Minimal altitude to start a “Suicide Burn” - variable thrust

In summary, the problem at hand is to calculate the absolute lowest safe altitude above a planet's surface to start firing the thrusters on a simulated lander in order to reach a velocity of zero at the planet's surface. The force of the thrusters is dependent on the density of the atmosphere, which in turn depends on the altitude above sea level. The goal is to find a general solution that returns an altitude H. The general parameters of the problem include not taking drag into account, a constant craft mass, a straight path of descent along the gravity vector, thrusters pointed straight down, a non-rotating planet, and negligible changes in the planet's gravity. Data accessible from telemetry includes the craft's altitude above the surface, altitude
  • #1
Daquicker
11
0

Homework Statement


I'm trying to calculate the absolute lowest safe altitude above a planet's surface to start firing the thrusters on a simulated lander in order tot just reach vCraft = 0 at the planet's surface.

The force the craft's thrusters responsible for desceleration generate is however dependent on the density of the atmosphere they're in, which in turn depends on the altitude above seaLevel they're currently at.

I'm looking for a general solution that returns an altitude H.

general parameters of the problem:
  • Drag is not to be taken into account.
  • Craft mass does not vary during descent. (Electricity fuels the thrusters so no solid/liquid fuel being burnt).
  • Craft falls straight down along the gravity vector of the planet.
  • Thrusters providing desceleration are pointed straight down along the gravity vector.
  • The planet does not rotate.
  • Planet g does not change. (At applicable altitudes change will be negligible).

Data accesible from telemetry:

general:

  • CraftAltitude above surface: xSurf is known at any time (in m)
  • CraftAltitude above seaLevel: xSea is known at any time (in m)
  • CraftVelocity (downwards): vCraft is known at any time (in m/s)
  • CraftMass: mCraft is known at any time (in Kg)
  • CraftMaxThrust at SeaLevel: xMaxThrustSea is known at any time (in Newton)
  • Planet g: is known at any time (in m/s^2)
for this example:
  • Atmosphere density: Altitude = 0m -> AtmDens = 1 | Altitude = 14400m -> AtmDens = 0
  • Thruster efficiency: AtmDens = 1 -> ThrustEff = 1 | AtmDens = 0.3 -> ThrustEff = 0

Homework Equations


  • Work = m * g * d | m: mCraft, g: aCraft, d: xSurf
  • Kinetic Energy = (m * v^2) / 2 | m: mCraft, v: vCraft

The Attempt at a Solution


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I started with the following simple and common idea:
Get an altitude from the Work required to dissipate the craft's Kinetic Energy

=> W = KE => d = (v^2) / (2 * g)

This however, fails to account for the change in g due to the change in the craft's altitude above sea level (xSea), instead always using the theoretical maximum thrust. The consequence being it gravely underestimates the required braking distance.

I then came up with the following function which describes the craft's instantanious thrust at an altitude xSea:

CraftMaxThrust(xSea) = cMaxThrustSea - (cMaxThrustSea / 100) * ((100 / 0.7) * (1 - (1 - xSea / 14400)))

The acceleration at an altitude xSea provided by the thrusters would then become:

a(xSea) = CraftMaxThrust(xSea) / mCraft

So I figured I needed some type of differential equation to adjust for this shift in force.
This is where I get stuck, all I can come up with is that it should probably be something amongst the lines of:

0 = vCraft + ∫(H->0) |some derivative of a(xSea)?| a(xSea)

With vCraft being initial velocity, a(xSea) adjusted with the planet's g, and H the altitude I've been looking for all along.Eventhough it's not an actual homework assignment, any help would be greatly appreciated, it's been evading me for a couple of days now.
 
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  • #2
Daquicker said:
Electricity fuels the thrusters
A fundamental principle of rocketry is that there has to be something to thrust. Electricity alone is not going to generate an upward force.
 
  • #3
haruspex said:
A fundamental principle of rocketry is that there has to be something to thrust. Electricity alone is not going to generate an upward force.
The electricity powers an "atmospheric thruster", it's more or less really big "fans". Anyways, it's not supposed to be real world, so this can safely be ignored.

Edit: on a rather unrelated sidenote, you did remind me of this article: http://arc.aiaa.org/doi/10.2514/1.B36120
 
  • #4
Daquicker said:
The electricity powers an "atmospheric thruster", it's more or less really big "fans". Anyways, it's not supposed to be real world, so this can safely be ignored.

Edit: on a rather unrelated sidenote, you did remind me of this article: http://arc.aiaa.org/doi/10.2514/1.B36120
Ok, so deceleration will be constant, right? What equations do you know for constant acceleration?
 
  • #5
haruspex said:
Ok, so deceleration will be constant, right? What equations do you know for constant acceleration?
No, deceleration will not be constant, it will increase as the craft's altitude above planetSeaLevel decreases. If it was constant I could have used EKin = Work and gotten a d from that like i wrote in my post?
 
  • #6
Daquicker said:
CraftMaxThrust(h) = cMaxThrustSea - (cMaxThrustSea / 100) * ((100 / 0.7) * (1 - (1 - xSea / 14400)))
That looks unnecessarily complicated. You're just saying the thrust is a linear function of height, right?
Might be easier to think of it backwards, taking off at max thrust, turning thrusters off at some height h, having reached escape velocity, or whatever.
At height x, acceleration is A-Bx. You can write that as a differential equation, yes?
 
  • #7
Your equation for thrust vs height is wrong if for no other reason than it doesn't depend on h. h doesn't appear in the equation!
 
  • #8
Cutter Ketch said:
Your equation for thrust vs height is wrong if for no other reason than it doesn't depend on h. h doesn't appear in the equation!
I edited it so the variable names match.
 
  • #10
haruspex said:
By the way, a linear function of height for density is not likely to be accurate. More likely negative exponntial. See e.g. https://en.wikipedia.org/wiki/Vertical_pressure_variation#In_the_context_of_Earth.27s_atmosphere
The simulation this has to work under is rather symplistic, the atmosphere does scale linearly. The thing I'm stuck on is building up this differential equation. Most, if not all of the information I come across describes acceleration in terms of either time, or velocity. Doing it in terms of position doesn't seem to be very popular.
 
  • #11
Daquicker said:
The thing I'm stuck on is building up this differential equation.
Did you read the last part of my post #6?
 
  • #12
haruspex said:
Did you read the last part of my post #6?
Yes, and I agree looking at the problem "from the bottom up" seems like the sensible thing to do as since it gives you a set starting point. Describing a in terms of altitude (xSea) with form A-Bx because it is a linear function is also ok, can do that.

=> a(xSea) = gPlanet - (cMaxThrustSea - (cMaxThrustSea / 100) * ((100 / 0.7) * (1 - (1 - xSea / 14400)))

with: xSea variable for altitude, cMaxThrust a constant for the particular craft (filling it in would shorten the function but also make it less generic, which is not what I need), and gPlanet the acceleration due to the planet's gravity. This Will return some negative acceleration value given that the thrust is sufficient to overcome the gravity of the planet.

It's the next part I can't get done atm.

The only thing I can come up with is:

vCraft^2 = vCraftInit + 2∫(xSurf -> X) a(X) dx

But I think this isn't correct.
 
  • #13
Daquicker said:
Describing a in terms of altitude ... with form A-Bx
So write that as a differential equation.
 
  • #14
haruspex said:
So write that as a differential equation.
I'll give it another shot tomorrow after a couple hours of sleep, this isn't working after a 26h day.
Thankyou for your time so far though :)
 
  • #15
haruspex said:
So write that as a differential equation.

The only thing I can come up with is:

vCraft^2 = vCraftInit + 2∫(xSurf -> X) a(X) dx

But I think this isn't correct.
 
  • #16
Daquicker said:
The only thing I can come up with is:

vCraft^2 = vCraftInit + 2∫(xSurf -> X) a(X) dx

But I think this isn't correct.

You are making it quite unnecessarily complicated to write and read the equations by using a computer language style. Much easier in normal algebra.
If x is the distance variable, and t is time, how does one normally write the acceleration in calculus notation?
If the acceleration is presumed to be A-Bx for some constants A and B, what differential equation does that give you?
 
  • #17
haruspex said:
You are making it quite unnecessarily complicated to write and read the equations by using a computer language style. Much easier in normal algebra.
If x is the distance variable, and t is time, how does one normally write the acceleration in calculus notation?
If the acceleration is presumed to be A-Bx for some constants A and B, what differential equation does that give you?

With x: distance, t: time, a: acceleration, v: velocity

as far as I know

with a constant -> integrate a to get v
=> v = ∫ a dt
=> v = v0 + at -> integrate v to get x
=> x = ∫ v dt
=> x = ∫ (v0 + at) dt
=> x = x0 + v0t + (at2)/2
<=> a = 2 * (x - x0 - v0t) / t2

with a variable:
a(t)
=> v(t) = v0 + ∫(0->t) a dt'
=> x(t) = x0 + ∫(0->t) v dt'

Sadly I still fail to see how this helps me, I'm probably just missing something really big...
 
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  • #18
Daquicker said:
With x: distance, t: time, a: acceleration, v: velocity

as far as I know

with a constant -> integrate a to get v
=> v = ∫ a dt
=> v = v0 + at -> integrate v to get x
=> x = ∫ v dt
=> x = ∫ (v0 + at) dt
=> x = x0 + v0t + (at2)/2
<=> a = 2 * (x - x0 - v0t) / t2

Sadly I still fail to see how this helps me, I'm probably just missing something really big...
As you pointed out, acceleration will not be not constant.
When I ask a sequence of questions, I am trying to guide you through one question at a time.
Please make an attempt at this very general question:
haruspex said:
If x is the distance variable, and t is time, how does one normally write the acceleration in calculus notation?
Have you actually studied differential equations?
 
  • #19
haruspex said:
As you pointed out, acceleration will not be not constant.
When I ask a sequence of questions, I am trying to guide you through one question at a time.
Please make an attempt at this very general question:

Have you actually studied differential equations?

Last time I had to use one was at least 4 years ago, which is clearly showing.

anyways, with position x(t)
=> v(t) = dx/dt
=> a(t) = dv/dt = d2x/dt2
 
  • #20
Daquicker said:
Last time I had to use one was at least 4 years ago, which is clearly showing.

anyways, with position x(t)
=> v(t) = dx/dt
=> a(t) = dv/dt = d2x/dt2
Right.
Believing that the acceleration should be of the form A-Bx, what differential equation can you write?
 
  • #21
haruspex said:
Right.
Believing that the acceleration should be of the form A-Bx, what differential equation can you write?

## \frac {d^2x}{dt} = A - Bx ##
## <=> \frac {d^2x}{dt} + Bx = A ##

Then get a characteristic equation for ## \frac {d^2x}{dt} + Bx = 0 ## I suppose?
Char. Eq.: ## r^2 + Bx = 0 <=> r = \sqrt{Bx} ## or ## r = - \sqrt{Bx} ##
## => x(t) = C_1 e^{\sqrt{Bx}t} + C_2 e^{- \sqrt{Bx}t}##

Then as since A is a constant, try x(t) = Y with Y a constant, as the "particular solution" of the entire equation?
##D^2(Y) = 0 => BY = A <=> Y = \frac {A}{B}##

Add to the general solution:
##x(t) = C_1 e^{\sqrt{Bx}t} + C_2 e^{- \sqrt{Bx}t} + \frac {A}{B}##

This anywhere near correct?
 
  • #22
Daquicker said:
## \frac {d^2x}{dt} = A - Bx ##
## <=> \frac {d^2x}{dt} + Bx = A ##

Then get a characteristic equation for ## \frac {d^2x}{dt} + Bx = 0 ## I suppose?
Char. Eq.: ## r^2 + Bx = 0 <=> r = \sqrt{Bx} ## or ## r = - \sqrt{Bx} ##
## => x(t) = C_1 e^{\sqrt{Bx}t} + C_2 e^{- \sqrt{Bx}t}##

Then as since A is a constant, try x(t) = Y with Y a constant, as the "particular solution" of the entire equation?
##D^2(Y) = 0 => BY = A <=> Y = \frac {A}{B}##

Add to the general solution:
##x(t) = C_1 e^{\sqrt{Bx}t} + C_2 e^{- \sqrt{Bx}t} + \frac {A}{B}##

This anywhere near correct?
Not bad, but you made a sign error. You should have got √(-B). More simply, try trig functions.
You might have recognised that the homogeneous part of the equation is SHM.
 

What is a "Suicide Burn" in the context of space exploration?

A "Suicide Burn" is a maneuver used by spacecraft to land on a celestial body with minimal fuel consumption. It involves descending towards the surface at a constant rate while firing engines at full thrust, with the goal of reaching zero velocity at the moment of touchdown.

What is the minimal altitude required to perform a "Suicide Burn"?

The minimal altitude required for a "Suicide Burn" varies depending on the specific conditions of the mission, such as the mass and thrust capability of the spacecraft, the gravity and atmosphere of the celestial body, and the precision of the landing target. Generally, it is recommended to start the maneuver at an altitude between 100-200 meters above the surface.

How does variable thrust affect the minimal altitude for a "Suicide Burn"?

Variable thrust, also known as throttle control, allows the spacecraft to adjust the intensity of its engines. This can affect the minimal altitude needed for a "Suicide Burn" as it allows for more precise control of the descent rate. With variable thrust, the minimal altitude can potentially be lower than with fixed thrust.

What are the risks of performing a "Suicide Burn" at a minimal altitude?

The main risk of performing a "Suicide Burn" at a minimal altitude is the potential for a crash landing if the maneuver is not executed perfectly. This can result in damage to the spacecraft or even mission failure. It is crucial to have precise calculations and precise control of the spacecraft during the maneuver.

How do scientists determine the minimal altitude for a "Suicide Burn" in a specific mission?

Scientists use complex mathematical calculations and simulations to determine the minimal altitude for a "Suicide Burn" in a specific mission. This involves considering various factors such as the mass and thrust capability of the spacecraft, the gravity and atmosphere of the celestial body, and the precision of the landing target. They also take into account any potential risks and make adjustments to the maneuver accordingly.

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