EP: Lafz (Audio Jukebox) | Garvit-Priyansh | Full Audio Songs | T-Series
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- Опубликовано: 20 май 2024
- Presenting the EP: Lafz (Audio Jukebox)" by Garvit-Priyansh.
Track List🎶:
Jiya Mera - 00:00
Rasta - 02:45
Baaton Hi Baaton - 05:19
Keh Do Na - 08:36
♪Full Song Available on♪
JioSaavn: bit.ly/3vNVNZd
Spotify: bit.ly/3vHcVzV
Hungama: bit.ly/3PVcgBJ
Apple Music: bit.ly/4cIQ2gd
Gaana: bit.ly/4cSjkc4
Amazon Prime Music: bit.ly/4cMNk9k
Wynk: bit.ly/43U5JNC
RUclips Music: bit.ly/49pgqJ7
Audio Credits:
Song: Jiya Mera
Singers: Garvit Soni, Priyansh Srivastava
Composers: Garvit - Priyansh
Lyricist: Priyansh Srivastava, Yashasvi Chaturvedi
Guitars - Aditya Kulkarni
Atmos Mix and Master - Srijan Mangolu
Music Label: T-Series
Song: Rasta
Singers: Garvit Soni, Priyansh Srivastava
Composers: Garvit - Priyansh
Lyricist: Priyansh Srivastava
Music Label: T-Series
Song: Baaton Hi Baaton
Singers: Garvit Soni, Priyansh Srivastava
Composers: Garvit - Priyansh, Dhairya Mehrotra, Shikhar Sharma
Music Arranged By - Garvit Soni, Dhairya Mehrotra
Lyricist: Priyansh Srivastava, Dhairya Mehrotra, Shikhar Sharma
Backing Vocals - Vidhi Trivedi
Mix Master - Garvit Soni
Music Label: T-Series
Song: Keh Do Na
Singers: Garvit Soni, Priyansh Srivastava
Composers: Garvit - Priyansh
Lyricist: Priyansh Srivastava
Music Label: T-Series
Download Song Beat: bit.ly/3Cjh24R
___________________________________
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Видеоклипы
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Song: Lafz!❤
টি সিরিজ খুব ভালো ভারো গান ছাড়ে ❤1k
"❤"
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Fast Comment....
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233
not be uniform throughout. Similarly, a mixture
of gases undergoing an explosive chemical
reaction (e.g. a mixture of petrol vapour and
air when ignited by a spark) is not an
equilibrium state; again its temperature and
pressure are not uniform [Fig. 11.6(b)].
Eventually, the gas attains a uniform
temperature and pressure and comes to
thermal and mechanical equilibrium with its
surroundings.
Fig. 11.6 (a) The partition in the box is suddenly
removed leading to free expansion of the
gas. (b) A mixture of gases undergoing an
explosive chemical reaction. In both
situations, the gas is not in equilibrium and
cannot be described by state variables.
In short, thermodynamic state variables
describe equilibrium states of systems. The
various state variables are not necessarily
independent. The connection between the state
variables is called the equation of state. For
example, for an ideal gas, the equation of state
is the ideal gas relation
P V = µ R T
For a fixed amount of the gas i.e. given µ, there
are thus, only two independent variables, say P
and V or T and V. The pressure-volume curve
for a fixed temperature is called an isotherm.
Real gases may have more complicated
equations of state.
The thermodynamic state variables are of two
kinds: extensive and intensive. Extensive
variables indicate the ‘size’ of the system.
Intensive variables such as pressure and
temperature do not. To decide which variable is
extensive and which intensive, think of a
relevant system in equilibrium, and imagine that
it is divided into two equal parts. The variables
that remain unchanged for each part are
intensive. The variables whose values get halved
in each part are extensive. It is easily seen, for
example, that internal energy U, volume V, total
mass M are extensive variables. Pressure P,
temperature T, and density ρ are intensive
variables. It is a good practice to check the
consistency of thermodynamic equations using
this classification of variables. For example, in
the equation
∆Q = ∆U + P ∆V
quantities on both sides are extensive*. (The
product of an intensive variable like P and an
extensive quantity ∆V is extensive.)
11.8 THERMODYNAMIC PROCESSES
11.8.1 Quasi-static process
Consider a gas in thermal and mechanical
equilibrium with its surroundings. The pressure
of the gas in that case equals the external
pressure and its temperature is the same as
that of its surroundings. Suppose that the
external pressure is suddenly reduced (say by
lifting the weight on the movable piston in the
container). The piston will accelerate outward.
During the process, the gas passes through
states that are not equilibrium states. The nonequilibrium states do not have well-defined
pressure and temperature. In the same way, if
a finite temperature difference exists between
the gas and its surroundings, there will be a
rapid exchange of heat during which the gas
will pass through non-equilibrium states. In
due course, the gas will settle to an equilibrium
state with well-defined temperature and
pressure equal to those of the surroundings. The
free expansion of a gas in vacuum and a mixture
of gases undergoing an explosive chemical
reaction, mentioned in section 11.7 are also
examples where the system goes through nonequilibrium states.
Non-equilibrium states of a system are difficult
to deal with. It is, therefore, convenient to
imagine an idealised process in which at every
stage the system is an equilibrium state. Such a
* As emphasised earlier, Q is not a state variable. However, ∆Q is clearly proportional to the total mass of
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28 comment ap ka Kitna ha
Kis kis ko song acha laga? 0:18
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