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fundamentals of engineering supplied-reference handbook - Ventech!

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Steam Trap<br />

Junction<br />

Pump<br />

See also THERMODYNAMICS section.<br />

Combustion and Combustion Products<br />

See THERMODYNAMICS section<br />

Energy Storage<br />

Energy storage comes in several forms, including chemical,<br />

electrical, mechanical, and thermal. Thermal storage can<br />

be either hot or cool storage. There are numerous<br />

applications in the HVAC industry where cool storage is<br />

utilized. The cool storage applications include both ice and<br />

chilled water storage. A typical chilled water storage<br />

system can be utilized to defer high electric demand rates,<br />

while taking advantage <strong>of</strong> cheaper <strong>of</strong>f-peak power. A<br />

typical facility load pr<strong>of</strong>ile is shown below.<br />

DEMAND POWER, kW<br />

WITH THERMAL STORAGE<br />

∆P on-peak<br />

WITHOUT THERMAL STORAGE<br />

MIDNIGHT 6 AM NOON 6 PM MIDNIGHT<br />

TIME OF DAY<br />

214<br />

MECHANICAL ENGINEERING (continued)<br />

The thermal storage tank is sized to defer most or all <strong>of</strong> the<br />

chilled water requirements during the electric utility’s peak<br />

demand period, thus reducing electrical demand charges.<br />

The figure above shows a utility demand window <strong>of</strong> 8<br />

hours (noon to 8 pm), but the actual on-peak period will<br />

vary from utility to utility. The Monthly Demand<br />

Reduction (MDR), in dollars per month, is<br />

MDR =∆Pon- peak R , where<br />

∆ Pon-<br />

peak =<br />

Reduced on-peak power, kW<br />

R = On-peak demand rate, $/kW/month<br />

The MDR is also the difference between the demand charge<br />

without energy storage and that when energy storage is in<br />

operation.<br />

A typical utility rate structure might be four months <strong>of</strong> peak<br />

demand rates (June – September) and eight months <strong>of</strong> <strong>of</strong>fpeak<br />

demand rates (October – May). The customer’s utility<br />

obligation will be the sum <strong>of</strong> the demand charge and the<br />

kWh energy charge.<br />

FLUID MECHANICS AND FLUID MACHINERY<br />

Fluid Statics<br />

See FLUID MECHANICS section.<br />

Incompressible Flow<br />

See FLUID MECHANICS section.<br />

Fluid Machines (Incompressible)<br />

See FLUID MECHANICS section and Performance <strong>of</strong><br />

Components above.<br />

Compressible Flow<br />

Mach Number<br />

The local speed <strong>of</strong> sound in an ideal gas is given by:<br />

c = kRT , where<br />

c ≡ local speed <strong>of</strong> sound<br />

C<br />

k ≡ ratio <strong>of</strong> specific heats =<br />

C<br />

R ≡ gas constant<br />

T ≡ absolute temperature<br />

This shows that the acoustic velocity in an ideal gas<br />

depends only on its temperature. The Mach number (Ma)<br />

is the ratio <strong>of</strong> the fluid velocity to the speed <strong>of</strong> sound.<br />

V<br />

Ma ≡<br />

c<br />

V<br />

≡ mean fluid velocity<br />

p<br />

v

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