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Transport Phenomena
CONTINUITY EQUATION IN 3
DIMENSIONS:
2
HELLO!
I’m Mujeeb UR Rahman
Chemical Engineering student @Mehran University
of Engineering & Technology Jamshoro, Pakistan.
You can find me at SlideShare @MujeebURRahman38
ResearchGate @Mujeeb UR Rahman, Academia @Mujeeb UR Rahman
Transport Phenomena
3
CONTINUITY EQUATION IN 3
DIMENSIONS:
β€œThe equation based on the principle of conversation of mass.”
A
E
C
D
G
F
H
B
dx
dz
2kg
1kg
1kg
x-axis (u)
y-axis (v)
z-axis (w)
4
β–ͺ Law of conservation of mass
CONTINUITY EQUATION IN 3
DIMENSIONS:
π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“
π‘–π‘›π‘π‘Ÿπ‘’π‘Žπ‘ π‘’
π‘œπ‘“ π‘šπ‘Žπ‘ π‘ 
=
π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“
π‘šπ‘Žπ‘ π‘ 
𝑖𝑛
βˆ’
π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“
π‘šπ‘Žπ‘ π‘ 
π‘œπ‘’π‘‘
Transport Phenomena
Transport Phenomena
5
CONTINUITY EQUATION IN 3
DIMENSIONS:
Direction of x, y, z.
u οƒž inlet velocity components in x direction.
v οƒž inlet velocity components in y direction.
w οƒž inlet velocity components in z direction.
Mass of fluid entering the face +ve face ABCD (inflow) per
second .
π‘š
𝑠
𝐷𝑒𝑛𝑠𝑖𝑑𝑦 𝜌 =
π‘š
𝑉
οƒž π‘š = 𝜌 Γ— 𝑉
π‘š
𝑠
οƒž
𝜌 Γ— 𝑉
𝑠
οƒž
𝜌 Γ— 𝐴 Γ— 𝑙
𝑠
οƒž 𝜌 Γ— π΄π‘Ÿπ‘’π‘Ž π‘œπ‘“ 𝐴𝐡𝐢𝐷 Γ— π‘£π‘’π‘™π‘œπ‘π‘–π‘‘π‘¦ 𝑖𝑛 π‘₯ π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘›
= πœŒπ΄π‘‰ οƒž 𝜌 Γ— 𝑒 Γ— (𝑑𝑦 Γ— 𝑑𝑧)
6
Mass of fluid leaving the face EFGH (outflow) per second,
CONTINUITY EQUATION IN 3
DIMENSIONS:
πœŒπ‘’ 𝑑𝑦𝑑𝑧 +
πœ•
πœ•π‘₯
πœŒπ‘’ 𝑑𝑦𝑑𝑧 𝑑π‘₯
Rate of increase in mass x-direction = mass through ABCD – mass through EFGH
= πœŒπ‘’ 𝑑𝑦𝑑𝑧 βˆ’ πœŒπ‘’ 𝑑𝑦𝑑𝑧 βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ 𝑑𝑦𝑑𝑧 𝑑π‘₯
= βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ 𝑑𝑦𝑑𝑧𝑑π‘₯
= βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ 𝑑π‘₯𝑑𝑦𝑑z
Transport Phenomena
7
Similarly,
Rate of increase in mass in y-direction = βˆ’
πœ•
πœ•π‘¦
πœŒπ‘£ 𝑑π‘₯𝑑𝑦𝑑z
Rate of increase in mass in y-direction = βˆ’
πœ•
πœ•π‘§
πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑z
➒ Total rate of increase in mass = βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ +
πœ•
πœ•π‘¦
πœŒπ‘£ +
πœ•
πœ•π‘§
πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑𝑧
CONTINUITY EQUATION IN 3
DIMENSIONS:
By the law of conversation of mass, there is no accumulation of mass
i.e mass is neither be created nor destroyed in the fluid element.
So net increase of mass per unit time in the fluid element must be
equal to the rate of increase of mass of fluid in the element.
...(1)
Transport Phenomena
8
CONTINUITY EQUATION IN 3
DIMENSIONS:
Mass of fluid in the element is = 𝜌 𝑑π‘₯𝑑𝑦𝑑𝑧 𝜌 =
π‘š
𝑉
π‘š = πœŒπ‘‰
its rate of increase with time
=
πœ•
πœ•π‘‘
𝜌 𝑑π‘₯𝑑𝑦𝑑𝑧
=
πœ•πœŒ
πœ•π‘‘
𝑑π‘₯𝑑𝑦𝑑𝑧
Equating eq. (i) and (ii)
βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ +
πœ•
πœ•π‘¦
πœŒπ‘£ +
πœ•
πœ•π‘§
πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑𝑧 =
πœ•πœŒ
πœ•π‘‘
𝑑π‘₯𝑑𝑦𝑑𝑧
…(2)
Transport Phenomena
9
CONTINUITY EQUATION IN 3
DIMENSIONS:
πœ•πœŒ
πœ•π‘‘
= βˆ’
πœ•
πœ•π‘₯
πœŒπ‘’ +
πœ•
πœ•π‘¦
πœŒπ‘£ +
πœ•
πœ•π‘§
πœŒπ‘€
This is the equation of continuity, which describes the time rate of
change of the fluid density at a fixed point in space.
This equation can be written more concisely by using vector
notation as follows
)
.
( V
t




βˆ’
=
ο‚Ά
ο‚Ά
Rate of increase
of mass per unit
volume
Net rate of addition of
mass per unit volume
by convection
Transport Phenomena

πœ•πœŒ
πœ•π‘‘
+
πœ•
πœ•π‘₯
πœŒπ‘’ +
πœ•
πœ•π‘¦
πœŒπ‘£ +
πœ•
πœ•π‘§
πœŒπ‘€ = 0
β–ͺ For steady state flow
πœ•πœŒ
πœ•π‘‘
= 0 and hence above equation becomes
as,
πœ•
πœ•π‘₯
πœŒπ‘’ +
πœ•
πœ•π‘¦
πœŒπ‘£ +
πœ•
πœ•π‘§
πœŒπ‘€ = 0
β–ͺ If the fluid is incompressible, then 𝜌 is constant and the above eq.
becomes as,
πœ•π‘’
πœ•π‘₯
+
πœ•π‘£
πœ•π‘¦
+
πœ•π‘€
πœ•π‘§
= 0
CONTINUITY EQUATION IN 3
DIMENSIONS:
Continuity equation in three-dimensions.
Transport Phenomena
Thanks!
11

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Transport phenomena (Continuity Equation)

  • 2. 2 HELLO! I’m Mujeeb UR Rahman Chemical Engineering student @Mehran University of Engineering & Technology Jamshoro, Pakistan. You can find me at SlideShare @MujeebURRahman38 ResearchGate @Mujeeb UR Rahman, Academia @Mujeeb UR Rahman
  • 3. Transport Phenomena 3 CONTINUITY EQUATION IN 3 DIMENSIONS: β€œThe equation based on the principle of conversation of mass.” A E C D G F H B dx dz 2kg 1kg 1kg x-axis (u) y-axis (v) z-axis (w)
  • 4. 4 β–ͺ Law of conservation of mass CONTINUITY EQUATION IN 3 DIMENSIONS: π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“ π‘–π‘›π‘π‘Ÿπ‘’π‘Žπ‘ π‘’ π‘œπ‘“ π‘šπ‘Žπ‘ π‘  = π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“ π‘šπ‘Žπ‘ π‘  𝑖𝑛 βˆ’ π‘Ÿπ‘Žπ‘‘π‘’ π‘œπ‘“ π‘šπ‘Žπ‘ π‘  π‘œπ‘’π‘‘ Transport Phenomena
  • 5. Transport Phenomena 5 CONTINUITY EQUATION IN 3 DIMENSIONS: Direction of x, y, z. u οƒž inlet velocity components in x direction. v οƒž inlet velocity components in y direction. w οƒž inlet velocity components in z direction. Mass of fluid entering the face +ve face ABCD (inflow) per second . π‘š 𝑠 𝐷𝑒𝑛𝑠𝑖𝑑𝑦 𝜌 = π‘š 𝑉 οƒž π‘š = 𝜌 Γ— 𝑉 π‘š 𝑠 οƒž 𝜌 Γ— 𝑉 𝑠 οƒž 𝜌 Γ— 𝐴 Γ— 𝑙 𝑠 οƒž 𝜌 Γ— π΄π‘Ÿπ‘’π‘Ž π‘œπ‘“ 𝐴𝐡𝐢𝐷 Γ— π‘£π‘’π‘™π‘œπ‘π‘–π‘‘π‘¦ 𝑖𝑛 π‘₯ π‘‘π‘–π‘Ÿπ‘’π‘π‘‘π‘–π‘œπ‘› = πœŒπ΄π‘‰ οƒž 𝜌 Γ— 𝑒 Γ— (𝑑𝑦 Γ— 𝑑𝑧)
  • 6. 6 Mass of fluid leaving the face EFGH (outflow) per second, CONTINUITY EQUATION IN 3 DIMENSIONS: πœŒπ‘’ 𝑑𝑦𝑑𝑧 + πœ• πœ•π‘₯ πœŒπ‘’ 𝑑𝑦𝑑𝑧 𝑑π‘₯ Rate of increase in mass x-direction = mass through ABCD – mass through EFGH = πœŒπ‘’ 𝑑𝑦𝑑𝑧 βˆ’ πœŒπ‘’ 𝑑𝑦𝑑𝑧 βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ 𝑑𝑦𝑑𝑧 𝑑π‘₯ = βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ 𝑑𝑦𝑑𝑧𝑑π‘₯ = βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ 𝑑π‘₯𝑑𝑦𝑑z Transport Phenomena
  • 7. 7 Similarly, Rate of increase in mass in y-direction = βˆ’ πœ• πœ•π‘¦ πœŒπ‘£ 𝑑π‘₯𝑑𝑦𝑑z Rate of increase in mass in y-direction = βˆ’ πœ• πœ•π‘§ πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑z ➒ Total rate of increase in mass = βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ + πœ• πœ•π‘¦ πœŒπ‘£ + πœ• πœ•π‘§ πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑𝑧 CONTINUITY EQUATION IN 3 DIMENSIONS: By the law of conversation of mass, there is no accumulation of mass i.e mass is neither be created nor destroyed in the fluid element. So net increase of mass per unit time in the fluid element must be equal to the rate of increase of mass of fluid in the element. ...(1) Transport Phenomena
  • 8. 8 CONTINUITY EQUATION IN 3 DIMENSIONS: Mass of fluid in the element is = 𝜌 𝑑π‘₯𝑑𝑦𝑑𝑧 𝜌 = π‘š 𝑉 π‘š = πœŒπ‘‰ its rate of increase with time = πœ• πœ•π‘‘ 𝜌 𝑑π‘₯𝑑𝑦𝑑𝑧 = πœ•πœŒ πœ•π‘‘ 𝑑π‘₯𝑑𝑦𝑑𝑧 Equating eq. (i) and (ii) βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ + πœ• πœ•π‘¦ πœŒπ‘£ + πœ• πœ•π‘§ πœŒπ‘€ 𝑑π‘₯𝑑𝑦𝑑𝑧 = πœ•πœŒ πœ•π‘‘ 𝑑π‘₯𝑑𝑦𝑑𝑧 …(2) Transport Phenomena
  • 9. 9 CONTINUITY EQUATION IN 3 DIMENSIONS: πœ•πœŒ πœ•π‘‘ = βˆ’ πœ• πœ•π‘₯ πœŒπ‘’ + πœ• πœ•π‘¦ πœŒπ‘£ + πœ• πœ•π‘§ πœŒπ‘€ This is the equation of continuity, which describes the time rate of change of the fluid density at a fixed point in space. This equation can be written more concisely by using vector notation as follows ) . ( V t     βˆ’ = ο‚Ά ο‚Ά Rate of increase of mass per unit volume Net rate of addition of mass per unit volume by convection Transport Phenomena
  • 10.  πœ•πœŒ πœ•π‘‘ + πœ• πœ•π‘₯ πœŒπ‘’ + πœ• πœ•π‘¦ πœŒπ‘£ + πœ• πœ•π‘§ πœŒπ‘€ = 0 β–ͺ For steady state flow πœ•πœŒ πœ•π‘‘ = 0 and hence above equation becomes as, πœ• πœ•π‘₯ πœŒπ‘’ + πœ• πœ•π‘¦ πœŒπ‘£ + πœ• πœ•π‘§ πœŒπ‘€ = 0 β–ͺ If the fluid is incompressible, then 𝜌 is constant and the above eq. becomes as, πœ•π‘’ πœ•π‘₯ + πœ•π‘£ πœ•π‘¦ + πœ•π‘€ πœ•π‘§ = 0 CONTINUITY EQUATION IN 3 DIMENSIONS: Continuity equation in three-dimensions. Transport Phenomena