Rocket in Drag

A rocket has an effective frontal area A and blasts off with a constant acceleration a straight up from the surface of the Earth (see Figure 1.1).

Figure 1.1

a) Use either dimensional analysis or an elementary derivation to find out how the atmospheric drag on the rocket should vary as some power(s) of the area A, the rocket velocity v, and the atmospheric density ρ (assuming that we are in the region of high Reynolds numbers).

b) Assume that the atmosphere is isothermal with temperature T. Derive the variation of the atmospheric density ρ with height z. Assume that the gravitational acceleration g is a constant and that the density at sea level is ρ₀.

c) Find the height h₀ at which the drag on the rocket is at a maximum.

SOLUTION

a) Use dimensional analysis to derive the drag force F on the rocket:

(1)

We then have

(2)

So α = γ = 1, β = 2, and

(3)

This formula is generally correct for high Reynolds numbers; for low Reynolds numbers we have Stokes’ law:

(4)

where η is the viscosity and is the radius.

b) For an isothermal atmosphere, take a column of air of height dz and area

A. The pressure difference between top and bottom should compensate the weight of the column:

(5)

or

Using

(6)

where μ is the molar weight of the air, and substituting (6) into (5), we obtain

(7)

Therefore,

(8)

c) At a height h we have, from (3),

(9)

where we used v² = 2ah for uniform acceleration. Now, the maximum force is defined by

(10)

So, assuming that the average temperature for the isothermal atmosphere T = 250 K, we find

(11)

مواضيع ذات صلة

مصطلحات الفيزياء النووية

إزاحة حمراء REDSHIFT

المركبات النانوية (Nanocomposites)

مولد فان دي جراف الالكتروستاتي

التطويرات التقنية الحديثة في المعجلات الالكتروستاتية

معجلات الالكترونات الالكتروستاتية

معجلات الفان دي جراف الترادفية

الحد من زيادة الطاقة في معجل فان دي جراف

أنبوبة التعجيل قي معجلات الجسيمات من نوع فان دي جراف

ارتكاز معجل فان دي جراف

مبدأ تشغيل معجل الفان دي جراف

القضايا الأخلاقية المتعلقة بتكنولوجيا النانو