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Notches
and
Weir
Introduction
 A notch is a device used for measuring the rate
of flow of a liquid through a small channel or a
tank.
 It may be define as an opening in the side of a
tank or a small channel in such a way that the
liquid surface in the tank or a channel is below
the top edge of the opening.
 A weir is a concrete or a masonry structure,
placed in an open channel over which the flow
occurs.
 It is generally in the form of vertical wall, with a
sharp edge at the top, running all the way
across the open channel.
 The notch is of small size while the weir is the
bigger size.
 The notch is generally made of metallic plate
while weir is made of concrete or masonry
structure.
 Nappe or Vein: The sheet of water flowing
through a notch or over a weir is called Nappe
or Vein.
 Crest or Sill: The bottom edge of a notch or a
top of weir over which the water flows, is known
as the sill or crest.
Classification of Notches and
Weir
 The notches are classified as;
 According to the shape of the opening:
1. Rectangular Notch
2. Triangular Notch
3. Trapezoidal Notch
4. Stepped Notch
 According to the effect of the sides of the nappe:
1. Notch with end contraction
2. Notch without end contraction or suppressed
notch
 Weir are classified according to the shape of the
opening the shape of the crest, the effect of the
sides on the nappe and nature of discharge
 According to the shape of the opening:
1. Rectangular weir
2. Triangular weir
3. Trapezoidal weir
 According to the shape of the crest:
1. Sharp-crested weir
2. Broad-crested weir
3. Narrow-crested weir
4. Ogee-shaped weir
 According to the effect of sides on the emerging
nappe:
1. Weir with end contraction
2. Weir without end contraction
Discharge Over a Rectangular
Notch or Weir
 The expression for discharge over a rectangular
notch or weir is the same.
 Consider a rectangular notch or weir provided in
a channel carrying water as shown in fig.
 Let, H = head of water over the crest and L =
Length of the notch or weir.
 For finding a discharge of water flowing over the
weir or notch, consider an elementary horizontal
strip of water of thickness dh and Length L at a
depth of h from free surface of water.
 The area of strip, = L x dh and,
 Theoretical velocity of water flowing through
strip = √2gh
 The discharge dQ, through strip is
dQ = Cd x Area x Velocity
= Cd x L x dh x √2gh
 The total discharge, Q for the whole notch or
weir is determined by integrating the above
equation between the limits 0 to H.
Q = Cd x L x √2gh dh
Q = (2/3) Cd x L x √2g [H]3/2
Discharge Over a Triangular
Notch or Weir
 The expression for the discharge over a
triangular notch or weir is the same.
 Let, H = head of water above V-notch and θ =
angle of notch
 Consider a horizontal strip of water of thickness
“dh” at a depth of h from the free surface of
water as shown in Fig.
 From Fig (b), we have
tan θ/2= AC/OC = AC/(H-h)
AC = (H – h) tan θ/2
 Width of strip, AB = 2AC = 2(H – h) tan θ/2
 Area of strip = 2 (H – h) tan θ/2 dh
 The theoretical velocity of water through strip =
√2gh
 Discharge, dQ through the strip is
= Cd x Area of Strip x Velocity
= 2 Cd (H – h) tan θ/2 dh √2gh
 Total Discharge, Q is will get by integrating the
strip discharge between 0 to H.
∴Q = 8/15 Cd tan θ/2 √2g H(5/2)
 For a right-angled V-notch, if Cd = 0.60
∴ Discharge Q = 1.417 H(5/2)
Advantages of Triangular Notch
or Weir:
 A triangular notch or weir is preferred to a
rectangular weir or notch due to following
reasons:
1. The expression for discharge for a right –
angled V-notch or weir is very simple.
2. For measuring low discharge, a triangular
notch gives more accurate results than a
rectangular.
3. In case of triangular notch, only one reading,
i.e. (H) is required for the computation of
discharge.
Discharge Over a Trapezoidal
Notch or Weir
 As shown in fig., a trapezoidal notch or weir is a
combination of a rectangular and triangular notch or
weir.
 Thus the total discharge will be equal to the sum of
discharge through rectangular weir or notch and
discharge through a triangular notch or weir.
 Let, H = Height of water over notch, L = Length of
the crest of the notch.
 Total Discharge Q
= (2/3) Cd x L x √2g [H]3/2 + 8/15 Cd tan θ/2 √2g
H(5/2)
Effect on Discharge Over a Notch or
Weir due to Error in the
Measurement of Head
 For an accurate value of the discharge over a
weir or notch, an accurate measurement of
head over a weir or notch is very essential as
the discharge over a triangular notch is
proportional H(5/2) to and in case of rectangular
notch it is proportional to H(3/2) .
 A small error in the measurement of head, will
affect the discharge considerably.
1. For rectangular Weir or Notch:
 The discharge for a rectangular weir or notch is
given by Q = (2/3) Cd x L x √2g [H]3/2
 Differentiating the above equation, we get
 dQ = k (3/2) H (½) dH
 Dividing, dQ/Q = (3/2) dH/H
 Equation show that an error of 1% in measuring
H will produce 1.5% error in discharge over a
rectangular weir or notch.
2. For Triangular Weir or Notch:
 The discharge for a triangular weir or notch is
given by Q = 8/15 Cd tan θ/2 √2g H(5/2)
 Differentiating the above equation, we get
 dQ = k (5/2) H (3/2) dH
 Dividing, dQ/Q = (5/2) dH/H
 Equation show that an error of 1% in measuring
H will produce 2.5% error in discharge over a
triangular weir or notch.
Velocity of Approach
 Velocity of approach is defined as the velocity with which
the water approaches or reaches the weir or notch
before it flows over it.
 Thus if Va is the velocity of approach, than an additional
head ha equal to Va
2/2g due to velocity of approach, is
acting on the water flowing over the notch.
 Then initial height of water over the notch becomes (H +
ha) and final height becomes equal to ha.
 Then all the formulae are changed in taking into
consideration of velocity approach.
 The velocity of approach, Va is determined by finding
the discharge over the notch or weir, neglecting velocity
approach.
 Then dividing the discharge by the c/s area of the
channel on the u/s side of the weir or notch, the velocity
of approach is obtained.
 Mathematically, Va = Q / area of channel
 This velocity of approach is used to find an additional
head.
 Again the discharge calculate and above process is
repeated for more accurate discharge.
 Discharge, over a rectangular weir, with velocity
approach = (2/3) Cd x L x √2g [(H1+ha) 3/2 - ha
3/2]
Empirical Formulae for
Discharge Over Rectangular
Weir
 The discharge over a rectangular weir is given
by,
Q = (2/3) Cd √2g L (H)3/2 without velocity
approach
= (2/3) Cd x L x √2g [(H1+ha)3/2 - ha
3/2]
with velocity of approach.
 Both equation are applicable to the weir or notch
for which the crest length is equal to the width of
the channel.
 This type of weir is called Suppressed weir. But
if the weir is not suppressed, the effect of end
Francis Formula
 Francis on the basis of his experiments established that
end contraction decreases the effective length of the
crest of weir and hence decreases the discharge.
 Each end contraction reduces the crest length by 0.1 x
H, where H is the head over the weir.
 For rectangular weir there are two end contractions only
and hence effective length,
L = (L – 0.2 H) and Q = (2/3) Cd √2g L (H)3/2
 If Cd = 0.623, g = 9.81 m/sec2, then
Q = 1.84 (L – 0.2 H)
 If end contractions are suppressed, then
H = 1.84 L H3/2
 If velocity of approach is consider, then
Q = 1.84 L [(H1+ha) 3/2 - ha
3/2]
Bazin’s Formula
 On the basis of results of a series of experiments, Bazin
proposed the following formula for the discharge over a
rectangular weir as,
Q = m L √2g H3/2
where, m = (2/3) Cd = 4.05 + (0.003/H)
 If velocity of approach is considered, then
Q = m1 L √2g [(H1+ha) 3/2 - ha
3/2]
where, m1 = 0.405 + 0.003 / (H + ha)
Discharge Over a Broad Crested
Weir
 A weir having a wide crest is known as broad
crested weir.
 Let, H = height of water above the crest and L =
length of the crest
 If 2L > H, the weir is called broad crested weir
 If 2L < H, the weir is called narrow crested weir
 As shown in fig. let, h = head of water at the
middle of weir which is constant, v = velocity of
flow over the weir.
 By applying Bernoulli’s equation to the still water
surface on the u/s side and running water at the
end of weir,
0 + 0 + H = 0 + v2/2g + h
∴ v2/2g = H – h
∴ v = √[2g (H - h)]
 The discharge over a weir, Q = Cd x Area x
Velocity
∴ Q = Cd x L x h x √[2g (H - h)]
∴ Q = Cd x L x √[2g (Hh2 – h3)]
 The discharge will be maximum, if Hh2 – h3 is
maximum or d/dh Hh2 – h3 = 0 or 2h x H + 3h =
0 or 2H = 3h, ∴ h = 2/3 H
 Qmax will obtained by substituting this value of h
in the equation,
Qmax = Cd x L x √[2g (Hh2 – h3)]
Qmax = 1.705 x Cd x L x H3/2
Discharge Over a Narrow
Crested Weir
 For narrow crested weir, 2L < H. it is similar to a
rectangular weir or notch hence, Q is given by,
∴Q = 2/3 x Cd x L x √2g x H3/2
Discharge Over an Ogee Weir
 As shown in fig. an Ogee weir, in which the crest
of the weir rises up to maximum height of 0.115
x H, and then falls.
 The discharge for an Ogee weir is same as that
of rectangular weir, and it is given by,
∴Q = 2/3 x Cd x L x √2g x H3/2
Discharge Over Submerged or
Drowned Weir
 When the water level on the d/s side of a weir is
above the crest of the weir, then the weir is
called to be submerged or drowned weir.
 The total discharge, over the weir is obtained by
the dividing the weir into two parts.
 The portion between u/s and d/s water surface
may be treated as free weir and portion between
d/s water surface and crest of weir as drowned
weir.
 Let, H = height of water on the u/s of the weir, h
= height of water on the d/s side of weir.
 Then, Q1 = discharge over upper portion
= 2/3 Cd1 x L x √2g x (H – h)3/2
 Q2 = discharge through drowned portion
= Cd2 x Area of flow x Velocity of flow
= Cd2 x L x h x √[2g (H – h)]
 ∴Total discharge, Q = Q1 + Q2
 Q = (2/3) Cd1 x L x √2g x (H – h)3/2 + Cd2 x L x h
x √[2g (H – h)]

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Notches and weir

  • 2. Introduction  A notch is a device used for measuring the rate of flow of a liquid through a small channel or a tank.  It may be define as an opening in the side of a tank or a small channel in such a way that the liquid surface in the tank or a channel is below the top edge of the opening.
  • 3.  A weir is a concrete or a masonry structure, placed in an open channel over which the flow occurs.  It is generally in the form of vertical wall, with a sharp edge at the top, running all the way across the open channel.  The notch is of small size while the weir is the bigger size.  The notch is generally made of metallic plate while weir is made of concrete or masonry structure.
  • 4.  Nappe or Vein: The sheet of water flowing through a notch or over a weir is called Nappe or Vein.  Crest or Sill: The bottom edge of a notch or a top of weir over which the water flows, is known as the sill or crest.
  • 5. Classification of Notches and Weir  The notches are classified as;  According to the shape of the opening: 1. Rectangular Notch 2. Triangular Notch 3. Trapezoidal Notch 4. Stepped Notch  According to the effect of the sides of the nappe: 1. Notch with end contraction 2. Notch without end contraction or suppressed notch
  • 6.  Weir are classified according to the shape of the opening the shape of the crest, the effect of the sides on the nappe and nature of discharge  According to the shape of the opening: 1. Rectangular weir 2. Triangular weir 3. Trapezoidal weir
  • 7.  According to the shape of the crest: 1. Sharp-crested weir 2. Broad-crested weir 3. Narrow-crested weir 4. Ogee-shaped weir  According to the effect of sides on the emerging nappe: 1. Weir with end contraction 2. Weir without end contraction
  • 8. Discharge Over a Rectangular Notch or Weir  The expression for discharge over a rectangular notch or weir is the same.  Consider a rectangular notch or weir provided in a channel carrying water as shown in fig.  Let, H = head of water over the crest and L = Length of the notch or weir.  For finding a discharge of water flowing over the weir or notch, consider an elementary horizontal strip of water of thickness dh and Length L at a depth of h from free surface of water.
  • 9.  The area of strip, = L x dh and,  Theoretical velocity of water flowing through strip = √2gh  The discharge dQ, through strip is dQ = Cd x Area x Velocity = Cd x L x dh x √2gh  The total discharge, Q for the whole notch or weir is determined by integrating the above equation between the limits 0 to H.
  • 10. Q = Cd x L x √2gh dh Q = (2/3) Cd x L x √2g [H]3/2
  • 11. Discharge Over a Triangular Notch or Weir  The expression for the discharge over a triangular notch or weir is the same.  Let, H = head of water above V-notch and θ = angle of notch  Consider a horizontal strip of water of thickness “dh” at a depth of h from the free surface of water as shown in Fig.  From Fig (b), we have tan θ/2= AC/OC = AC/(H-h)
  • 12. AC = (H – h) tan θ/2  Width of strip, AB = 2AC = 2(H – h) tan θ/2  Area of strip = 2 (H – h) tan θ/2 dh  The theoretical velocity of water through strip = √2gh  Discharge, dQ through the strip is = Cd x Area of Strip x Velocity = 2 Cd (H – h) tan θ/2 dh √2gh  Total Discharge, Q is will get by integrating the strip discharge between 0 to H.
  • 13. ∴Q = 8/15 Cd tan θ/2 √2g H(5/2)  For a right-angled V-notch, if Cd = 0.60 ∴ Discharge Q = 1.417 H(5/2)
  • 14. Advantages of Triangular Notch or Weir:  A triangular notch or weir is preferred to a rectangular weir or notch due to following reasons: 1. The expression for discharge for a right – angled V-notch or weir is very simple. 2. For measuring low discharge, a triangular notch gives more accurate results than a rectangular. 3. In case of triangular notch, only one reading, i.e. (H) is required for the computation of discharge.
  • 15. Discharge Over a Trapezoidal Notch or Weir  As shown in fig., a trapezoidal notch or weir is a combination of a rectangular and triangular notch or weir.  Thus the total discharge will be equal to the sum of discharge through rectangular weir or notch and discharge through a triangular notch or weir.  Let, H = Height of water over notch, L = Length of the crest of the notch.  Total Discharge Q = (2/3) Cd x L x √2g [H]3/2 + 8/15 Cd tan θ/2 √2g H(5/2)
  • 16. Effect on Discharge Over a Notch or Weir due to Error in the Measurement of Head  For an accurate value of the discharge over a weir or notch, an accurate measurement of head over a weir or notch is very essential as the discharge over a triangular notch is proportional H(5/2) to and in case of rectangular notch it is proportional to H(3/2) .  A small error in the measurement of head, will affect the discharge considerably.
  • 17. 1. For rectangular Weir or Notch:  The discharge for a rectangular weir or notch is given by Q = (2/3) Cd x L x √2g [H]3/2  Differentiating the above equation, we get  dQ = k (3/2) H (½) dH  Dividing, dQ/Q = (3/2) dH/H  Equation show that an error of 1% in measuring H will produce 1.5% error in discharge over a rectangular weir or notch.
  • 18. 2. For Triangular Weir or Notch:  The discharge for a triangular weir or notch is given by Q = 8/15 Cd tan θ/2 √2g H(5/2)  Differentiating the above equation, we get  dQ = k (5/2) H (3/2) dH  Dividing, dQ/Q = (5/2) dH/H  Equation show that an error of 1% in measuring H will produce 2.5% error in discharge over a triangular weir or notch.
  • 19. Velocity of Approach  Velocity of approach is defined as the velocity with which the water approaches or reaches the weir or notch before it flows over it.  Thus if Va is the velocity of approach, than an additional head ha equal to Va 2/2g due to velocity of approach, is acting on the water flowing over the notch.  Then initial height of water over the notch becomes (H + ha) and final height becomes equal to ha.  Then all the formulae are changed in taking into consideration of velocity approach.
  • 20.  The velocity of approach, Va is determined by finding the discharge over the notch or weir, neglecting velocity approach.  Then dividing the discharge by the c/s area of the channel on the u/s side of the weir or notch, the velocity of approach is obtained.  Mathematically, Va = Q / area of channel  This velocity of approach is used to find an additional head.  Again the discharge calculate and above process is repeated for more accurate discharge.  Discharge, over a rectangular weir, with velocity approach = (2/3) Cd x L x √2g [(H1+ha) 3/2 - ha 3/2]
  • 21. Empirical Formulae for Discharge Over Rectangular Weir  The discharge over a rectangular weir is given by, Q = (2/3) Cd √2g L (H)3/2 without velocity approach = (2/3) Cd x L x √2g [(H1+ha)3/2 - ha 3/2] with velocity of approach.  Both equation are applicable to the weir or notch for which the crest length is equal to the width of the channel.  This type of weir is called Suppressed weir. But if the weir is not suppressed, the effect of end
  • 22. Francis Formula  Francis on the basis of his experiments established that end contraction decreases the effective length of the crest of weir and hence decreases the discharge.  Each end contraction reduces the crest length by 0.1 x H, where H is the head over the weir.  For rectangular weir there are two end contractions only and hence effective length, L = (L – 0.2 H) and Q = (2/3) Cd √2g L (H)3/2  If Cd = 0.623, g = 9.81 m/sec2, then Q = 1.84 (L – 0.2 H)
  • 23.  If end contractions are suppressed, then H = 1.84 L H3/2  If velocity of approach is consider, then Q = 1.84 L [(H1+ha) 3/2 - ha 3/2]
  • 24. Bazin’s Formula  On the basis of results of a series of experiments, Bazin proposed the following formula for the discharge over a rectangular weir as, Q = m L √2g H3/2 where, m = (2/3) Cd = 4.05 + (0.003/H)  If velocity of approach is considered, then Q = m1 L √2g [(H1+ha) 3/2 - ha 3/2] where, m1 = 0.405 + 0.003 / (H + ha)
  • 25. Discharge Over a Broad Crested Weir  A weir having a wide crest is known as broad crested weir.  Let, H = height of water above the crest and L = length of the crest  If 2L > H, the weir is called broad crested weir  If 2L < H, the weir is called narrow crested weir  As shown in fig. let, h = head of water at the middle of weir which is constant, v = velocity of flow over the weir.
  • 26.  By applying Bernoulli’s equation to the still water surface on the u/s side and running water at the end of weir, 0 + 0 + H = 0 + v2/2g + h ∴ v2/2g = H – h ∴ v = √[2g (H - h)]  The discharge over a weir, Q = Cd x Area x Velocity ∴ Q = Cd x L x h x √[2g (H - h)] ∴ Q = Cd x L x √[2g (Hh2 – h3)]
  • 27.  The discharge will be maximum, if Hh2 – h3 is maximum or d/dh Hh2 – h3 = 0 or 2h x H + 3h = 0 or 2H = 3h, ∴ h = 2/3 H  Qmax will obtained by substituting this value of h in the equation, Qmax = Cd x L x √[2g (Hh2 – h3)] Qmax = 1.705 x Cd x L x H3/2
  • 28. Discharge Over a Narrow Crested Weir  For narrow crested weir, 2L < H. it is similar to a rectangular weir or notch hence, Q is given by, ∴Q = 2/3 x Cd x L x √2g x H3/2
  • 29. Discharge Over an Ogee Weir  As shown in fig. an Ogee weir, in which the crest of the weir rises up to maximum height of 0.115 x H, and then falls.  The discharge for an Ogee weir is same as that of rectangular weir, and it is given by, ∴Q = 2/3 x Cd x L x √2g x H3/2
  • 30. Discharge Over Submerged or Drowned Weir  When the water level on the d/s side of a weir is above the crest of the weir, then the weir is called to be submerged or drowned weir.  The total discharge, over the weir is obtained by the dividing the weir into two parts.  The portion between u/s and d/s water surface may be treated as free weir and portion between d/s water surface and crest of weir as drowned weir.  Let, H = height of water on the u/s of the weir, h = height of water on the d/s side of weir.
  • 31.  Then, Q1 = discharge over upper portion = 2/3 Cd1 x L x √2g x (H – h)3/2  Q2 = discharge through drowned portion = Cd2 x Area of flow x Velocity of flow = Cd2 x L x h x √[2g (H – h)]  ∴Total discharge, Q = Q1 + Q2  Q = (2/3) Cd1 x L x √2g x (H – h)3/2 + Cd2 x L x h x √[2g (H – h)]