Showing posts with label RAC. Show all posts
Showing posts with label RAC. Show all posts

Monday, 19 February 2018

Psychrometry

Psychrometric Properties

A mixture of dry air (molecular weight 28.966) and water vapour (molecular weight 18.015) is known as moist air. Degree of freedom of moist air is 3.

1. Specific Humidity / humidity ratio


Humidity ratio (w) is defined as mass of water available in moist air per kilogram of dry air. 

\[ w = \frac{mass of vapour}{mass of dry air} = \frac{m_v}{m_a}\]

Assuming both water vapour and dry air is perfect gas,
\[ \boxed{w = 0.622 \frac{P_v}{P_a} = 0.622\frac{P_v}{P_t - P_a}}\]
Here,  Pv : Partial Pressure of vapour    
Pa : Partial Pressure of air
Pt : Total pressure             

2. Relative Humidity


Relative humidity (φ) is defined as the ratio of mass of vapour to the mass of vapour under saturation condition in the same volume and temperature. 

\[ \boxed{φ = \frac{m_v}{m_{vs}} = \frac{P_v}{P_{vs}}}\]
In case of relative humidity is 100% then 
  • Dry bulb temperature (DBT),  
  • Wet bulb temperature (WBT), 
  • Dew point temperature (DPT), 
  • Saturation temperature will be equal.


If unsaturated moist air is cooled at constant pressure, then the temperature at which the condensation starts is known as dew-point temperature (DPT) of air.


3. Degree of Saturation (μ) 


The ratio of actual specific humidity to specific humidity of saturated air at same temperature is known as degree of saturation. 

\[ μ  = \frac{w}{w_s} = φ \Big(\frac{P_t - P_{vs}}{P_t - P_v}\Big)\]

4. Enthalpy of Moist Air


Total enthalpy will be sum of enthalpy of dry air and vapour.

\( H = H_a + H_v = m_ah_a + m_vh_v\)

moist air enthalpy per kg of dry air = \( \frac{H}{m_a} = h = h_a + w.h_v\)
\[h = 1.005 t + w(2500 + 1.88 t) \]
where, h is in kJ / kg dry air
t is dry bulb temperature in °C

Psychrometric Chart



  • The chart is plotted for one barometric pressure (Atmospheric pressure).
  • Constant enthalpy lines and Wet Bulb Temperature doesn't coincide but practical purpose we can assume them as parallel. 

 Basic Process in Air Conditioning



  • Process of heating/cooling air at constant specific humidity(w) is called sensible heating/cooling.
  • Process of increasing/decreasing specific humidity at constant DBT is called humidification/dehumidification.
  • All other process are combination of these two as shown in above figure.


Sensible Heat Factor


Sensible heat factor (SHF) is defined as the ratio of sensible heat to the total heat.

\[ SHF = \frac{sensible \quad heat}{total \quad heat} = \frac{h_2 - h_1}{h_3 - h_1}\]

  • SHF = 1 for sensible cooling/heating
  • SHF = 0 for humidification/dehumidification





Chemical Dehumidification


This process is done using hygroscopic material which absorbs water vapour from moist air. If process is thermally isolated then enthalpy of air remains constant which causes increases in temperature of air as its moister content decreases.  




Mixing of Two Streams


1. Without Condensation


mass balance of vapour and dry air:
\[m_{a1} + m_{a2} = m_{a3}\]
\[m_{a1}.w_1 + m_{a2}.w_2 = m_{a3}.w_3\]

Energy balance:
\[m_{a1}.h_1 + m_{a2}.h_2 = m_{a3}.h_3\]

from above equations,

Specific humidity of mixture:

\[\boxed{w = \frac{m_{a1}.w_1 + m_{a2}.w_2}{m_{a1} + m_{a2}}}\]

Enthalpy of mixture:

\[\boxed{h = \frac{m_{a1}.h_1 + m_{a2}.h_2}{m_{a1} + m_{a2}}}\]

Temperature of mixture can be approximated:

\[\boxed{t = \frac{m_{a1}.t_1 + m_{a2}.t_2}{m_{a1} + m_{a2}}}\]


2. With Condensation

After condensation some amount of water (Wc) leaves system as liquid water. Due to this, specific humidity of resulting mixture (point 4) will be less than that at point 3. Temperature of air increases due to the release of latent heat of condensation.


\[w_4 = w_3 - w_c\]
\[w4 = \frac{m_{a1}.w_1 + m_{a2}.w_2}{m_{a1} + m_{a2}} - w_c\]
\[h4 = \frac{m_{a1}.h_1 + m_{a2}.h_2}{m_{a1} + m_{a2}} - w_c.h_{f4}\]


By-Pass Factor (BPF)

If Air  is heated from temperature t1 to t2 by coils (ts) then BPF is defines as:


\[ BPF = \frac{Actual \quad loss}{Ideal \quad gain} = \frac{t_s - t_2}{t_s - t_1}\]

Efficiency of Coil = 1 - BPF

If 'n' number of coils with BPF x in a row then equivalent BPF is $x^n$.




  • For sensible heating, coil temperature (ts) should be greater than DBT of air.
  • For sensible cooling, coil temperature should be less than DBT but more than DPT.
  • For cooling and dehumidification $t_s < DPT < DBT$.

Related Post:

Sunday, 18 February 2018

Refrigeration

Refrigeration is the process of producing and maintaining temperature below that of the surrounding atmosphere.

Refrigerant


It is a substance used for producing lower temperature. e.g. NH3, Water, R11, R134. There are two types of refrigerants:
  • Primary Refrigerant: Those refrigerant which absorbs heat directly from storage by undergoing in a cycle. It absorbs latent heat. e.g. NH3, R11,R22, R134.
  • Secondary Refrigerant: These refrigerants are first cooled by primary refrigerants and then used for cooling at the required space. It will not undergo in a cycle and absorbs sensible heat. e.g. Water, brines, glycols and sometimes even halocarbons.

Designation of Refrigerants

  1. For saturated hydrocarbons \( C_mH_nF_pCl_q\) designation is given by:
R (m-1) (n+1)p     and n + p + q = 2m + 2

     for example: $CHF_2Cl$   $\Rightarrow$   R22
                             $CF_2Cl_2$     $\Rightarrow$   R12
                             $C_2H_6$     $\Rightarrow$   R170

    2. For saturated hydrocarbons \( C_mH_nF_pCl_q\) designation is given by:

R 1 (m-1) (n+1)p     and n + p + q = 2m

     for example: $C_2H_4$   $\Rightarrow$   R1150

    3. For inorganic compounds designation is given by:

R  (700 + Molecular weight of refrigerant)

     for example:    $NH_3$   $\Rightarrow$   R717
                             $H_2O$     $\Rightarrow$   R718
                             $CO_2$     $\Rightarrow$   R744

Desirable Properties of Refrigerant


Thermodynamic Properties
  • High critical temperature for high COP.
  • Freezing point should be low as it must operate in the cycle above its freezing point.
  • Specific heat low in liquid phase and high in vapour phase.
  • High thermal conductivity

Chemical Properties
  • non- toxic and non flammable
  • It should not act with material of construction

Physical Properties
  • low viscosity
  • No leakage tendency
  • high dielectric strength

Refrigeration Effect and Capacity

Heat Pump / Refrigerator

Both Heat pump and refrigerator transfers heat from low temperature to high temperature but requirement of refrigerator is to cool the space, however heat pump requirement is to heating the place.


Refrigeration effect(RE) is defined as the heat which is extracted from storage in order to maintain low temperature. 


\( COP_R = \frac{Q_2}{Q_1 - Q_2}= \frac{RE}{Q_1 - Q_2} = \frac{RE}{W}\)


\( COP_{HP} = \frac{Q_1}{W} = 1 + COP_R\)

  • COP signifies the running cost.
  • Higher the COP lower the running cost.
  • COP of heat pump is always greater than one. 

Refrigeration Capacity = Refrigeration effect x mass flow rate

generally refrigeration capacity unit is defined as ton of refrigeration (TR). A ton of refrigeration is defined as "the amount of heat to be removed from one ton (1000 kg) of water at 0°C in order to convert it into ice at 0°C in 24 hrs."

1 TR = 3.5 kJ/s  =  210 kJ/min


Ideal Refrigeration/ Reverse Carnot Cycle


It is the most efficient efficient refrigeration cycle and has highest theoretical COP. COP doesn't depends on working substance in this case.

\[ COP_R = \frac{Q_2}{Q_1 - Q_2}= \frac{T_L}{T_H - T_L}\]

Vapour Compression Refrigeration System (VCRS)

This works on reverse Rankine cycle.


  • Process 1 - 2 : Isentropic Compression
  • Process 2 - 3 : Constant pressure heat rejection
  • Process 3 - 4: iso - enthalpic expansion (h3 = h4)
  • Process 4 - 1 : Constant pressure heat addition
\[ COP = \frac{Q_2}{W} = \frac{h_1 - h_4}{h_2 - h_1} = \frac{h_1 - h_3}{h_2 - h_1}\]

Cascade Refrigeration


In a cascade system a series of refrigerants with progressively lower boiling point are used in a series of single stage units. This is uses for obtaining very low temperature and saves considerable compression work.

  

\[ COP_{overall} =  \frac{COP_1* COP_2}{1 + COP_1 + COP_2}\]

Vapour Absorption Refrigeration System (VARS)


These systems run on low grade energy thus, they are preferred where waste heat is available.  
It employs two fluids refrigerant and absorbent and low pressure refrigerant vapor is absorbed into absorbent and releases large amount of heat. This solution is pumped at high pressure generator where heat is added and added heat causes desorbs from absorbent and its vapour flows to condenser where heat is rejected. The liquid refrigerant throttled through an expansion valve to lower pressure evaporator where it absorbs heat and provides cooling. The remaining absorbent in generator pass through vale to Absorber. 



Maximum COP is given by
\[ COP_{max}  = η_{carnot} . COP_R    = \bigg( \frac{T_G - T_O}{T_G}\bigg) \bigg( \frac{T_R}{T_O - T_R} \bigg)\]
 where To is ambient temperature.


Gas Refrigeration Cycle / Reverse Brayton Cycle

This cycle also known as Joule or Bell - Colemn cycle. 
  • Process 1 - 2 : Isentropic Compression
  • Process 2 - 3 : Constant pressure heat rejection
  • Process 3 - 4:  Isentropic expansion 
  • Process 4 - 1 : Constant pressure heat addition



\[ COP = \frac{1}{\frac{T_2}{T_1} - 1}= \frac{1}{{r_p}^{\frac{γ-1}{γ}} - 1} \]

$r_p$ is pressure ratio = $\frac{P_2}{P_1}$


  • Its COP is low but used in aircraft because of low weight and less costly.

Next: Psychrometry


Related Post:

Contact Form

Name

Email *

Message *