First Law of Thermodynamics: Energy Conservation For Mechanical and Industrial Engineering

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Lesson 2: First Law of Thermodynamics: Energy Conservation 1 Taught By Meng Chamnan,

Transcript of First Law of Thermodynamics: Energy Conservation For Mechanical and Industrial Engineering

Lesson 2:

First Law of Thermodynamics:

Energy Conservation

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Taught By Meng Chamnan,

Energy; what is it?

2 By Meng Chamnan GIM

2 2

2 1 2 1

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2KE KE KE m V V

kinetic energy, KE, of the body.

The change in kinetic energy, ΔKE

gravitational potential energy, PE.

The change in gravitational potential

energy, ΔPE 2 1 2 1PE PE PE mg z z

A basic idea is that energy can be stored within systems in

various forms. Energy also can be converted from one form to

another and transferred between systems. For closed systems,

energy can be transferred by work and heat transfer.

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Example 1:

a. To illustrate the proper use of units in the

calculation of such terms, consider a system having a

mass of 1 kg whose velocity increases from 15 m/s to

30 m/s while its elevation decreases by 10 m at a

location where g = 9.7 m/s2.

b. For a system having a mass of 1 lb whose

velocity increases from 50 ft/s to 100 ft/s while its

elevation decreases by 40 ft at a location where g =

32.0 ft/s2.

Both a and b, what are the value of ΔKE and ΔPE?

By Meng Chamnan GIM

Work

work done by the force

can be considered a

transfer of energy to the

body, where it is stored as

gravitational potential

energy and/or kinetic

energy.

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1

dsFW

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W > 0: work done by the system

W < 0: work done on the system

Power

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The rate of energy transfer by work is called power

and is denoted by when a work interaction involves

an observable force; W F V

Power Transmitted by a Shaft

T = FtR

tW F V R R T T

Electric Power.

W i

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Example 2:

Let us evaluate the power required for a bicyclist traveling

at 5.6 m/s to overcome the drag force imposed by the

surrounding air. This aerodynamic drag force is given by

, where CD is a constant called the drag

coefficient, A is the frontal area of the bicycle and rider, and

ρ is the air density. Calculate the power that required for a

bicyclist if using typical values: CD = 0.88, A = 1.2 m2, and ρ

= 0.0005 kg/m3 together with V = 5.6 m/s.

By Meng Chamnan GIM

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2D DF C A V

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Example 3:

A 12-V automotive storage battery is charged with

a constant current of 2 amp for 24 h. If electricity

costs $0.08 per kW·h, determine the cost of

recharging the battery.

By Meng Chamnan GIM

Work: Expansion or Compression

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W pAdx W pdV 2

1

V

V

W pdV

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Example 4:

A gas in a piston–cylinder assembly undergoes an

expansion process for which the relationship between

pressure and volume is given by

The initial pressure is 3 bar, the initial volume is 0.1 m3,

and the final volume is 0.2 m3. Determine the work for the

process, in kJ, if (a) n = 1.5, (b) n = 1.0, and (c) n = 0.

By Meng Chamnan GIM

Energy Transfer by Heat

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Q > 0: heat transfer to the system

Q < 0: heat transfer from the system

adiabatic process there is no energy transfer by heat

Form of Energy

Energy

Kinetics

Potential

Internal

Bulk motion

Position (level)

All other than kinetics and potential

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Energy Accounting: Energy Balance for

Closed Systems

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KE PE U Q W

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Example 5: Four kilograms of a certain gas is contained within a piston–

cylinder assembly. The gas undergoes a process for which

the pressure–volume relationship is

The initial pressure is 3 bar, the initial volume is 0.1 m3, and

the final volume is 0.2 m3. The change in specific internal

energy of the gas in the process is u2 - u1 = - 4.6 kJ/kg. There

are no significant changes in kinetic or potential energy.

Determine the net heat transfer for the process, in kJ.

By Meng Chamnan GIM

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Example 6:

Air is contained in a vertical piston–cylinder assembly

fitted with an electrical resistor. The atmosphere exerts a

pressure of 14.7 lbf/in.2 on the top of the piston, which has

a mass of 100 lb and a face area of 1 ft2. Electric current

passes through the resistor, and the volume of the air

slowly increases by 1.6 ft3 while its pressure remains

constant. The mass of the air is 0.6 lb, and its specific

internal energy increases by 18 Btu/lb. The air and piston

are at rest initially and finally. The piston–cylinder material

is a ceramic composite and thus a good insulator. Friction

between the piston and cylinder wall can be ignored, and

the local acceleration of gravity is g = 32.0 ft/s2.

By Meng Chamnan GIM

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Example 6 (continue…)

Determine the heat transfer from the resistor to the

air, in Btu, for a system consisting of (a) the air alone,

(b) the air and the piston.

By Meng Chamnan GIM

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Example 7: During steady-state operation, a gearbox receives 60 kW

through the input shaft and delivers power through the output

shaft. For the gearbox as the system, the rate of energy

transfer by heat is , where h is a constant, is

the outer surface area of the gearbox, Tb = 300 K (27°C) is the

temperature at the outer surface, and Tf = 293 K (20°C) is the

temperature of the surrounding air away from the immediate

vicinity of the gearbox. For the gearbox, evaluate the heat

transfer rate and the power delivered through the output shaft,

each in kW.

b fQ hA T T

By Meng Chamnan GIM

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Example 8: A silicon chip measuring 5 mm on a side and 1 mm in

thickness is embedded in a ceramic substrate. At steady state,

the chip has an electrical power input of 0.225 W. The top

surface of the chip is exposed to a coolant whose temperature

is 20°C. The rate of energy transfer by heat between the chip

and the coolant is given by , where Tb and Tf are

the surface and coolant temperatures, respectively, A is the

surface area, and If heat transfer between the chip and the

substrate is negligible, determine the surface temperature of

the chip, in °C.

b fQ hA T T

By Meng Chamnan GIM

Energy Analysis of Cycles

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Systems undergoing cycles of the type deliver a

net work transfer of energy to their surroundings

during each cycle

cycle in outW Q Q

Thermal efficiency:

Power Cycles

1cycle in out out

in in in

W Q Q Q

Q Q Q

Refrigeration and Heat Pump Cycles

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cycle out inW Q Q

COP of Refrigeration Cycles

COP of Heat Pump Cycles

in in

cycle out in

Q Q

W Q Q

out out

cycle out in

Q Q

W Q Q

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Example 9:

Each line in the following table gives information

about a process of a closed system. Every entry

has the same energy units. Fill in the blank spaces

in the table.

By Meng Chamnan GIM

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Example 10:

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Wcycle ?

η ?

Qin ?

Wcycle ?

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Example 11:

By Meng Chamnan GIM

Qin ?

Wcycle ?

Qin ?

β ?

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Example 12: A gas undergoes a thermodynamic cycle consisting of three

processes:

Process 1–2: constant volume, V = 0.028 m3, U2 - U1 = 26.4

kJ

Process 2–3: expansion with pV = constant, U3 = U2

Process 3–1: constant pressure, p = 1.4 bar, W31 = -10.5 kJ

There are no significant changes in kinetic or potential

energy.

(a) Sketch the cycle on a p–V diagram.

(b) Calculate the net work for the cycle, in kJ.

(c) Calculate the heat transfer for process 2–3, in kJ.

(d) Calculate the heat transfer for process 3–1, in kJ.

Is this a power cycle or a refrigeration cycle?

By Meng Chamnan GIM