first law for a control volume p m v subbarao professor mechanical engineering department modeling...
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First Law for A Control Volume
P M V SubbaraoProfessor
Mechanical Engineering Department
Modeling of True Engineering Systems…..
Laws of Nature for A Control Mass
Conservation of Mass : constantCMm
Conservation of Momentum : tFVmVm CMCMCMCM
12
First law of thermodynamics :212112 WQEE CMCM
Rate Equations for Laws of Nature for A Control Mass
Conservation of Mass : 0dt
dmCM
Conservation of Momentum :
Fdt
Vmd CMCM
First law of thermodynamics : WQdt
dECM
CM & CV Representation of a Device
• Control Mass representation of Can:
• The total Deodorant
• Control Volume representation of Can:
• Deodorant in side the can
• At time t = 0, (before spray).
• The total mass of Deodorant =Mass of Deodorant in side the can
• Control mass is same as control volume
CM & CV Representation of a Device
• At t = t (after spraying)
• Control mass = control volume + spray
• It is possible to relate CM and CV of a device at any instant!
• Principle of Conservation mass says that the rate of change of mass for a control mass is always zero.
• What about control volume?
The Thermodynamic Control Volume
• In real engineering devices, we are usually interested in a region of space, i.e, control volume and not particular control mass.
• The laws of nature are connected to Control Mass.
• Therefore, we need to transform Laws of Conservation for a control mass to a control volume.
• This is accomplished through the use of Reynolds Transport Theorem.
• Specially derived in thermodynamics for CV .
Flowing Fluid Through A CV
• A typical control volume for flow in an funnel-shaped pipe is bounded by the pipe wall and the broken lines.
• At time t0, all the fluid (control mass) is inside the control volume.
The control volume at time t0+t .
There will be differences between the fluid (control mass) and the control volume at time t0 +t .
The control mass at time t0 +t .
I
II
• Consider a control mass and a control volume (C.V.) as follows:
• the control mass occupies region I and C.V. (region II) at time t0.
• Fluid particles of region – I are trying to enter C.V. (II) at time t0.
II
III
• the same control mass occupies regions (II+III) at t0 + t
• Fluid particles of I will enter CV-II in a time t.
•Few more fluid particles which belong to CV – II at t0 will occupy III at time t0 + t.
A Generalized Functional Model for CV
The control volume may move as time passes.I
II
At time t0
II
III At time t0+t
CVV
I is trying to enter CV at time t0
III has left CV at time t0+t
Reynolds' Transport Theorem
For and infinitesimal time duration
• The rate of change of property B of the system.
t
B
t
B
t
BB
t
B tI
ot
ttIII
ot
tCVttCV
ot
CM
ot
0000 limlimlimlim
IIIICVCM BB
dt
dB
dt
dB
The above mentioned change has occurred over a time t, thereforeTime averaged change in any general property of a control mass, BCM is
t
B
t
B
t
BB
t
B tIttIIItCVttCVCM
0000
A Simple Accounting !!!
Conservation of Mass
• Let B = mass of the system, m.
inoutCVCM mm
dt
dm
dt
dm
The rate of change of mass in a control mass should be zero.
0 inoutCV mm
dt
dm
Conservation of Momentum
• Let B = momentum of the system, mV.
inoutCVCM VmVm
dt
Vmd
dt
Vmd
The rate of change of momentum for a control mass should be equal to resultant external force.
FVmVmdt
Vmdinout
CV
First Law of Thermodynamics
• Let B = E, Energy of the system, me.
inoutCVCM mm
dt
med
dt
med
The rate of change of energy of a control mass should be equal to difference of work and heat transfer rates.
WQmmdt
medinout
CV
Rate Equations for Laws of Nature : Control Mass
Conservation of Mass : 0dt
dmCM
Conservation of Momentum :
Fdt
Vmd CMCM
First law of thermodynamics : WQdt
dECM
First Law for A Control Volume
• Conservation of mass:
0 inoutCV mm
dt
dm
• Conservation of energy:
WQdt
dEinout
CV
Wdt
dEQ out
CVin
FVmVmdt
Vmdinout
CV
• Conservation of momentum:
More Mathematical Definitions for A CV
V
CV dVm V
CV dVeE
inletinlet A
in
A
in AdVAdVm
..
outletoutlet A
out
A
out AdVAdVm
..
inletinlet A
inin
A
ininin AdVAdVm
..
inletoutlet A
outout
A
outoutout AdVAdVm
..
Thermodynamic Nature of Variables of CV
• Incoming and outgoing mass flow rates are steady.• Properties of incoming and outgoing flows are
homogeneous and invariant.• Properties of CV can be inhomogeneous and variant.• Following features for CV are possible.• Inhomogeneous and variant : Difficult to solve using
thermodynamics.• Homogeneous and invariant : A trivial situation for a CV.
No heat or work interactions required.• Inhomogeneous and invariant: Steady State System. • Rate of work and heat interactions must be invariant too.• Homogeneous and variant: Transient System. • Rate of work and heat interactions are variant.
First Law for CV:Steady State Steady Flow
• Conservation of mass:
00 inoutCV mm
dt
dm
• Conservation of energy:
Wdt
dEQ out
CVin
Properties of CV are Invariant:
WQdt
dEoutin
CV 0
NO accumulation or depletion of mass of a CV.
NO addition or removal of energy for a CV.
Rate of Work and Heat Transfers : SSSF
Both rate of heat transfer and rate of work transfer are invariant.
The work done per unit mass and heat transfer per unit mass are invariant.
The specific work transfer at various parts of a CV can be different.
The specific heat transfer at various parts of a CV can be different.
CVCV wmW
Let : mmm outin
CVCV qmQ
Complex Engineering Control Volume : SSSF
CV
out
out
in
inCV WgzV
hmgzV
hmQ
22
22
SSSF: Conservation of mass
outin mm
First Law :
CVoutoutininCV WmmQ
Comparison of A control mass and SSSF CV during a change of state
Consider compression processes using CM and CV devices.
Reciprocating compressor : A Control Mass : mCM
Initial State : p1,v1 and T1. Final State : p2,v2 and T2.
constant21
12
CMm
vv
pp
Centrifugal compressor : A Control Volume @SSSF
mmm outin
m mInlet State : pin,vin and Tin.
Outlet State : pout,vout and Tout.
constant
CV
outin
inout
m
vv
pp
Various parts of A CV are at different states during SSSF process !!
Salient Features of CV @SSSF Process
• Rate of mass inflow = Rate mass outflow.• Work done per unit mass is invariant.• Heat transfer per unit mass is invariant.• Change of state or process is not for the CV!• The incoming fluid changes its state from inlet to exit
conditions.• A CM possesses different states at different time intervals.• A CV possesses All states at any time but at different
spatial locations.• A CV with SSSF process is an inhomogeneous device.• A CV can work continuously without changing its state.• A CV lowers the importance of time !