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Air Cooling
of
Electronic Equipments.
Submitted By:-
Shashank kapoor
Mech. 3 rd yr
Submitted To:-
Dr. Manoj Dixit
•
•
Electronic components depend on the passage of electric current
to perform their duties, and they become potential sites for
excessive heating, since the current flow through a resistance is
accompanied by heat generation.
Continued miniaturization of electronic systems has resulted in
a dramatic increase in the amount of heat generated per unit
volume
INTRODUCTION
• The failure rate of electronic equipment increases
exponentially with temperature.
COOLING LOAD OF
ELECTRONIC EQUIPMENT
• The first stage of selection and design of a cooling system is the
determination of heat dissipation.
• The current flow through a resistance is always accompanied by
the heat generation in the amount of Q= 𝐼2Rt.
• The duty cycle is another important consideration in the
design and selection of a cooling technique.
METHODS OF COOLING
Depending upon the load the cooling method is generally chosen.
The methods are:-
 Natural convection cooling.
 Forced convection cooling with air.
 Immersion cooling with natural convection.
 Immersion cooling with boiling.
 Forced circulation of water.
 Heat Pipe.
METHODS OF COOLING
The choice of the cooling method can be decided by using the
chart if we know the heat flux.
 The component manufacturers provide the data about the heat dissipation
rate and maximum allowable temperature for each of the component. The
heat dissipation rate divided by the component area gives the heat flux. For
a heat flux of 0.1 W/cm2 and allowable temperature difference of 60°C
natural convection with radiation can be chosen. If direct forced
convection is adopted for this flux the temperature rise will be limited to
about 15°C. For a heat flux of 1 W/cm2 forced convection will lead to
more than 100°C temperature rise and so the next suitable method,
immersion with fluorocarbons may be the choice.
METHODS OF COOLING
METHODS OF COOLING
Depending upon the load the cooling method is generally chosen.
The methods are:-
 Natural convection cooling.
 Forced convection cooling with air.
 Immersion cooling with natural convection.
 Immersion cooling with boiling.
 Forced circulation of water.
 Heat Pipe.
•Electronic components or PCBs placed in enclosures such as a
TV or DVD player are cooled by natural convection by
providing a sufficient number of vents on the case to enable
the cool air to enter and the heated air to leave the case freely
AIR COOLING:
NATURAL CONVECTION & RADIATION
AIR COOLING:
NATURAL CONVECTION & RADIATION
Heat transfer coefficient can be determined by equation of the
form below for natural convection.
where K depends on the geometric shape and positioning of the
body, L is the flow length on the body and ΔT = TS – T∞
ℎ = 𝑘
∆𝑇
𝐿
0.25
• When hot surfaces are surrounded by cooler surfaces such
as the walls and ceilings of a room or just the sky, the
surfaces are also cooled by radiation
AIR COOLING:
FORCED CONVECTION
•
•
When natural convection cooling is not adequate, we
simply add a fan and blow air through the enclosure that
houses the electronic components.
By doing so, we can increase the heat transfer coefficient by a
factor of up to about 10.
Hollow core cooling
Hollow core cooling
 In cases where air is not allowed to pass over the electronic components,
hollow core method is adopted. Cooling air flows through the hollow space
between the PCBs, collecting heat from the devices mounted on the circuit
boards. The flow area is a rectangle of sides equal to width of PCB and the
depth of the hollow core. Heat generated by the components is conducted
through the PCB and a thin layer of epoxy board to reach the cooling air.
Heat picked up by air is given by
Q = mcp (Tair out – Tair in)
 The heat flow can be also calculated by
Q = hAs ΔTmean
 where As is the heat transfer area. Convection coefficient h, is to be calculated
using the correlations for internal flow. As the temperature difference may
vary, ΔTmean is used for property values. In the case of PCBs heat is
generated uniformly along the length. So in the hollow core cooling the
correlation for constant heat flux should be used.
Thank you

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Air cooling of electrical equipments

  • 1. Air Cooling of Electronic Equipments. Submitted By:- Shashank kapoor Mech. 3 rd yr Submitted To:- Dr. Manoj Dixit
  • 2. • • Electronic components depend on the passage of electric current to perform their duties, and they become potential sites for excessive heating, since the current flow through a resistance is accompanied by heat generation. Continued miniaturization of electronic systems has resulted in a dramatic increase in the amount of heat generated per unit volume INTRODUCTION
  • 3. • The failure rate of electronic equipment increases exponentially with temperature.
  • 4. COOLING LOAD OF ELECTRONIC EQUIPMENT • The first stage of selection and design of a cooling system is the determination of heat dissipation. • The current flow through a resistance is always accompanied by the heat generation in the amount of Q= 𝐼2Rt.
  • 5. • The duty cycle is another important consideration in the design and selection of a cooling technique.
  • 6. METHODS OF COOLING Depending upon the load the cooling method is generally chosen. The methods are:-  Natural convection cooling.  Forced convection cooling with air.  Immersion cooling with natural convection.  Immersion cooling with boiling.  Forced circulation of water.  Heat Pipe.
  • 7. METHODS OF COOLING The choice of the cooling method can be decided by using the chart if we know the heat flux.
  • 8.  The component manufacturers provide the data about the heat dissipation rate and maximum allowable temperature for each of the component. The heat dissipation rate divided by the component area gives the heat flux. For a heat flux of 0.1 W/cm2 and allowable temperature difference of 60°C natural convection with radiation can be chosen. If direct forced convection is adopted for this flux the temperature rise will be limited to about 15°C. For a heat flux of 1 W/cm2 forced convection will lead to more than 100°C temperature rise and so the next suitable method, immersion with fluorocarbons may be the choice. METHODS OF COOLING
  • 9. METHODS OF COOLING Depending upon the load the cooling method is generally chosen. The methods are:-  Natural convection cooling.  Forced convection cooling with air.  Immersion cooling with natural convection.  Immersion cooling with boiling.  Forced circulation of water.  Heat Pipe.
  • 10. •Electronic components or PCBs placed in enclosures such as a TV or DVD player are cooled by natural convection by providing a sufficient number of vents on the case to enable the cool air to enter and the heated air to leave the case freely AIR COOLING: NATURAL CONVECTION & RADIATION
  • 11. AIR COOLING: NATURAL CONVECTION & RADIATION Heat transfer coefficient can be determined by equation of the form below for natural convection. where K depends on the geometric shape and positioning of the body, L is the flow length on the body and ΔT = TS – T∞ ℎ = 𝑘 ∆𝑇 𝐿 0.25
  • 12. • When hot surfaces are surrounded by cooler surfaces such as the walls and ceilings of a room or just the sky, the surfaces are also cooled by radiation
  • 13. AIR COOLING: FORCED CONVECTION • • When natural convection cooling is not adequate, we simply add a fan and blow air through the enclosure that houses the electronic components. By doing so, we can increase the heat transfer coefficient by a factor of up to about 10.
  • 15. Hollow core cooling  In cases where air is not allowed to pass over the electronic components, hollow core method is adopted. Cooling air flows through the hollow space between the PCBs, collecting heat from the devices mounted on the circuit boards. The flow area is a rectangle of sides equal to width of PCB and the depth of the hollow core. Heat generated by the components is conducted through the PCB and a thin layer of epoxy board to reach the cooling air. Heat picked up by air is given by Q = mcp (Tair out – Tair in)  The heat flow can be also calculated by Q = hAs ΔTmean  where As is the heat transfer area. Convection coefficient h, is to be calculated using the correlations for internal flow. As the temperature difference may vary, ΔTmean is used for property values. In the case of PCBs heat is generated uniformly along the length. So in the hollow core cooling the correlation for constant heat flux should be used.