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"Energi & Hukum I Termodinamika" Bagian - 2

energi & hukum i termodinamika - bagian 2 - mhs

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Page 1: energi & hukum i termodinamika - bagian 2 - mhs

"Energi & Hukum I Termodinamika"

Bagian - 2

Page 2: energi & hukum i termodinamika - bagian 2 - mhs

Hukum Dalam Termodinamika

Hukum Pertama

Tulus B.S. - Teknik Mesin USU2

Terkait dengan kekekalan energi.

Bermakna “energi tidak dapat diciptakandan dimusnahkan namun dapat dikonversidari suatu bentuk ke bentuk yang lain.“

“Perubahan energi dalam dari suatu sistemtermodinamika tertutup sama dengan total dari jumlah energi kalor yang disuplai kedalam sistem dan kerja yang dilakukanterhadap sistem”.

Page 3: energi & hukum i termodinamika - bagian 2 - mhs

Hukum Termodinamika - 1

• The net heat put into a system is equal to the change ininternal energy of the system plus the work done BY thesystem.

• The net heat put into a system is equal to the change ininternal energy of the system plus the work done BY thesystem.

Q = U + W final - initial)

• Conversely, the work done ON a system is equal to thechange in internal energy plus the heat lost in the process.

Tulus B.S. - Teknik Mesin USU3

Page 4: energi & hukum i termodinamika - bagian 2 - mhs

SIGN CONVENTIONS FOR FIRST LAW

• Heat Q input is positive

Q = U + W final - initial)

• Heat Q out is negative

• Work BY a gas is positive

• Work ON a gas is negative

+Qin

+Wout

U

-Win

-Qout

U

Hukum Termodinamika - 1

Tulus B.S. - Teknik Mesin USU4

Page 5: energi & hukum i termodinamika - bagian 2 - mhs

Proses Dalam Termodinamika

Proses Isovolume : V = 0 & W = 0

Proses Isovolume : V = 0 & W = 0

Proses Isobar : P = 0

Proses Isothermal : T = 0 & U = 0

Proses Adiabatik : Q = 0

Dari Hukum Pertama : Q = U + W

Tulus B.S. - Teknik Mesin USU5

Page 6: energi & hukum i termodinamika - bagian 2 - mhs

Proses Isovolume Dikenal juga dengan proses

isometrik atau isokorik

Pada proses isovolume :

V = 0 & W = 0

Kemudian :

Q = U + W so that

Q = U

0

+U -U

QIN QOUT

HEAT IN = INCREASE IN INTERNAL ENERGY

HEAT OUT = DECREASE IN INTERNAL ENERGY

No Work Done

Tulus B.S. - Teknik Mesin USU6

Page 7: energi & hukum i termodinamika - bagian 2 - mhs

Proses Isobar Pada proses isobar : P = 0

Kemudian :

Q = U + W dan

W = P V

-U

QIN QOUT

Work Out Work In

+U

HEAT IN = Wout + INCREASE ININTERNAL ENERGY

HEAT OUT = Wout + DECREASE ININTERNAL ENERGY

Tulus B.S. - Teknik Mesin USU7

Page 8: energi & hukum i termodinamika - bagian 2 - mhs

Proses Isotermal

Pada proses isothermal

T = 0 & U = 0

Q = U + W &

Q = W

NET HEAT INPUT = WORK

OUTPUT

WORK INPUT = NET

HEAT OUT

U = 0Work Out

QIN

U = 0

QOUT

Work In

Tulus B.S. - Teknik Mesin USU8

Page 9: energi & hukum i termodinamika - bagian 2 - mhs

Proses Adiabatik

NO HEAT EXCHANGE : Q = 0

Q = U + W ; W = -U or U = -W

Work done at EXPENSE of internal energy

INPUT Work INCREASES internal energy

Work Out Work In

U +U

Q = 0

W = -U U = -W

Tulus B.S. - Teknik Mesin USU9

Page 10: energi & hukum i termodinamika - bagian 2 - mhs

Reversible

System changes state and can be restored byreversing original process.

Example : Water (s) Water (l)

Irreversible

System changes state and must take a differentpath to restore to original state.

Example : CH4 + 2O2 CO2 + 2H2O

Proses Reversibel & Irreversibel

Tulus B.S. - Teknik Mesin USU 10

Page 11: energi & hukum i termodinamika - bagian 2 - mhs

Aplikasi Hukum Pertama

Tulus B.S. - Teknik Mesin USU11

Energy cannot be created or destroyed; it can only

change forms

Page 12: energi & hukum i termodinamika - bagian 2 - mhs

Aplikasi Hukum Pertama

Tulus B.S. - Teknik Mesin USU12

The energy change of a system during a process is equal to the net work and heat transfer between the system and its surroundings.

In the absence of any work interactions, the energy change of a system is equal to the net heat transfer.

Page 13: energi & hukum i termodinamika - bagian 2 - mhs

Aplikasi Hukum Pertama

Tulus B.S. - Teknik Mesin USU13

The increase in the energy of a potato in an oven is equal to the amount of heat transferred to it.

The work (shaft) done on an adiabatic system is equal to the increase in the energy of the system.

Page 14: energi & hukum i termodinamika - bagian 2 - mhs

Energy Balance

Tulus B.S. - Teknik Mesin USU14

The net change (increase or decrease) in the total energyof the system during a process is equal to the differencebetween the total energy entering and the total energyleaving the system during that process.

That is,

Page 15: energi & hukum i termodinamika - bagian 2 - mhs

Mechanisms of Energy Transfer

Tulus B.S. - Teknik Mesin USU15

Energy can be transferred to or from a system in three forms : heat, work, and mass flow.

The energy content of a control volume can be changed by mass flow as well as heat and work interactions.

Page 16: energi & hukum i termodinamika - bagian 2 - mhs

Massa Atur & Volume Atur

Tulus B.S. - Teknik Mesin USU16

Massa Atur (Closed System) Volume Atur (Open System)

Page 17: energi & hukum i termodinamika - bagian 2 - mhs

Example Cooling of a Hot Fluid in a Tank

Tulus B.S. - Teknik Mesin USU17

A rigid tank contains a hot fluid that is cooled while being stirred by a paddle wheel.

Initially, the internal energy of the fluid is 800 kJ.

During the cooling process, the fluid loses 500 kJ of heat, and the paddle wheel does 100 kJ of work on the fluid.

Determine the final internal energy of the fluid.

Neglect the energy stored in the paddle wheel.

Page 18: energi & hukum i termodinamika - bagian 2 - mhs

Solution

Tulus B.S. - Teknik Mesin USU18

A fluid in a rigid tank looses heat while being stirred.

The final internal energy of the fluid is to be determined.

Assumptions

1 The tank is stationary and thus the kinetic and potential energy changes are zero, KE = PE= 0.

Therefore, E=U and internal energy is the only form of the system’s energy that may change during this process.

2 Energy stored in the paddle wheel is negligible.

Page 19: energi & hukum i termodinamika - bagian 2 - mhs

Tulus B.S. - Teknik Mesin USU19

Analysis : Take the contents of the tank as the system.

This is a closed system since no mass crosses the boundary during the process.

We observe that the volume of a rigid tank is constant, and thus there is no moving boundary work.

Also, heat is lost from the system and shaft work is done on the system.

Applying the energy balance on the system gives

Therefore, the final internal energy of the system is 400 kJ.

Page 20: energi & hukum i termodinamika - bagian 2 - mhs

Energy Conversion Efficiencies

Tulus B.S. - Teknik Mesin USU20

The definition of performance is not limited to thermodynamics only.

Page 21: energi & hukum i termodinamika - bagian 2 - mhs

Combustion Efficiency

Tulus B.S. - Teknik Mesin USU21

Then the performance of combustion equipment can be characterized by combustion efficiency, defined as

A combustion efficiency of 100 percent indicates that the fuel is burned completely and the stack gases leave the combustion chamber at room temperature, and thus the amount of heat released during a combustion process is equal to the heating value of the fuel.

Page 22: energi & hukum i termodinamika - bagian 2 - mhs

Heating Value

Tulus B.S. - Teknik Mesin USU22

Heating value of the fuel, which is the amount of heat released when a unit amount of fuel at room temperature is completely burned and the combustion products are cooled to the room temperature

The definition of the

heating value of gasoline

Page 23: energi & hukum i termodinamika - bagian 2 - mhs

Overall Eficiency

Tulus B.S. - Teknik Mesin USU23

The effects of other factors are incorporated by defining an overall efficiency for the power plant as the ratio of the net electrical power output to the rate of fuel energy input.

The overall efficiencies are about 26-30 percent for gasoline automotive engines, 34-40 percent for diesel engines, and 40-60 percent for large power plants.

Page 24: energi & hukum i termodinamika - bagian 2 - mhs

Efficiency of a Cooking

Tulus B.S. - Teknik Mesin USU24

Efficiency of a cooking appliance can be defined as the ratio of the useful energy transferred to the food to the energy consumed by the appliance

The efficiency of a cooking appliance represents the fraction of the energy supplied to the appliance that is transferred to the food.

Page 25: energi & hukum i termodinamika - bagian 2 - mhs

Efficiencies of Mechanical and Electrical Devices

Tulus B.S. - Teknik Mesin USU25

The mechanical efficiency of a fan isthe ratio of the kinetic energy of air at

the fan exit to the mechanical power input

Page 26: energi & hukum i termodinamika - bagian 2 - mhs

Pump Efficiency and Turbine Efficiency

Tulus B.S. - Teknik Mesin USU26

Page 27: energi & hukum i termodinamika - bagian 2 - mhs

Motor and Generator Efficiency

Tulus B.S. - Teknik Mesin USU27

A pump is usually packaged together with its motor, and a turbine with its generator.

Therefore, we are usually interested in the combined or overall efficiency of pump-motor and turbine-generator combinations which are defined as

Page 28: energi & hukum i termodinamika - bagian 2 - mhs

Example Performance of a Hydraulic Turbine–Generator

Tulus B.S. - Teknik Mesin USU28

The water in a large lake is to be used to generate electricity by the installation of a hydraulic turbine-generator at a location where the depth of the water is 50 m.

Water is to be supplied at a rate of 5000 kg/s.

If the electric power generated is measured to be 1862 kW and the generator efficiency is 95 percent, determine (a) the overall efficiency of the

turbine-generator,

(b) the mechanical efficiency of the turbine, and

(c) the shaft power supplied by the turbine to the generator.

Page 29: energi & hukum i termodinamika - bagian 2 - mhs

Solution

Tulus B.S. - Teknik Mesin USU29

A hydraulic turbine-generator is to generate electricity from the water of a lake.

The overall efficiency, the turbine efficiency, and the turbine shaft power are to be determined.

Assumptions

1 The elevation of the lake remains constant.

2 The mechanical energy of water at the turbine exit is negligible.

Properties The density of water can be taken to be = 1000 kg/m3.

Analysis (a) We take the bottom of the lake as the reference level for convenience.

Then kinetic and potential energies of water are zero, and the change in its mechanical energy per unit mass becomes

Page 30: energi & hukum i termodinamika - bagian 2 - mhs

Tulus B.S. - Teknik Mesin USU30

Page 31: energi & hukum i termodinamika - bagian 2 - mhs

Energy & Environment

Tulus B.S. - Teknik Mesin USU31

Motor vehicles are the largest source of air pollution.

Ground-level ozone,which is the primarycomponent of smog,forms when HC and NOxreact in the presence ofsunlight in hot calm days.

Page 32: energi & hukum i termodinamika - bagian 2 - mhs

Acid Rain

Tulus B.S. - Teknik Mesin USU32

Sulfuric acid and nitric acid are formed when sulfur oxides and nitric oxides react with water vapor and other chemicals high in the atmosphere in the presence of sunlight.

Page 33: energi & hukum i termodinamika - bagian 2 - mhs

Greenhouse Effect

Tulus B.S. - Teknik Mesin USU33

The greenhouse effect makes life on earth possible by keeping the earth warm (about 30°C warmer).

However, excessive amounts of these gases disturb the delicate balance by trapping too much energy, which causes the average temperature of the earth to rise and the climate at some localities to change.

These undesirable consequences of the greenhouse effect are referred to as global warming or global climate change.

Page 34: energi & hukum i termodinamika - bagian 2 - mhs

Tugas Rumah(Jawaban diketik dan dikirim ke email : [email protected])

Tulus B.S. - Teknik Mesin USU34

Page 35: energi & hukum i termodinamika - bagian 2 - mhs

Soal - 1

Tulus B.S. - Teknik Mesin USU35

Water is being heated in a closed pan on top of a range while being stirred by a paddle wheel.

During the process, 30 kJ of heat is transferred to the water, and 5 kJ of heat is lost to the surrounding air.

The paddle-wheel work amounts to 500 Nm.

Determine the final energy of the system if its initial energy is 10 kJ.

Page 36: energi & hukum i termodinamika - bagian 2 - mhs

Soal - 2

Tulus B.S. - Teknik Mesin USU36

Water is pumped from a lower reservoir to a higher reservoir by a pump that provides 20 kW of shaft power.

The free surface of the upper reservoir is 45 m higher than that of the lower reservoir.

If the flow rate of water is measured to be 0.03 m3/s, determine mechanical power that is converted to thermal energy during this process due to frictional effects.

Page 37: energi & hukum i termodinamika - bagian 2 - mhs

Soal - 3

Tulus B.S. - Teknik Mesin USU37

An oil pump is drawing 35 kW of electric power while pumping oil with =860 kg/m3 at a rate of 0.1 m3/s.

The inlet and outlet diameters of the pipe are 8 cm and 12 cm, respectively.

If the pressure rise of oil in the pump is measured to be 400 kPa and the motor efficiency is 90 percent,determine the mechanical efficiency of the pump.