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Zachary Lovering<br />

Oct. 31, 2008<br />

MAE 2<br />

HW#3<br />

Homework 3 <strong>Solution</strong><br />

Problem 5.23<br />

Description:<br />

Consider a finite wing with an area and aspect ratio of 21.5 and 5, respectively (this is comparable to<br />

the wing on a Gates Learjet, a twin-jet executive transport). Assume the wing has a NACA 65-210 airfoil,<br />

a span efficiency factor of 0.9, and a profile drag coefficient of 0.004. If the wing is at a 6° angle of<br />

attack, calculate and .<br />

Given:<br />

Wing area, 21.5 <br />

Aspect ratio, 5<br />

Airfoil, NACA 65-210<br />

Span efficiency factor, 0.9<br />

Profile drag coefficient, 0.004<br />

Angle of attack, 6°<br />

Find:<br />

Lift coefficient, <br />

Drag coefficient, <br />

Assumptions:<br />

1. Steady flight<br />

2. Incompressible flow<br />

3. Finite wing<br />

Equations:<br />

<br />

<br />

. / (5.65)<br />

(Slope of a straight line)<br />

(5.61)<br />

<br />

(5.58)<br />

Analysis:<br />

The lift curve slope is given in equation 5.65 as<br />

<br />

<br />

1 57.3 / <br />

As noted on pg. 333, “… and are theoretically different but are in practice approximately the same<br />

value for a given wing.” So, we set . To find , the slope of the infinite wing lift curve can be<br />

evaluated at any two points on the linear section of the curve. This curve in found in Appendix D for the<br />

NACA 65-210 wing section. Selecting two points on this curve, the slope is given by


Additionally, from this same curve, the angle of attack at zero lift, , can be found. With these values<br />

known, the finite wing lift coefficient, , is given in equation 5.61 as,<br />

<br />

<br />

<br />

1 57.3 /<br />

The finite wing drag coefficient is given in equation 5.58 as,<br />

<br />

<br />

Since is known and is simply the profile drag, can be found.<br />

Numerical Substitution:<br />

Selecting the following two points on the linear portion of the lift slope curve for the NACA 65-210<br />

airfoil,<br />

Next the slope is calculated to be,<br />

Using the equation for found in the analysis,<br />

Using the equation for found in the analysis,<br />

1.05 at 8°<br />

0 at 1.5°<br />

1.05 0<br />

<br />

8° 1.5°<br />

1.05<br />

9.5°<br />

0.11 <br />

0.11<br />

<br />

1<br />

6° 1.5°<br />

<br />

57.3 0.11<br />

1 <br />

1<br />

<br />

0.95<br />

0.825<br />

1.4458<br />

0.57<br />

0.004 0.57<br />

0.95<br />

0.027


Problem 5.26<br />

Description:<br />

Consider a light, single-engine airplane such as the Piper Super Cub. If the maximum gross weight of the<br />

airplane is 7780 , the wing area is 16.6 , and the maximum lift coefficient is 2.1 with flaps down,<br />

calculate the stalling speed at sea level.<br />

Given:<br />

Gross weight, 7780 <br />

Wing area, 16.6 <br />

Maximum lift coefficient, , 2.1<br />

Find:<br />

Stalling speed, <br />

Assumptions:<br />

1. Sea level<br />

2. Steady level flight<br />

Equations:<br />

<br />

<br />

,<br />

(5.71)<br />

Analysis:<br />

The stalling speed may be calculated using equation 5.71.<br />

Numerical Substitution:<br />

Sea level density is found in Appendix A as,<br />

Using the equation from the analysis,<br />

<br />

<br />

2<br />

, 1.225 <br />

<br />

27780 <br />

1.225 <br />

16.6 2.1<br />

15560 · <br />

<br />

42.7035 <br />

<br />

19.1


Problem 9.4<br />

Description:<br />

Consider a turbojet-powered airplane flying at a standard altitude of 40000 at a velocity of 530 /<br />

. The turbojet engine has an inlet and exit areas of 13 and 10 , respectively. The velocity and<br />

pressure of the exhaust gas at the exit are 1500 / and 450 / , respectively. Calculate the thrust<br />

of the turbojet.<br />

Given:<br />

Standard altitude, 40000 <br />

Air speed, 530 /<br />

Inlet Area, 13 <br />

Exit Area, 10 <br />

Exhaust velocity, 1500 /<br />

Exhaust pressure, 450 / <br />

Find:<br />

Thrust, <br />

Assumptions:<br />

1. Steady flow<br />

2. Conditions at the inlet are the free stream conditions<br />

Equations:<br />

(9.25)<br />

<br />

Analysis:<br />

Using the thrust equation (Eq. 9.25),<br />

<br />

To solve for the air mass flow rate, , the continuity equation is used.<br />

<br />

Substituting the continuity equation into the thrust equation yields,<br />

<br />

where and are found from Appendix A at the altitude of 40000 .<br />

Numerical Substitution:<br />

At a standard altitude of 40000 , from Appendix A it is found that<br />

393.12 <br />

<br />

5.8727 · 10<br />

The velocity must be converted into consistent units,


530 <br />

<br />

777 <br />

<br />

Using the equation for thrust found in the analysis,<br />

Note that,<br />

5.8727 · 10<br />

<br />

1 <br />

5280 <br />

1 3600 <br />

<br />

777<br />

13 1500 <br />

<br />

450 393.12 10 · <br />

4289 567 4858 <br />

<br />

· <br />

<br />

<br />

777


Problem 9.6<br />

Description:<br />

A small ramjet engine is to be designed for a maximum thrust of 1000 at sea level at a velocity of<br />

950 /. If the exit velocity and pressure are 2000 / and 1.0 , respectively, how large should<br />

the inlet be?<br />

Given:<br />

Maximum thrust, 1000 <br />

Air velocity, 950 /<br />

Exit velocity, 2000 /<br />

Exit pressure, 1.0 <br />

Find:<br />

Inlet area, <br />

Assumptions:<br />

1. Sea level<br />

2. Steady flow<br />

3. Conditions at the inlet are the free stream conditions<br />

Equations:<br />

(9.25)<br />

<br />

Analysis:<br />

Using the thrust equation (Eq. 9.25),<br />

<br />

Since the air pressure ahead of the engine, , and exit pressure, , are equal, the thrust equation<br />

reduces to,<br />

Finally, substituting in the continuity equation,<br />

and solving for yields,<br />

<br />

<br />

<br />

<br />

Numerical Substitution:<br />

The density at sea level is 0.002377 / . Using the equation found for inlet area from the<br />

analysis,<br />

1000 <br />

0.002377 <br />

950<br />

<br />

2000<br />

<br />

950


· <br />

1000<br />

<br />

2371 <br />

· 0.42


Problem 9.16<br />

Description:<br />

For the turbojet engine operating under the conditions given in Example 9.3, calculate the propulsive<br />

efficiency, as defined in Prob. 9.15.<br />

Given:<br />

Air velocity, 500 /<br />

Exhaust velocity, 1600 /<br />

Find:<br />

The propulsive efficiency, <br />

Assumptions:<br />

1. Steady flow<br />

2. Thrust from pressure difference is negligible<br />

3. Conditions at the inlet are the free stream conditions<br />

Equations:<br />

<br />

<br />

/ <br />

Analysis:<br />

The propulsive efficiency was defined in Problem 9.15 as,<br />

Numerical Substitution:<br />

Converting the air velocity to consistent units,<br />

Using the equation from the analysis,<br />

500 <br />

<br />

733.33 <br />

<br />

2<br />

<br />

1 / <br />

1 <br />

5280 <br />

1 3600 <br />

2<br />

<br />

<br />

1600<br />

1 <br />

733.33 <br />

<br />

<br />

2<br />

3.1818<br />

0.63

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