(a) In order to determine the lift force, Equation 10.28 \sum\limits_{z}{F_{z}} = F_{L} + F_{B} – W – F_{D} = ma_{z} = 0 (Newton’s second law of motion) is applied in the vertical direction. The frontal area is used to compute the drag force for the hot-air balloon, and the drag force is determined by applying Equation 10.12 F_{D} = C_{D} \frac{1}{2} \rho v^{2}A as follows:
\sum\limits_{z}{F_{z}} = F_{L} + F_{B} – W – F_{D} = ma_{z} = 0
D_{b}: = 15 ft A_{frontb}: = \frac{\pi . D_{b}^{2}}{4} = 176.715 ft^{2} h_{b}: = 13 ft C_{Db}: = 1.3
V: = 25 \frac{ft}{sec} b_{c}: = 4 ft d_{c}: = 4 ft h_{c}: = 4 ft \gamma _{air}: = 0.056424 \frac{lb}{ft^{3}}
V_{bc}: = \frac{\pi .D_{b}^{3}}{12} + \frac{1}{3} \left[ \frac{\pi .D_{b}^{2} (h_{b} + h_{c})}{4} \right] – \frac{1}{3} \left(\frac{\pi . b_{c}^{2} h_{c}}{4} \right) + b_{c}. d_{c} . h_{c} = 1.932 \times 10^{3} ft^{3}
W_{b}: = 200 lb W_{c}: = 300 lb W_{bc}: = W_{b} + W_{c} = 500 lb
Guess value: F_{B}: = 100 lb F_{D}: = 100 lb F_{L}: = 100 lb
Given
F_{L} + F_{B} – W_{bc} – F_{D} = 0 F_{B} = \gamma _{air} . V_{bc} F_{D} = C_{Db} \frac{1}{2} \rho _{air} .V^{2} . A_{frontb}
\left ( \begin{matrix} F_{B} \\ F_{D} \\ F_{L} \end{matrix} \right ) : =Find ( F_{B},F_{D}, F_{L})
F_{B} = 109.022 lb F_{D} = 170.631 lb F_{L} = 561.609 lb
(b) The planform area of the hot-air balloon is used to model the lift force for the hotair balloon, and the lift coefficient is determined by applying the lift force equation, Equation 10.21 F_{L} = C_{L} \frac{1}{2} \rho.V^{2} . A, as follows:
slug: = 1 lb \frac{sec^{2}}{ft} \rho _{air} : = 0.0017555 \frac{slug}{ft^{3}} \mu _{air}: = 0.35343 \times 10^{-6} lb \frac{sec}{ft^{2}}
Aplanc: = \frac{\pi . D_{b}^{2}}{4} = 176.715 ft^{2}
Guess value: R : = 10000 C_{L} : = 1.0
F_{L} = C_{L} \frac{1}{2} \rho _{air} .V^{2} . Aplanc R = \frac{\rho _{air} .V .D_{b}}{\mu _{air}}
\left ( \begin{matrix} R \\ C_{L} \end{matrix} \right ) : = Find (R, C_{L})
R = 1.863 \times 10^{6} C_{L} = 5.793
Since R = 1.863 \times 10^{6} , this confirms the assumption that R > 10,000 (see Table 10.6). Furthermore, it is important to note that because such simplistic assumptions (for instance, the planform area of the hot-air balloon in the lift equation) have been made in the estimation and modeling of the lift force, F_{L} , the estimated value of the lift coefficient, C_{L} is a rough estimate at best.
The Drag Coefficient, C_{D} for Three-Dimensional Bodies at Given Orientation to the Direction of Flow, v for R > 10,000 |
 |
C_{D} = 1.3 |
 |
ν
(m/s) |
C_{D} |
10 |
1.0 – 1.4 |
20 |
0.8 – 1.2 |
30 |
0.5 – 0.9 |
40 |
0.3 – 0.7 |
Parachute, A = \pi D^{2}/4 |
Tree, A= frontal area |
 |
C_{D} = 1.0 – 1.4 |
 |
Position |
C_{D} A ( ft^{2} ) |
Standing |
9 |
Sitting |
6 |
Crouching |
2.5 |
High-rise buildings, A = frontal area |
Average person |
|
Position |
A ( ft^{2} ) |
C_{D} |
 |
C_{D} = 0.4 |
 |
Upright |
5.5 |
1.1 |
 |
Racing |
3.9 |
0.88 |
 |
Drafting |
3.9 |
0.5 |
 |
Streamlined |
5.0 |
0.12 |
Bikes |
Large birds, A = frontal area |
 |
Without deflector
C_{D} = 0.96 |
 |
Minivan:
C_{D} = 0.4 |
With deflector:
C_{D} = 0.76 |
 |
Passengercar or
sports car:
C_{D} = 0.3 |
Tractor-trailer truck, A= frontal area |
Automotive, A = frontal area |