00 a.m.
Wednesday (41)
5.00p.m.
to Psychology (A/S) (48)
20th
3.00p.m
march,2013
2.00 p.m.
Percussion (A) (69)
to
5.30p.m.
11.00 a.m. 3.00p.m
Thursday
History & Development of
to to English Literature (22)
21 nd
Indian Music (A) (65)
March,2013
2.00 p.m. 6.00p.m.
Information Technology
Information
11.00 a.m. 3.00 p.m. Technology
Friday (Online Examination)
to to (Online Examination)
22nd Science (97)
march,2013
1.30 p.m. 5.30 p.m. Science (97)
Arts (98)

20. Commerce (99) Arts (98)
Commerce (99)
Information
Information Technology
Technology
11.00 a.m. (Online Examination) 3.00 p.m.
Saturday (Online Examination)
to Science (97) to
23rd Science (97)
March,2013
1.30 p.m. Arts (98) 5.30 p.m.
Arts (98)
Commerce (99)
Commerce (99)
Information
Information Technology
Technology
11.00 a.m. (Online Examination) 3.00 p.m.
Monday (Online Examination)
to Science (97) to
25th Science (97)
March,2013
1.30 p.m. Arts (98) 5.30 p.m.
Arts (98)
Commerce (99)
Commerce (99)
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Durex
Home>Electronics> Home Appliances > Washing Machines > Semi Automatic > Videocon Semi
Automatic Washing Machine 6.5 kg Kyle
Videocon Semi Automatic Washing Machine 6.5 kg Kyle
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41. Price: 7400
Buy At: 6660
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About Videocon Semi Automatic Washing Machine 6.5 kg Kyle
| Create your review

42. Water fall gives better circulation of water , and better dispersion of detergent , providing better wash
Videocon Semi Automatic Washing Machine 6.5 kg Kyle Details
Brand Videocon See All Videocon Products
Category Semi Automatic
body : Pp
pulsator Type : Normal
wash Timer (in Min) : 15
spin Time (in Min) : 5
knob : Normal
water Inlet : 1
waterfall/ Cascade : Yes
Other features
castor : Yes
water Level : 3
lint Collector : Magic Filter
spin Shower : Yes
wash Window : Transparent
spin Window : Transparent
spin Motor (w) : 180
Warranty 1 Year Videocon India Warranty
Active Soak
Convenience features
Yes
Wxdxh
Dimensions
795 X 460 X 900
No Of Wash Programs
2
Soft Dry
Washing features Yes
Wash Motor
380
Spin Shower

43. 5
Spin Speed Rpm
Yes
Rust Free Plastic Body
waterfall
Key features spin Shower Rinsing
3 Water Level Indicator
castor
Color
Body
Grey Light
Wash Capacity
General features
6.5 Kg
User Reviews for Videocon Semi Automatic Washing Machine 6.5 kg Kyle
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Videocon Semi Automatic Washing Machine 6.5 kg Kyle
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EMI Calculator
EMI Plan Monthly Instalments Total Cost
3 Months 2220/- 6660/-
6 Months 1110/- 6660/-
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Sold Out Sold Out Sold Out Sold Out
Rs 5999 Rs
Price Rs 4999 Rs 4999 Rs 6190
459023% Off
Sold Out Sold Out Sold Out Sold Out
Availability Dispatched in 2 Dispatched in 2 Dispatched in 2 Dispatched in 2
business days business days business days business days

48. NA NA NA NA
Highlights - Dual SIM (GSM - Dual SIM - Android v2.3.5 - 4 Inch Touch
+ GSM) - Wi-Fi Enabled (Gingerbread) OS Screen
- 1 GHz - 1.2 GHz ARM - 2 MP Primary - Android 4.0 ICS
Qualcomm Cortex-A5 Camera OS
Scorpion Processor - 4.3-inch TFT - Dual SIM
Processor - Android v2.3.5 Capacitive - 3MP Camera
- Android v2.3.5 (Gingerbread) OS Touchscreen
(Gingerbread) OS - Dual SIM
- 3.5-inch
Capacitive
Touchscreen
Technical Specification
GENERAL
FEATURES
Keypad No No No No
Battery, Charger, Battery, Charger, Battery, Charger,
Handset, Battery,
Data Cable, Data Cable, Data Cable,
Charger, Headset,
Handset, Handset, Handset,
In Sales Package USB Cable, User
Headset,User Headset,User Headset,User
Manual, Warranty
Guide, Warranty Guide, Warranty Guide, Warranty
Card
Card Card Card
Form Touch Touch Touch Touch
Dual Dual Dual
SIM Dual SIM
SIM(GSM+GSM) SIM(GSM+GSM) SIM(GSM+GSM)
PLATFORM
Android v2.3.5 Android v2.3.5 Android v2.3.5
OS Android 4.0 ICS
(Gingerbread) (Gingerbread) (Gingerbread)
Java No No No No
1 GHz Qualcomm 1 GHz ARM 1 GHz ARM
Processor 1.0 GHz
Scorpion Cortex-A5 Cortex-A5
Graphics Adreno NA NA N/A
DISPLAY
Type TFT TFT TFT TFT
Size 3.5 Inches 4.3 Inches 4.3 Inches 4 Inches
Resolution N/A N/A N/A N/A
Colors 262 K 262 K 262 K NA
DIMENSIONS
69.7x130x10.95 69.7x130x10.95
Size 62x116x12 mm 124 64 10.6mm
mm mm
Weight 108.96 g 148 g 148 g 113 NA
CAMERA
Primary Camera 3 Megapixel 2 Megapixel 2 Megapixel 3 Megapixel
Secondary
No 0.3 Megapixel 0.3 Megapixel No
Camera
Flash No No No No

49. Video
Yes Yes Yes Yes
Recording
Zoom Yes Yes Yes Yes
BATTERY
Type Li-Ion, 1300 mAh Li-Ion, 1350 mAh Li-Ion, 1350 mAh 1450 mAh
Talktime N/A N/A N/A Up to 4hrs
Standby Time 170 hrs (2G) 205 hrs (2G) 205 hrs (2G) Up to 170 hrs
MEMORY
AND
STORAGE
Internal 130 MB 190 MB 190 MB 4GB ROM
microSD, upto 32 microSD, upto 32 microSD, upto 32
External Up to 32GB
GB GB GB
256 MB RAM, 512 2 GB RAM, 4 GB 2 GB RAM, 4 GB
Memory 512MB RAM
MB ROM ROM ROM
INTERNET &
CONNECTIVI
TY
Yes, 7.2 Mbps
3G HSDPA,5.76 Mbps No No Yes
HSUPA
Wifi Yes, 802.11 b/g/n Yes, 802.11 b/g/n Yes, 802.11 b/g/n Yes
GPRS Yes, Class 10 Yes, Class 12 Yes, Class 12 Yes
Bluetooth Yes Yes Yes Yes
USB
Yes Yes Yes Yes
connectivity
MULTIMEDIA
Music Player Yes Yes Yes Yes
Video Player Yes Yes Yes Yes
Ringtone 128 Polyphonic MP3, WAV MP3, WAV MP3, WAV
FM Yes Yes Yes Yes
Audio Jack 3.5 mm 3.5 mm 3.5 mm 3.5 mm
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