thermodynamics i introduction to naval engineering

24
THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

Upload: vernon-long

Post on 26-Dec-2015

233 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

THERMODYNAMICSI

INTRODUCTION TONAVAL

ENGINEERING

Page 2: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

ENERGY ANDHEAT TRANSFER

INTRODUCTION TONAVAL

ENGINEERING

Page 3: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

THERMODYNAMICS:

The science concerned with the inter-relationship between

thermal energy and mechanical energy

Page 4: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

WHAT ARE THE TYPES OF ENERGY?

Stored– Potential (based on position)– Kinetic (based on velocity)

Transitional– Energy that is in the process of being

transferred from one object or system to another. All energy in transition begins and ends as stored energy

Page 5: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

HOW CAN KINETIC ENERGY BE STORED ENERGY?

Definition of energy– “the ability to produce an effect”

The Bullet example– Has the capability for an effect– But it needs something to hit in order

to transfer that energy (the effect)

Page 6: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

MECHANICAL ENERGY

Potential Energy (PE)– PE = mgh

Kinetic Energy (KE)– KE = (1/2)mV2

Mechanical Energy in TRANSITION:– Called Work– Wk = FD

Page 7: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

THERMAL ENERGY Stored Thermal Energy: Called Internal

– Internal Potential Energy• Associated with the force of attraction that exist

between molecules.

– Internal Kinetic Energy• Associated primarily with the activity of the molecules

Thermal Energy in TRANSITION:– Called Heat– Requires a temperature difference between two

systems

Page 8: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

MEASURING THERMAL ENERGY

In the real world we use CALORIES and JOULES but...

BRITISH THERMAL UNIT– Quantity of Heat required to raise the

temperature of 1 lbm of water from 50.9F to 60.9F

– Please don’t write that down

Page 9: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

MODES OF HEAT TRANSFER

Page 10: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

(1) CONDUCTION

Heat flows from hotter to colder region when there is physical contact between the regions

Page 11: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

CONDUCTION (cont.)

The total quantity of heat passed– is proportional to the cross-sectional

area of the conductor over a given time– is proportional to the time of heat flow– in a given length of time is proportional

to the thermal gradient (temp difference)

– depends on the thermal conductivity of the substances

Page 12: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

GENERAL CONDUCTION EQUATION

Q = kTA (t1-t2)/Lwhere

Q : Quantity of heat (Btu or cal)k : Coefficient of thermal conductivity (Btu/((hr)(F)(ft))T : Time (hr)t1 : Temp at hot end (F)

t2 : Temp at cold end (F)

L : Distance between the two ends (in)A : Cross sectional area (sq ft)

Page 13: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

CONDUCTION EXAMPLE

HOT COLD

LENGTH

AREA

Page 14: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

(2) RADIATION

Mode of heat transfer that does not involve any physical

contact between the emitting and receiving regions

Page 15: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

(3) CONVECTION

The mechanical transportation of a mass of fluid from one place to another– Beyond the molecular level– Movement of fluid within fluid– Transportation, not transfer– Fluid’s thermal energy remains in stored

form unless it is transferred by radiation or conduction

Page 16: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

CONVECTION (cont)

TWO TYPES OF CONVECTION– Natural

• Occurs when there are differences in the density of different parts of the fluid. The difference in density are usually caused by a temperature difference.

– Forced• Occurs when some mechanical device,

such as a pump or a fan, produces movement

Page 17: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

DEFINITIONS Sensible Heat

– When heat added results in the change in temperature (kinetic energy)

Latent Heat– When the heat added results in a physical change of

the substance (potential energy)

Saturation Temperature/Pressure– Psat/Tsat– The point at which liquid and vapor may exist in

equilibrium contact with each other

Page 18: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

DEFINITIONS (cont)

Saturated Liquid/Vapor– A liquid/vapor at a specified pressure which is at

Tsat for the pressure– “Wet vapor”

Subcooled Liquid– A liquid at that specified pressure which is below

the Tsat

Superheated Vapor– A vapor that has been raised above Tsat for a

given pressure

Page 19: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

DEFINITIONS (cont)

Latent Heat of Vaporization– Amount of heat necessary to change a mass

of liquid to vapor without changing the temperature

Latent Heat of Fusion– Amount of heat that must be

added/removed to a unit mass to melt/solidify it

Page 20: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING
Page 21: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

GENERAL CONDUCTION EQUATION REVISITED

Q = kTA (t1-t2)/L

MAXIMIZE MINIMIZE

Page 22: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

CounterflowHeat

Exchanger

Parallel Heat Exchanger

TYPES OF HEAT EXCHANGERS

Page 23: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

Crossflow Heat Exchanger

TYPES OF HEAT EXCHANGERS

Page 24: THERMODYNAMICS I INTRODUCTION TO NAVAL ENGINEERING

FACTORS FOR “K”

THE BOUNDARY LAYER SCALE/CHEMICAL DEPOSITS SOOT/DIRT BUILDUP