Thermal Energy Flashcards

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1
Q

Change in thermal energy

A

ΔQ = CΔT
or
ΔQ = mcΔT

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2
Q

Heat capacity

A

C= mc

with c = specific heat in J/K per kg

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3
Q

Thermal energy during phase change

A

During a phase change the temperature stays constant

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4
Q

Thermal energy during phase change equation

A

ΔQ = mL, where L = latent heat of evaporation or fusion

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5
Q

Three ways of thermal energy and heat transfer

A
  • Conduction
  • Convection
  • Radiation
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6
Q

Conduction

A

transfer of heat and energy through an object

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7
Q

Parameters that play a role in conductivity

A
  • Temperature difference (T1-T2)
  • Area (cross-section) (A)
    Thickness or length (d or l)
  • Type of material
    -> Thermal conductivity k (W/m*K)
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8
Q

Fourier’s law of heat conduction:

A

P (W) = kA(T1-T2)/d

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9
Q

thermal conductivity k:

A

Is high for for highly conductive materials
Low for not so conductive materials
k<0.2 for insulating materials (wood, paper, glass)

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10
Q

Convection

A

Movement of energy through a fluid based on density differences due to temperature gradients

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11
Q

Convection equation

(Heat transfer due to convection at boundary of body
)

A

P/A = Nu*k(T1-T2)/L

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12
Q

nu =

A

Nusselt number

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13
Q

Radiation

A

Heat transfer by electromagnetic waves

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14
Q

Radiation equation

A

Pe/A = εσT^4

ε = emissivity
σ ~ 5.67 x 10-8 W/(m2K4) (Stefan-Boltzmann constant)

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15
Q

Example of forced convection

A

an oven

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16
Q

Main factors influencing heat conductivity

A
  • thermal conductivity
  • thickness
  • area
17
Q

Ways to improve heat transfer

A
  • use high emessivity materials
  • use high thermal conductvity materials
  • thin walls, large area
  • optimize design to stimulate convection
18
Q

reduce heat transfer

A
  • low emissivity
  • apply insulation to reduce conduction
  • thick walls, small area
  • limit or control ventilation
19
Q

Thermal insulation equation

A

Q = UAΔT

20
Q

Thermal conductance equation

A

U = 1/R = k/d

21
Q

Thermal mass

A

use the thermal capacity of the building to maintain steady interior atmosphere

Example: During the day a large concrete floor absorbs extra heat and radiates it during the night/ cools down during the night.

22
Q

First law of thermodynamics

A

The heat input in a system (Q) and the work output of a system (W) are equal to the change in internal energy ΔU

(mass conservation)

23
Q

Firts law of thermodynamics eqaution

A

ΔU = Q-W

24
Q

Specific enthalpy equation

A

h = u + p*v = u + (p/ρ)

25
Q

Second law of thermodynamics

A
  • The entropy of an isolated system never decreases
  • Heat flows from a high to a low temperature
  • Not all heat can be converted into work
26
Q

Second law thermo equation

A

ηc = 1 - (T2/T1)

27
Q

adiabatic

A

no heat transfer with the surroundings

Q = 0

28
Q

isotherm

A

tempreature stays constant

ΔT = 0

29
Q

Isobaric

A

pressure stays constant

ΔP = 0

30
Q

Isochoric

A

volume stays constant

ΔV = 0

31
Q

enthalpy is useful for describing

A

1) heat transfer at constant pressure

2) Adiabatic compression or expansion

32
Q

formula for heat transfer at constant pressure

A

h1 - h2 = Q

33
Q

Adiabatic compression equation

A

W = h1 - h2

34
Q

Work in thermodynamics

A

W = p * v

35
Q

When there is adiabatic compression or expansion

A

there is no change in entropy

36
Q

entropy equation

A

Δs = ΔQrev/T

37
Q

Two types of closed cycle power plants

A
  • carnot cycle

- rankine cycle

38
Q

The carnot cycle

A

Work goes in at the compressor and leaves at the turbine

Heat comes in at the boiler and leaves at the condensor

39
Q

Carnot cycle power plant

A

Q1 - Q2 = Wt - Wcomp