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Thermodynamics Solar Hydrothermal Energy

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Presentation on theme: "Thermodynamics Solar Hydrothermal Energy"— Presentation transcript:

1 Thermodynamics Solar Hydrothermal Energy
By: Aaron Vanderpool

2 Problem: To find a cheap and easy way to heat a home. Question: How much heat can be obtained using the Sun and a water mass collector? Hypothesis: Water can be heated and transfer a significant amount of energy into a building with little to no maintenance if designed correctly using our understanding of physics.

3 My Collector Glass donated by Incline Tahoe Glass

4 Heat is like work and is a form of energy that can be transferred by having a difference in temperature. Ways of transferring heat: Radiation: Happens through empty space in the form of electromagnetic waves. Conduction: Usually through a solid as molecules collide with one another. Convection: Usually in a liquid of gas as lots of molecules are moving about mixing with one another.

5 Radiation We have about 5 kWh/m^2/day average (NREL)
4/24/2015 5:41 0.6 4/24/2015 6:41 4.4 4/24/2015 7:41 18.1 4/24/2015 8:41 30.6 4/24/2015 9:41 144.4 4/24/ :41 196.9 4/24/ :41 460.6 4/24/ :41 1104.4 4/24/ :41 291.9 4/24/ :41 429.4 4/24/ :41 100.6 4/24/ :41 245.6 4/24/ :41 109.4 4/24/ :41 10.6 4/24/ :41 4/24/ :41 3148.7 Radiation 2/5/2015 6:46 0.6 2/5/2015 7:46 30.6 2/5/2015 8:46 31.9 2/5/2015 9:46 51.9 2/5/ :46 598.1 2/5/ :46 641.9 2/5/ :46 639.4 2/5/ :46 576.9 2/5/ :46 46.9 2/5/ :46 34.4 2/5/ :46 33.1 2/5/ :46 2686.3 We have about 5 kWh/m^2/day average (NREL) 1366W/m^2 strikes Earth’s atmosphere. 1000 Watts / m^2 My collector panel m^2 = watts Watts * Seconds = Joules 755.8 watts * 60 seconds * 60 minutes = 2721 kj in 1 hour 2721 kj = 2579 BTU’s 2579 BTUs / lb (15 Gal/56.78 kg Tank) = F (11.45 C) in 1 100% efficiency Reverse Engineer Q = mc ∆T Q = kg * 4186 J/kg C (specific heat of 15C) * C = 2721 kj

6 Conductivity A = Area, d = thickness, k = smC (thermal conductivity of glass) ∆T = change in temperature CPVC (.95 BTU/in/hr/ft.2/°F) Q/t = 6 smC * m^2 * C / .002 m = 8395 J/s Radiation = 1000W/m^2 * m^2 = Watts * 1 second = J/s The back of the collector if just wood Q/t = .1 smC * m^2 * C / .018 m = 48 J/s The glass glazing of the collector Q/t = .84 smC * m^2 * C / m = 2271 J/s (8178 kj/s) Air Q/t = .023 smC * m^2 * C / .06 m = J/s Water Q/t = .56 smC * m^2 * C / .06 m = J/s Limit convection of air Limiting factor is air.

7 Convection buoyancy Accel = 9.8 * (1-(ϱw/ϱ)) 15C
9.8*(1-(1/999.1)) = 26C 9.8*(1-(1/999.1)) = = m/s^2 = 1.4 mm/min^2 = .053 in/min^2 (need a drag force) 4 °C

8 Flow Poiseuille's equation Non-laminar .0001131 * .762 = 0.0000861822
Boyles law Flow Length 15.34m of CPVC pipe Area x 10-4 m^2 Volume x 10 ^-3 m^3 inside piping Viscosity η = .001 Pa*s (water at 20C) F = η A v/l Idea = Find velocity  Find pressure (Bernoulli’s equation)  Find flow (Poiseuille’s equation) V = .007m/s P1 = 1 atm (Bernoulli’s equation) P2 = P1 + ϱg(y1-y2) + 1/2 ϱ (v1^2-v2^2) P2 = ( N/m^2) + (996.8 kg/m^3 * 9.8 * -.5m) + ½ (996.8*.007^2 m/s) = Q = ( ) * pi * ^4 / (8 * .001 * 1) = m^3/s = 2436 cm^3/s P275

9 Convection buoyancy = 1.4 mm/min^2 * 5 min = .007mm/min * x 10-4 m^2 = 7.917×10^-7 m^3 = cm^3/min (need a drag force of pipe and viscosity) 4 °C

10 Putting heat back into the room Thermal Radiation, conduction and convection
Stefan-Boltzman equation Tank Q = 1 * 5.67 x 10^-8 W/m^2*K * .759 m^2 * 299.2^4 K = 345W Watts * Seconds = Joules 345 * Seconds = 2.721×10^6 joules Seconds = 7887 = 2.19 hours in a vacuum Wherever you are not putting radiation heat into the system, the system is losing heat and all those need to be added up.


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