Work:- Work is force acting through a distance when the force is parallel to the direction of motion.
Energy:- Types of Work Stored like kinetic energy, potential energy, thermal energy.
Power:- Power expresses a rate of work or energy
Common units include the joule (J), newtonmeter, watt-hour (Wh), foot-pound-force
(ft-lbf), calorie (cal), and the British thermal unit (Btu). Where
Btu = 1055 J(It is the amount of energy needed to heat one pound of water by one degree
Fahrenheit)
Cal = 4.2 J(it is the amount of thermal energy needed to raise the temperature of 1 gram of water by 1°C) ft-lbf = 1.356 J
Common units for power are the watt (W), horsepower (hp), and the ft-lbf/s.
Where
1 hp = 550 ft-lbf/s.
1 hp = 745.7 watt
πΚΉ − πΚΉ = ππΈ ππ‘
Thermal energy is positive when there is an addition of thermal energy to the system and negative when there is a removal.
Work is positive when the system is doing work on the environment and negative when work is done on the system.
π1 Ι£ π£1
2
+ π§1 +
2∗π
+ βπ =
π2 Ι£ π£2
2
+ π§2 +
2∗π
+ βπ‘ + βπΏ
The preview equation based on three main assumptions:-
(a)the flow is steady.
(b) the control volume has one inlet port and one exit port.
(c) the density of the flow is constant.
A horizontal pipe carries cooling water at 10°C for a thermal power plant from a reservoir as shown. The head loss in the pipe is where L is the length of the pipe from the reservoir to the point in question, V is the mean velocity in the pipe, and D is the diameter of the pipe. If the pipe diameter is 20 cm and the rate of flow is 0.06 m3/s, what is the pressure in the pipe at L = 2000 m.
π1
+ π§1 + Ι£
Where π£1
2
2∗π
+ βπ =
π2 Ι£
P1=Patm=0, v1=0, hp=0, ht=0 π£2
2
+ π§2 +
2∗π
+ βπ‘ + βπΏ
Z1=100m, z2=20m π£2 = βπΏ =
π2
π΄
=
0.02∗
0.2
0.06
Π
4
2000
∗(0.2
2 )
∗1.912
= 1.910 m/s
2
= 37.2 m
2∗9.81
100 =
π2
1000 ∗ 9.81
+ 20 +
1.91
2
2 ∗ 9.81
+ 37.2
From the Equation P2 = 418 KPa
πππ€ππ = πΚΉ ∗ π ∗ β
There are loses in energy due to factors such as mechanical friction and leakage.
Efficiency is the ratio of power output to power input
Then
πΌπππ’π‘ πππ€ππ = πΆ ∗ πΚΉ ∗ π ∗ β
A pipe 50 cm in diameter carries water
(10°C) at a rate of 0.5 m3/s. A pump in the pipe is used to move the water from an elevation of 30 m to 40 m. The pressure at section 1 is 70 kPa gage and the pressure at section 2 is 350 kPa gage. What power in kilowatts and in horsepower must be supplied to the flow by the pump? Assume
hL = 3 m of water.
π1
+ π§1 + Ι£
Where π£1
2
2∗π
+ βπ =
π2 Ι£
P1=70000 Pa, P2=350000 Pa π£2
2
+ π§2 +
2∗π z1=30 m, z2=40m
V1=v2, Ht=0, hL=3m
70000
1000 ∗ 9.81
+ 30 + βπ
=
350000
1000 ∗ 9.81
+ 40 + 3
+ βπ‘ + βπΏ
βπ = 41.5π πππ€ππ = πΚΉ ∗ π ∗ β = 1000*0.5*9.81*41.5=204kW
At the maximum rate of power generation, a small hydroelectric power plant takes a discharge of
14.1 m3/s through an elevation drop of 61 m. The head loss through the intakes, penstock, and outlet works is 1.5 m. The combined efficiency of the turbine and electrical generator is 87%. What is the rate of power generation?
π1
+ π§1 + Ι£
Where π£1
2
2∗π
P1=P2=Patm=0
+ βπ =
π2 Ι£ π£2
2
+ π§2 +
2∗π
+ βπ‘ + βπΏ
Z1=61m, z2=0
V1=v2=0
Hp=0, hL=1.5m
Ht=61-1.5=59.5m
πππ€ππ = πΚΉ ∗ π ∗ β =1000*9.81*14.1*59.5=8.23MW
ππ’π‘ πππ€ππ = πΆ ∗ πππ€ππ = 0.87 ∗ 8.23 = 7.16ππ