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## Drag: Loss in Ascent, Gain in Descent, and What It Means for Scalability

Jon Goff had an analysis (no equations or numbers though!) of an air-launched reusable SSTO idea, furthermore he promised to look at other reusable orbital launch vehicle ideas in the future. I thought I’d drop a few lines in regards to almost all architectures.

The summary is that big rockets have little drag losses going up but coming down they come too fast and need some tricks.

## Drag in Ascent

The total negative impulse of drag during ascent is to a big order well approximated to be proportional to the frontal area of a rocket. $I_{drag} = \int C_d A \rho_{air}(t)v(t)^2dt \propto A$

Drag loss as delta vee is a more ideal, but even more useful variable. It is simply the integral of drag force per mass. $\Delta v_{drag} =\int \frac{C_d A \rho_{air}(t)v(t)^2}{m(t)} dt$

Of course, mass at any point is directly proportional to takeoff mass. $m(t) \propto m_{glow}$

And thus $\Delta v_{drag} \propto \frac{A}{m_{glow}} = \frac{A}{A \cdot l \cdot \rho_{rocket}} = \frac{1}{l \cdot \rho_{rocket}}$

So the profound result is that drag loss as delta vee is directly proportional to frontal area per liftoff mass, or in the case of a constant shape rocket, inversely proportional to rocket length l and rocket density rho.

It is NOT proportional to frontal area alone. This means that if you have a rocket that is, say, 50 m tall at takeoff, and you make an enlarged version and double it’s diameter while not changing the density, the drag loss delta vee stays the same. Drag loss grows in Joules or Newton seconds of course, but the rocket’s energy and total impulse grow as much at the same time, because the mass grows – both frontal area and thus mass are quadrupled.

What this of course means is that shorter rockets will always suffer from worse drag losses. Increasing density and decreasing the drag coefficient might help a little but probably not that much. Of course, in real life the acceleration profile and trajectory mean a lot too. Here is some data gleaned from this thread at nasaspaceflight.com and from “Space Propulsion Analysis and Design” by Ronald Humble.

• Ariane A-44L: Gravity Loss: 1576 m/s Drag Loss: 135 m/s
• Atlas I: Gravity Loss: 1395 m/s Drag Loss: 110 m/s
• Delta 7925: Gravity Loss: 1150 m/s Drag Loss: 136 m/s
• Shuttle: Gravity Loss: 1222 m/s Drag Loss: 107 m/s
• Saturn V: Gravity Loss: 1534 m/s Drag Loss: 40 m/s (!!)
• Titan IV/Centaur: Gravity Loss: 1442 m/s Drag Loss: 156 m/s

The Saturn V being by far the tallest has a much lower drag loss than the rest. Though it also had the slowest acceleration in the low atmosphere.

## Drag in Descent

The very first post in the whole blog derived the analytical solution for delta vee in a vertical powered landing that takes into account the drag force. The total landing delta vee is: $\Delta v_{land} = v_{ter}(1+\frac{2g}{3a})$

This means the system is sensitive to terminal velocity. And terminal velocity is determined by terminal mass, drag coefficient and frontal area: $m_{ter} g = C_d A \rho_{air} v_{ter}^2$

and $v_{ter} = \sqrt{(m_{ter} g) / (C_d A \rho_{air} ) }$

and $v_{ter} = \sqrt{ (l \rho_{ter} g) / (C_d \rho_{air} ) }$

Meaning that the terminal velocity is inversely proportional to the square root of the length of the rocket l and the density of the almost empty rocket, rho_ter. This means that if density is held constant (a reasonable first assumption), as well as shape (similar C_d), the terminal velocity is doubled when the rocket size (length) is quadrupled. And this means more delta vee needed for landing. It doesn’t matter if the rocket is lengthened and widened or only lengthened. If the constant density is held, the increased length (or depth) just means more mass per frontal area. So, rocket size presents a scalability problem for the powered landing. Bigger rockets have bigger terminal velocities and need more landing deceleration propellants.

## Scalability

What does this mean? Well, a rocket should be tall and dense for ascent to minimize drag losses. And it should be short and fluffy to minimize powered landing requirements. Slenderness or stubbiness is not necessary, but absolute tallness is what counts here, if we assume a constant cross section.

What can be done to help? Well, obviously, the rocket can have small frontal area in ascent but deploy a speed brake when descending to lower terminal velocity. From looking at TGV rockets’ materials, they already have thought of this. But it seems to me they are the first to actually do it. It’s weird that for example Armadillo or Masten hasn’t talked about speed brakes before. They could be very simple structures. The first idea that pops to mind self-evidently is a system that has brake plates on the surface of the rocket that are hinged at the top. During ascent the airflow pushes the brake to stay closed, but during tail-first descent the airflow raises the brake plate up until it hits a builtin stop at 90 degrees. Then it’s perpendicular to the airflow and exerts a maximum drag force. Quadrupling frontal area leads to halving of terminal velocity and thus halving of landing propellant needs.

Let us assume a 1000 kg empty vehicle and braking deceleration of 20 m/s^2 or 2 gees. Penalty is 0.3 and thus total delta vee 1.3 v_ter. Furthermore we can assume an ISP of 255 s or v_ex 2500 m/s.

Entering at 300 m/s (transonic at sea level), the needed braking propellant mass is about 1000 kg * 390 m/s / 2500 m/s = 156 kg. If we use a drag device to quadruple the area (double frontal diameter) the terminal velocity drops to half and propellant needed to 78 kg. Thus we can estimate that the drag device can be mass-useful if it weighs less than 78 kg. On one hand, it introduces additional failure modes, but on the other, it can be deployed pretty early and reduces timing and sensor criticality a lot by decreasing the terminal velocity.

### 7 Responses

1. on Friday 2008.01.11 at 07:29 | Reply Jonathan Goff

Gravity Loss,
Actually, we have talked about drag brakes before. They’re just far enough down the line from where we’re at now that we don’t need them yet. Take a look at the animations of XA-1.0. The notional drag brakes shown haven’t been sized, but they have been thought of.

~Jon

2. on Friday 2008.01.11 at 12:06 | Reply David

Fluffier vehicles have the additional advantage of lower reentry heating. So a deployable drag device could also potentially save on TPS weight as well as lowering the required performance of the TPS.

3. on Friday 2008.01.11 at 14:01 | Reply gravityloss

Ah Jon,
http://masten-space.com/blog/?p=57
I didn’t remember the speed brakes, probably because they look so small and for orientation purposes only, since they’re retracted once the rocket is ignited…
Of course, since the XA-1.0 is so small (100 kg to 100 km) it will probably have a low terminal velocity anyway.
The TGV rocket is much bigger.

But I agree that my tone was too judging, we haven’t actually seen much big designs yet.

4. on Thursday 2010.02.25 at 17:25 | Reply affan

hi sir,
me want to make a rocket in my college event .
i am a student of chemical engieer in the nirma university in the last semester. need ur help sir
hope u will give positive rply

5. […] gravity loss is the more dominant factor over aerodynamic loss. You want another smack…??? Drag: Loss in Ascent, Gain in Descent, and What It Means for Scalability Gravity Loss […]

6. […] quite sleep deprived now.) For those who like to jump into conclusions, it’s going to be like this all over […]

7. on Wednesday 2011.07.06 at 14:47 | Reply trololologuy

Wondering why they make the saturn and the Ares V so high if only gives an extra loss of say 50 m/s if they make them half as tall but 1.41 times as wide. Seems to me a lot of construction weight could be saved that way and a lot of constraints for the payload could go away to. Really insightfull derivation you did there. Thanks.