Hydraulic Calculations for CAFA Given: Discharge density = 0.1 GPM/ft2 Protection area = 1,500 ft2 Protection area per sprinkler = 225 ft2 Sprinkler spacing = 15 ft by 15 ft KβFactor = 5.6 GPM/psi1/2 Considering the sprinkler system of CAFA arrange using conventional tree system configuration Calculate the total number of sprinklers and number of sprinkler per branch line at the hydraulically most demanding area of operation. π‘ππ‘ππ ππ’ππππ ππ π πππππππππ =
1,500 ππ‘ 2 = 7 π πππππππππ 225 ππ‘ 2
1.2β1,500 ππ‘ 2 ππ’ππππ ππ π ππππππππ πππ πππππβ ππππ = = 3.1 or 4 sprinklers 15 ππ‘ Note: Consider only 3 sprinklers per branch line (referring to the attached Appendix drawing) Step 1. At sprinkler head no. 1 Flow of the most remote sprinkler: π1 = 0.10
πΊππ ππ‘ 2
(225 ππ‘ 2 )
π1 = 22.5 GPM Pressure to obtain a flow of 22.5 GPM: π = πΎβπ π1 = π1 =
π2 πΎ2 (22.5 )2 (5.6) 2
= 16.14 ππ π
Step 2: Moving towards sprinkler head no. 2 Friction loss from sprinkler head no. 1 to sprinkler head no. 2: Using Hazen/Williams equation, π=
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Where: Q = 22.5 GPM d = 1ββ C = 120 (Galvanized Iron)
π=
4.52(22.5)1.85 ππ π = 0.20426 1.85 4.87 (120) (1) ππ‘
Pressure loss due to friction @ actual length (L) = 15 ft from sprinkler head no. 1 to 2: ππ=πΏ π₯ π ππ=15 π₯ 0.20426
ππ= 3.064 psi The pressure loss in this segment of pipe due to friction is added to the pressure required to deliver minimum flow to the end sprinkler head. Pressure required at sprinkler head no. 2: P2 = 16.14 + 3.064 P2 = 19.204 psi Expected flow at sprinkler head no. 2: π = πΎβπ π = 5.6β19.204 Q2 = 24.541 GPM Note the increase in flow at sprinkler head no. 2. The pipe feeding sprinkler no. 2 is carrying the combined flow of 22.5 GPM to sprinkler head no. 1 and 24.541 GPM to sprinkler head no. 2. Total flow from sprinkler head no. 2 towards sprinkler no. 1: Qt = 22.5 + 24.541 Qt = 47.041 GPM Step 3: Moving towards sprinkler head no. 3 Friction loss from sprinkler head no. 2 to sprinkler head no. 3: Using Hazen/Williams equation, π=
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Where: Q = 47.041 GPM d = 1ββ C = 120 (Galvanized Iron)
π=
4.52(47.041)1.85 ππ π = 0.7993 1.85 4.87 (120) (1) ππ‘
Pressure loss due to friction @ actual length (L) = 15 ft from sprinkler head no. 2 to 3: ππ=πΏ π₯ π ππ=15 π₯ 0.7993 ππ = 11.99 psi The pressure loss in this segment of pipe due to friction is added to the pressure required to deliver minimum flow to the end sprinkler head. Pressure required at sprinkler head no. 3: P3 = 19.204 + 11.99 P3 = 31.194 psi Expected flow at sprinkler head no. 3: π = πΎβπ π = 5.6β31.194 Q3 = 31.277 GPM Note the increase in flow at sprinkler head no. 3. The pipe feeding sprinkler no. 3 is carrying the combined flow of 47.041 GPM to sprinkler head no. 1 and 2 and 31.277 GPM to sprinkler head no. 3. Total flow from sprinkler head no. 3 towards sprinkler no. 1 and 2: Qt = 47.041 + 31.227
Qt = 78.268 GPM Step 4: Moving towards A1 Friction loss from sprinkler head no. 2 point A1: Using Hazen/Williams equation, π=
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Where: Q = 78.268 GPM d = 1 1/4ββ C = 120 (Galvanized Iron) 4.52(78.268)1.85 ππ π π= = 0.6916 1.85 4.87 (120) (1.25) ππ‘ Pressure loss due to friction @ actual length (L) = 5.63 ft from sprinkler head no. 3 to point A1: ππ=πΏ π₯ π ππ= 5.63 π₯ 0.6916 ππ = 3.894 psi Pressure required at point βA1β: PA1 = 31.194 + 3.894 PA1 = 35.088 psi Since there is no flow at point βA1β: QA1 = 0 GPM Qt = 78.268 + 0 = 78.268 GPM Step 5: At Elbow @ point βA1β Friction loss at elbow is the same with friction loss at sprinkler head no. 3 to point βA1β:
π = 0.6916
ππ π ππ‘
1
Equivalent length of1 4β 90o long turn elbow: Le = 2 ft C value multiplier for C = 120; multiplying factor = 1.011 (interpolated) LE = 1.011(2) = 2.022 ft Pressure loss due to friction @ equivalent length (LE) = 2.022 ft:
PΖ = 0.6916 (2.022) = 1. 398 psi Pressure required at elbow: Pat elbow = 1. 398 + 35.088 = 36.486 psi Step 6: Moving towards point βA2β Friction loss at point βA2β is the same with friction loss at sprinkler head no. 3 to point βA1β: π = 0.6916
ππ π ππ‘
Pressure loss due to friction @ actual length (L) = 1.64ft from elbow at point βA1β to point βA2β: PΖ = Ζ x L = 0. 6916 (1.64) PΖ = 1.134 psi Pressure loss due to change in elevation @ H = 1.64ft: Since pressure loss due to change in elevation is 0.433 psi/ft, Pe = 0.433(1.64) = 0.71 psi Pressure required at point βA2β: PA2 = 36.486 + 1.134 + 0.71 PA2 = 38. 33 psi Determining the Kβfactor for this demand will be helpful since this is a significant point in the system and the Kβfactor will use in later calculation process. πΎπ΄2 =
ππ΄2 βππ΄2
=
Step 7: Moving towards point βBβ Friction loss from point βA2β to point βBβ:
78.268 β38.33
= 12.64
πΊππ 1
ππ π 2
Using Hazen/Williams equation,
π=
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Where: Q = 78.268 GPM d = 2ββ C = 120 (Galvanized Iron)
π=
4.52(78.268)1.85 ππ π = 0.07 1.85 4.87 (120) (2) ππ‘
Pressure loss due to friction @ actual length (L) = 15 ft: PΖ = 0.07(15) = 1.05 psi Pressure required at Point βBβ: PB = 1.05 + 38. 33 PB = 39.38 psi Step 8: The next step is to determine the flow and pressure at sprinkler head no.4. Again, minimum flow and pressure are established at this point. Examining the system, note that sprinkler head no. 4 through 6 are laid out exactly the same as heads no. 1 through 3. The procedure for calculating heads 4 through 6 is identical and will results in exactly the same as results in heads 1 through 3. The demand at reference point βBβ is again 78.268 GPM and 38. 33 psi. This is the second time reference point βBβ is reached in the calculation process. There are two calculated pressures at point βBβ. However, only one can exist. The most demanding pressure is the
greater of the two or 39.38 psi. Since the flow and pressure demands are the same, it stands to reason that: KB = KA2 Qnew = KA2 βπ Qnew = 12.64β39.38 = 79.32 GPM (adjusted flow at point "B") The total flow leaving at point βBβ: QB = 78.268 + 79. 32 = 157.588 GPM Step 9: Moving towards point βCβ Friction loss from point βBβ to point βCβ: Using Hazen/Williams equation,
π=
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Where: Q = 157.588 GPM d = 2ββ C = 120 (Galvanized Iron)
π=
4.52(157.588 )1.85 ππ π = 0.256 1.85 4.87 (120) (2) ππ‘
Pressure loss due to friction @ actual length (L) = 15 ft: PΖ = 0.256(15) = 3.84 psi Pressure required at Point βCβ:
PC = 3.84 + 39.38 PC = 43.22 psi Step 10: Again, the next step is to determine the flow and pressure at sprinkler head no. 7. The minimum flow and pressure are established at this point. Examining the system, note that sprinkler head no. 7 through 9 are laid out exactly the same as heads no. 1 through 3. The procedure for calculating heads 7 through 9 is identical and will results in exactly the same as results in heads 1 through 3. The demand at reference point βCβ is again 78.268 GPM and 38.33 psi. This is the second time reference point βCβ is reached in the calculation process. There are two calculated pressures at point βCβ. However, only one can exist. The most demanding pressure is the greater of the two or 43.22 psi. Since the flow and pressure demands are the same, it stands to reason that: KC = KA2 Qnew = KA2 βπ Qnew = 12.64β43.22 = 83.1 GPM (adjusted flow at point "C") The total flow leaving at point βCβ: QB = 157.588 + 83.1 QB = 240.69 GPM
Step 10: At sprinkler head no. 7 π1 = 0.10
πΊππ (225 ππ‘ 2 ) ππ‘ 2
π1 = 22.5 GPM Pressure to obtain a flow of 22.5 GPM: π = πΎβπ π1 = π1 =
π2 πΎ2 (22.5 )2 (5.6) 2
= 16.14 ππ π
Moving towards point βCβ Actual length (include fittings) = 5.63 + 1.64 +2(1.011) = 9.29 ft Lele = 1.64 ft Friction loss from sprinkler head no. 7 to point βCβ: Using Hazen/Williams equation, 4.52π1.85 ππ π π = 1.85 4.87 ( ) πΆ π ππ‘ Where: Q = 22.5 GPM d = 1 1/4ββ C = 120 (Galvanized Iron)
π=
4.52(22.5 )1.85 ππ π = 0.069 1.85 4.87 (120) (1.25) ππ‘
Pressure loss due to friction @ actual length (L) = 9.29 ft from sprinkler head no. 7 to point C: ππ=πΏ π₯ π ππ= 9.29 π₯ 0.069
ππ = 0.641 psi Pressure loss due to elevation @ H = 1.64ft: Pe = 0.433(1.64) = 0.71 psi Pressure required at point βCβ: PC = 16.14 + 0.641 + 0.71 PC = 17.491 psi KβFactor at point βCβ: πΎπΆ =
ππΆ βπΆ
=
22.5 β17.491
= 5.37
πΊππ 1
ππ π 2
This is the second time reference point βCβ is reached in the calculation process. There are two calculated pressures at point βCβ. However, only one can exist. The most demanding pressure is the greater of the two or 43.22 psi. Since the flow and pressure demands are the same, it stands to reason that: Qnew = KC βπ Qnew = 5.37 β43.22 = 35. 3 GPM (adjusted flow at point "C") The total flow leaving at point βCβ: QC = 157.588 + 35. 3 QC = 191.89 GPM Step 11: Moving towards point βIβ (base of the riser) Friction loss from point βCβ to point βIβ: Using Hazen/Williams equation,
π=
Where:
4.52π1.85 ππ π ( ) πΆ 1.85 π 4.87 ππ‘
Q = 191.89 GPM d = 6ββ C = 120 (Galvanized Iron)
π=
4.52(191.89 )1.85 ππ π = 0.00175 1.85 4.87 (120) (6) ππ‘
Actual length (include fittings) = 216.5 + 22.5 + 1.011(2(32) + 3 + 14) = 320 ft Lele = 22.5 ft Pressure loss due to friction @ LT = 168 ft: PΖ = 0.00175 (320) = 0.56 psi Pressure loss due to change in elevation @ H = 22.71ft Pe = 0.433(22.5) = 9.7425 psi Pressure required at point βIβ (base of the riser): PI = 0.56 + 9.7425 + 43.22 PI = 53.52 psi
Additional residual pressure of 15 psi, thus: PI = 53.52 + 15 P1 = 68.32 psi The demand at the base of the riser is 200 GPM and 70 psi