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From Goddard's Unsolved Variational Rocket Problem to Saturn IGM: Calculus of Variations in Rocket Development

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From Goddard’s Unsolved Variational Rocket Problem to Saturn IGM: Calculus of Variations in Rocket Development

The calculus of variations entered modern rocketry before liquid-fueled rockets had even flown.

In 1916 Robert H. Goddard wrote to the Smithsonian Institution that his theoretical rocket problem had forced him to use an approximation in order to avoid what he called “a new and unsolved problem in the Calculus of Variations.”

Three years later his A Method of Reaching Extreme Altitudes made the issue explicit.

Goddard wanted to determine a rocket ascent for which the initial mass required to deliver a specified final mass to a specified altitude would be a minimum.

That is an optimization problem over an entire trajectory, not merely an algebra problem at one instant.

By the Apollo era, the same broad mathematical idea had become practical engineering.

The Saturn launch vehicle did not solve the full nonlinear calculus-of-variations boundary-value problem aboard the vehicle.

Instead, Marshall Space Flight Center engineers used variational optimization to identify a simple near-optimal steering structure, then built an iterative digital guidance algorithm around that structure.

The result was the Saturn Iterative Guidance Mode, or IGM.

This article follows that history:

  • Goddard’s early minimum-mass ascent problem,
  • the later mathematical development of optimum rocket trajectories,
  • the V-2, Redstone, Jupiter, and Pershing guidance lineage,
  • the Army ballistic Missile Agency transition to NASA Marshall,
  • the variational origin of linear tangent steering,
  • the way Saturn IGM converted an optimization result into an onboard guidance law.

PIC

Figure 1. A compressed historical timeline. Goddard recognized the variational structure of rocket optimization before practical liquid-fuel rocketry existed. Army missile guidance later emphasized reference-trajectory correction, while the Saturn era combined optimization theory with digital onboard computation.

1 A necessary historical distinction

There was not one continuous algorithm passed unchanged from Goddard to Apollo.

Several different lines of development converged.

The three lines can be summarized without treating them as one continuous algorithm:

  • Mathematical line: rocket performance led to trajectory optimization and then to calculus-of-variations formulations.
  • Missile-guidance line: V-2 experience led into Redstone, Jupiter, and Pershing, with analog computation and reference-trajectory correction.
  • Computational line: ground-based optimization was gradually joined by digital onboard computation and path-adaptive guidance.

The historical importance of IGM is that these lines finally met.

2 Goddard’s question was already variational

Goddard’s 1919 report begins with a performance question.

Suppose a rocket loses mass continuously while climbing vertically.

A final payload mass is to remain when the rocket reaches a required altitude.

What initial mass is necessary?

Goddard did not merely ask for the motion produced by a prescribed rocket.

He asked which motion minimizes the required mass.

He wrote the vertical speed as an unknown function of altitude:

v = f (s),
(1)

where

s
(2)

is altitude.

The expelled mass then depends on the entire function

f (s ).
(3)

The goal is therefore schematically

        ∫     (        )
          sf        df-
m [f] =     F   s,f,ds   ds →  min .
         s0
(4)

That is the structure of a calculus-of-variations problem.

PIC

Figure 2. Goddard’s vertical rocket problem. Gravity and atmospheric resistance oppose ascent while propellant mass is expelled. The unknown is not one number but an ascent history, which is why minimization naturally becomes a variational problem.

3 Why ordinary differential equations were not enough

If the thrust or mass-loss history were already known, the equations of motion could be integrated.

Optimization changes the nature of the problem.

The trajectory must satisfy dynamics such as

˙
h = v,
(5)

    T −  D
˙v = -------−  g,
      m
(6)

and

       T
m˙=  − --,
       c
(7)

while a performance quantity is extremized.

Here:

  • h  is altitude,
  • v  is vertical speed,
  • m  is rocket mass,
  • T  is thrust,
  • D  is drag,
  • c  is effective exhaust velocity.

A modern Goddard-type problem can be stated as

max h (tf)
(8)

or, in a form closer to Goddard’s original concern,

min m0
(9)

subject to prescribed final conditions.

The optimization therefore includes a function such as

T(t)
(10)

or an equivalent burning history.

4 Goddard’s unsolved calculus-of-variations problem

In the published report Goddard explained that the minimum requires an unknown velocity function

v =  f(s)
(11)

for which

δm =  0.
(12)

He then stated that determining this function by the rigorous procedure led to a new and unsolved calculus-of-variations problem.

Instead of stopping, he constructed an approximate procedure.

He divided the ascent into altitude intervals, treated important quantities approximately within each interval, and searched for the minimum mass required in each segment.

The historical lesson is important:

  • Rocket optimization appeared before the mathematical and computational machinery needed to solve the realistic problem cleanly.

5 Goddard was asking an optimal-control question before optimal control existed

The modern language of states and controls came later.

Retrospectively, Goddard’s problem contains all of the basic elements:

  • dynamical state variables,
  • a controllable burning history,
  • variable mass,
  • gravity,
  • drag,
  • endpoint requirements,
  • an integral or terminal performance criterion.

This is the same general structure later formalized by:

  • the classical calculus of variations,
  • the Mayer, Lagrange, and Bolza problem formulations,
  • the Pontryagin maximum principle,
  • modern optimal control.

It is therefore reasonable to call the later vertical ascent optimization problem the Goddard problem, but the modern textbook form should not be confused with every detail of Goddard’s original 1919 approximation.

6 Hamel and the interwar mathematical continuation

The problem did not disappear.

Georg Hamel returned to Goddard’s rocket optimization problem in 1927 and treated the optimum burning program explicitly with calculus-of-variations methods.

Later historical reviews of optimal flight mechanics identify Goddard and Hamel as early examples of applying variational ideas to rocket-powered flight.

During the following decades, increasingly general formulations were developed for:

  • optimum climb,
  • minimum fuel,
  • maximum altitude,
  • maximum range,
  • constrained flight paths.

By the 1950s and early 1960s, the mathematical literature on optimum rocket trajectories had become much richer.

Later reviews list work by Tsien and Evans, Miele and Cavoti, Leitmann, Garfinkel, and others as part of the continuing development of the Goddard problem.

7 The wartime and missile-guidance line developed differently

The practical guidance systems of early ballistic missiles were not simply onboard calculus-of-variations solvers.

A missile had to:

  • sense attitude and acceleration,
  • reject disturbances,
  • follow a useful trajectory,
  • shut down propulsion at the correct condition,
  • operate with the computers available at the time.

The available hardware strongly shaped the guidance philosophy.

8 V-2 to Redstone, Jupiter, and Pershing

Clyde D. Baker’s 1965 historical summary of Saturn guidance described an important lineage.

Beginning with the V-2 and continuing through the Army’s Redstone, Jupiter, and Pershing missiles, the delta-minimum concept was used successfully.

Its basic philosophy was:

  • determine a nominal geometrical trajectory before flight,
  • measure how the actual vehicle differs from that reference,
  • command corrections that drive the vehicle back toward the reference trajectory.

The nominal trajectory was determined before flight.

Guidance corrections attempted to reduce deviations from it.

Analog computation was well suited to this type of implementation.

PIC

Figure 3. Delta-minimum guidance and variational guidance answer different questions. Delta-minimum tries to recover a precomputed reference path. Variational guidance asks what steering history best satisfies a performance objective and terminal constraints from the state that actually exists.

9 Why delta-minimum worked for missiles

For a ballistic missile:

  • the mission geometry was highly repeatable,
  • the desired path could be designed before launch,
  • onboard analog computing resources were limited,
  • returning toward a known reference trajectory was a practical strategy.

This did not mean optimization was irrelevant.

Optimum trajectories could still be designed on the ground.

But the onboard guidance system did not have to solve a new optimum trajectory during flight.

10 The U.S. Army rocket-development bridge

After World War II, the German rocket team and U.S. Army missile organizations developed a sequence of increasingly capable vehicles.

The Redstone became the first operational U.S. large ballistic missile.

The Jupiter program extended Army ballistic-missile experience.

Pershing continued the tactical ballistic-missile line.

Jupiter-C and Juno connected that missile technology to early U.S. space launch.

The same broad technical community in Huntsville then became central to Saturn.

PIC

Figure 4. The institutional and technical bridge from Army rocketry to Saturn. The Army Ballistic Missile Agency concentrated experience in propulsion, inertial guidance, computation, testing, and flight mechanics. Its core transferred to NASA Marshall in 1960.

11 The Army Ballistic Missile Agency

The Army Ballistic Missile Agency, ABMA, was created in 1956 around the Redstone development organization.

Its work included:

  • Redstone,
  • Jupiter,
  • Jupiter-C,
  • early Saturn concepts,
  • inertial guidance and control,
  • flight computation and simulation.

On July 1, 1960, the technical and administrative core of ABMA transferred to NASA and became the George C. Marshall Space Flight Center.

That institutional continuity matters.

Saturn guidance did not begin in isolation.

It grew from engineers already experienced with V-2-derived and Army missile technology, but who now faced a substantially different space-launch problem.

12 Why Saturn required a different guidance philosophy

Baker identified two changes around 1960.

First, new optimization methods made payload maximization and minimum-propellant trajectory design increasingly practical.

Second, digital computers were replacing analog computers as onboard hardware.

Saturn also demanded greater mission flexibility.

A space launch vehicle might have to accommodate:

  • engine-performance dispersions,
  • staging variations,
  • engine-out conditions,
  • different orbital targets,
  • translunar injection conditions.

For this environment, forcing every disturbed flight back toward one nominal geometrical trajectory was unnecessarily restrictive.

A better guidance question was:

  • Given the vehicle’s measured state now, what thrust direction should be commanded so that the required terminal conditions are still achieved with nearly minimum propellant?

That is much closer to an optimal-control question.

13 The full optimum Saturn problem was still too difficult onboard

A realistic Saturn optimization model would include:

  • a rotating Earth,
  • spheroidal gravity,
  • multiple stages,
  • changing thrust and mass,
  • coast intervals,
  • three-dimensional motion,
  • terminal position and velocity requirements.

In principle, calculus-of-variations methods can formulate this problem.

But Baker explicitly noted that the full optimum-thrust-direction calculation required computational resources far beyond the onboard computer capability of the time.

The engineering solution was therefore not to abandon optimization.

It was to simplify the variational problem until its structure could be carried onboard.

14 The simplified variational model

Consider vacuum powered flight over a flat Earth with constant gravity.

Use two position coordinates:

x
(13)

downrange and

y
(14)

vertical.

The simplified dynamics are

x˙= vx,
(15)

y˙= vy,
(16)

v˙x =  a(t) cos𝜃,
(17)

˙vy = a(t)sin 𝜃 − g.
(18)

The thrust magnitude history

a(t)
(19)

is treated as known from the vehicle model.

The control is the thrust direction

𝜃 (t).
(20)

15 A variational derivation of the steering structure

Introduce multipliers

px,  py,  qx,   qy
(21)

for the position and velocity equations.

An augmented integrand can be written schematically as

ℒ = px(vx −ẋ) + py(vy −ẏ) (22)
+ qx(a cos 𝜃 −vx) (23)
+ qy(a sin 𝜃 − g −vy). (24)

Stationarity with respect to the states gives the adjoint structure

p˙x = 0,     p˙y = 0,
(25)

and

˙qx = − px,    q˙y = − py.
(26)

Therefore the velocity multipliers are affine functions of time.

PIC

Figure 5. The crucial mathematical simplification behind linear tangent steering. In the flat-Earth constant-gravity variational model, position costates are constant and velocity costates are affine in time. Stationarity aligns thrust with the velocity-costate vector.

16 Why a tangent becomes linear

Suppose the final downrange position is free.

The corresponding transversality condition gives

px = 0.
(27)

Then

qx = C
(28)

is constant, while

qy = A +  Bt.
(29)

Stationarity with respect to thrust direction gives

     [   ]
       qx
uT  ∥  qy .
(30)

Hence

tan 𝜃(t) =  qy=  A  + B  t.
           qx    0     0
(31)

This is the linear tangent steering law.

The angle itself is not linear.

Its tangent is.

PIC

Figure 6. Linear tangent steering. The variational solution gives a thrust-direction law of the form tan 𝜃 = A + Bt  under the simplified model and appropriate terminal freedom. Saturn guidance used this optimal-law structure rather than solving the full variational boundary-value problem onboard.

17 If both endpoint coordinates are constrained

If the downrange terminal coordinate is also constrained, then generally

px ⁄= 0.
(32)

Both

qx
(33)

and

qy
(34)

are affine in time.

The steering law then has the more general form

           A + Bt
tan 𝜃(t) = -------.
           C + Dt
(35)

This later appears naturally in generalized linear-tangent and powered-explicit guidance formulations.

The simpler Saturn IGM structure can be understood as exploiting a special but highly useful variational result.

18 From the optimal law to IGM

The key engineering insight was:

  • do not integrate a full calculus-of-variations boundary-value problem onboard; use the shape of its optimal steering law and solve only for the coefficients needed to hit the target.

The Iterative Guidance Mode repeatedly:

  1. read the current navigation state,
  2. estimate time-to-go,
  3. evaluate stage performance integrals,
  4. solve for steering-law parameters,
  5. predict terminal position and velocity,
  6. update the steering command,
  7. repeat.

PIC

Figure 7. Conceptual IGM loop. The variational calculation supplies the steering-law form. The onboard digital computer repeatedly updates the law’s coefficients from the measured state, stage performance, and desired terminal conditions.

19 Why it was called iterative

The vehicle did not receive one fixed steering program and blindly follow it.

IGM continually recalculated quantities such as:

  • time remaining to cutoff,
  • steering coefficients,
  • stage integrals,
  • terminal-state predictions.

Each cycle used the current measured state.

This made IGM path adaptive.

A disturbed Saturn did not have to return to exactly the same geometric path that an undisturbed Saturn would have flown.

It could instead fly a new near-optimal path from its current state to the desired terminal conditions.

20 IGM was variational in origin, not a full variational solver onboard

This distinction resolves an apparent contradiction in historical descriptions.

Some descriptions say IGM was based on calculus of variations.

Others emphasize that IGM itself did not numerically solve a full calculus-of-variations problem during flight.

Both statements can be correct.

The full realistic optimum problem was too computationally demanding for the Saturn onboard computer.

The simplified variational problem supplied the steering-law structure.

IGM then solved an iterative guidance problem within that structure.

The relationship is better read as a sequence of engineering steps:

  • calculus of variations supplies the structure of an optimal steering law,
  • that structure is simplified into a form suitable for flight computation,
  • the onboard guidance system repeatedly solves for the coefficients needed to satisfy the terminal conditions.

21 The Marshall guidance team

Baker’s 1965 account credited the Saturn iterative-guidance development primarily to Helmut J. Horn and his associates in the Dynamics Analysis and Flight Mechanics organization at Marshall.

Later accounts also identify important work by:

  • Daniel T. Martin,
  • Isaac E. Smith,
  • Judson J. Hart,
  • Clyde D. Baker,
  • later Roland Jaggers in the evolution toward Linear Tangent Guidance.

This was a team development rather than the work of one isolated mathematician.

22 The Army-to-NASA continuity

The organizational transition from ABMA to Marshall preserved deep practical experience in:

  • inertial navigation,
  • missile control,
  • analog simulation,
  • flight testing,
  • trajectory design.

What changed was the mission.

Army ballistic missiles had emphasized reliable delivery along a mission-specific trajectory.

Saturn had to maximize payload and meet orbital or translunar terminal conditions despite dispersions.

The combination of:

  • Army missile experience,
  • variational trajectory theory,
  • digital computers

made path-adaptive guidance practical.

23 Saturn V and Apollo

IGM belonged to the Saturn launch vehicle guidance system.

It should not be confused with the guidance equations executed by the Apollo spacecraft computer after separation.

Nevertheless, during an Apollo launch, Saturn IGM was the launch-vehicle guidance method responsible for steering the upper stages toward required orbital or translunar conditions.

Thus the phrase “Apollo IGM” is useful informally only if one remembers that IGM was a Saturn function within the Apollo launch stack.

24 A dramatic test: AS-502

The value of path-adaptive guidance was demonstrated by flight anomalies.

During Saturn V flight AS-502, the Apollo 6 mission, two S-II stage engines were lost during powered flight.

NASA’s later guidance-system review reported that IGM still brought the vehicle close to the required altitude constraint even though the original implementation had been designed around a less severe engine-out case.

This is precisely the kind of situation in which a path-adaptive law is more useful than simply forcing the vehicle back toward one nominal path.

25 The first-stage limitation

Saturn did not apply the same optimum vacuum guidance law from liftoff.

During the high-dynamic-pressure part of first-stage flight:

  • aerodynamic loads mattered strongly,
  • angle of attack had to remain small,
  • structural bending and heating imposed constraints.

A programmed tilt trajectory was therefore used during the early atmospheric phase.

Closed-loop iterative guidance became most natural after the vehicle had left the severe atmospheric-load region.

This also illustrates a general principle:

  • An optimal law derived for one model is not automatically optimal when the neglected physics becomes important.

26 What calculus of variations actually contributed

The calculus of variations did not contribute just one formula.

It contributed a way to think.

The change in viewpoint can be stated as two questions:

  • Forward simulation: What trajectory will this prescribed steering program produce?
  • Trajectory optimization: What steering program extremizes payload, fuel, time, altitude, or another mission objective while satisfying the equations of motion and terminal constraints?

That reversal is the conceptual foundation of trajectory optimization.

PIC

Figure 8. The historical role of calculus of variations in rocketry. It began as an analysis problem that Goddard could only approximate, matured into trajectory-optimization theory, and finally supplied simple optimal steering structures that could be embedded in practical digital guidance.

27 The most important historical transition

The deepest transition was not merely a change from analog to digital computation.

It was a change in guidance philosophy:

  • earlier systems emphasized correction back toward a reference path,
  • Saturn-era guidance increasingly emphasized finding a feasible near-optimal path from the measured state to the required target conditions.

Digital computation made that transition practical onboard.

Calculus of variations supplied the mathematical structure.

28 From IGM to later guidance

The story did not stop with Saturn.

The same line of reasoning evolved into:

  • generalized Linear Tangent Guidance,
  • Apollo-era guidance-theory studies,
  • Shuttle Powered Explicit Guidance,
  • later launch-vehicle explicit guidance methods.

Later guidance systems changed models, constraints, and numerical methods.

But the historical pattern remained recognizable:

  1. formulate an optimum trajectory problem,
  2. derive structure from variational or optimal-control theory,
  3. simplify that structure into a form suitable for onboard computation,
  4. update the solution using the measured state.

29 Goddard and IGM side by side

The historical symmetry is striking.

Goddard faced a realistic optimization problem whose rigorous variational solution was beyond the practical mathematics available to him.

He therefore built an approximate method that preserved enough of the physics to answer the engineering question.

Half a century later, Saturn engineers faced a realistic optimization problem whose full variational solution was beyond the practical onboard computation available to them.

They also simplified the problem while preserving the essential optimal structure.

The difference was that the simplified law could now be recomputed repeatedly during flight.

30 A compact mathematical comparison

The two problems can be compared directly:

  • Goddard: choose an ascent history that minimizes the required initial mass or expelled propellant.
  • Saturn vacuum guidance: choose a thrust-direction history that reaches the terminal conditions with near-minimum propellant.

Both are trajectory optimization problems.

Both require choosing a function, not merely one scalar.

Both naturally lead to variational reasoning.

31 Historical cautions

Several oversimplifications should be avoided.

  1. Goddard did not derive Saturn IGM.
  2. The V-2, Redstone, Jupiter, and Pershing did not use Saturn IGM.
  3. Army delta-minimum guidance was not the same as calculus-of-variations optimal guidance.
  4. Saturn IGM did not numerically solve the full rotating-Earth calculus-of-variations problem onboard.
  5. Modern optimal-control versions of the Goddard problem contain later mathematical developments and should not be treated as identical to Goddard’s original 1919 calculation.
  6. IGM was Saturn launch-vehicle guidance used during Apollo missions, not an Apollo spacecraft guidance mode.

These distinctions make the historical connection stronger rather than weaker.

They show how an abstract optimization idea gradually became an engineering method.

32 Study questions

  1. Why does minimizing initial rocket mass require choosing an entire function rather than one number?
  2. In modern notation, identify possible state and control variables in Goddard’s vertical-ascent problem.
  3. Why did Goddard resort to an approximate interval method?
  4. What is the conceptual difference between delta-minimum guidance and path-adaptive guidance?
  5. Why were analog computers naturally associated with early reference-trajectory missile guidance?
  6. What institutional connection linked Army ballistic-missile development to NASA Marshall?
  7. Why was the full optimum Saturn guidance problem unsuitable for direct onboard variational solution?
  8. Starting from the simplified flat-Earth equations, derive
    ˙px = ˙py = 0.
    (36)

  9. Show that free final downrange position implies a constant horizontal velocity costate.
  10. Derive
    tan 𝜃 = A + Bt.
    (37)

  11. Explain why linear tangent steering is an optimal-law structure rather than a complete guidance system.
  12. Explain why IGM is both variational in origin and not a full onboard calculus-of-variations solver.
  13. Why does engine-out capability favor path-adaptive guidance over strict reference-path recovery?
  14. Why was vacuum guidance separated from the high-dynamic-pressure atmospheric phase?
  15. Explain the historical progression from Goddard’s variational problem to LTG and PEG.

33 Summary

In 1916 Goddard explicitly recognized that realistic rocket performance optimization led him into an unsolved calculus-of-variations problem.

His 1919 report posed the minimum-mass ascent as a problem of determining an unknown velocity function

v =  f(s)
(38)

such that the required propellant mass is minimized.

Hamel and later flight-mechanics researchers continued the mathematical development of optimum rocket trajectories.

Meanwhile, practical missile guidance developed through the V-2 and the U.S. Army’s Redstone, Jupiter, and Pershing programs using reference-path concepts such as delta-minimum guidance and analog computation.

The technical core of the Army Ballistic Missile Agency became NASA Marshall in 1960.

At Marshall, the requirements of Saturn and the availability of digital onboard computing encouraged a different guidance philosophy.

Calculus of variations showed that a simplified vacuum, flat-Earth, constant-gravity optimum problem has a steering law of the form

tan 𝜃 = A + Bt.
(39)

Saturn IGM used this kind of variationally derived steering structure inside an iterative, path-adaptive onboard guidance algorithm.

The historical arc is therefore not one of a single equation surviving unchanged for fifty years.

It is the history of an idea:

  • choose the trajectory itself, or a steering function that generates it, so that the mission objective is optimized while the dynamics and terminal constraints are satisfied.

That idea moved from Goddard’s unsolved theoretical obstacle to one of the mathematical foundations of Apollo-era launch guidance.

References

References

[1]   R. H. Goddard, A Method of Reaching Extreme Altitudes, Smithsonian Miscellaneous Collections, Vol. 71, No. 2, Smithsonian Institution, Washington, 1919.

[2]   R. H. Goddard, Proposal to the Smithsonian Institution, September 27, 1916, Smithsonian Institution Archives.

[3]   G. Hamel, A Problem in the Calculus of Variations Related to Rocket Theory, 1927; English translation reproduced in N. A. Rynin, Interplanetary Flight and Communication.

[4]   A. Miele, Flight Mechanics, Volume 1: Theory of Flight Paths, Addison-Wesley, 1962.

[5]   H. Seywald, Optimal Control Problems With Switching Points, NASA Contractor Report 4393, 1991.

[6]   C. D. Baker, Concepts of the Iterative Guidance Law for Saturn Launch Vehicles, in Aero-Astrodynamics Research Review No. 3, NASA TM X-53389, George C. Marshall Space Flight Center, October 15, 1965.

[7]   W. Haeussermann, Description and Performance of the Saturn Launch Vehicle’s Navigation, Guidance, and Control System, NASA TN D-5869, July 1970.

[8]   National Aeronautics and Space Administration, historical materials on Redstone, the Army Ballistic Missile Agency, and the establishment of Marshall Space Flight Center.

[9]   M. Mangad and M. D. Schwartz, Guidance, Flight Mechanics and Trajectory Optimization, Volume 4: The Calculus of Variations and Modern Applications, NASA CR-1003, 1968.


"From Goddard's Unsolved Variational Rocket Problem to Saturn IGM: Calculus of Variations in Rocket Development" is owned by bloftin.
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Also defines:  Goddard variational rocket problem, delta-minimum guidance, linear tangent steering, Iterative Guidance Mode, path-adaptive launch guidance
Keywords:  Robert Goddard, calculus of variations, rocket optimization, Army Ballistic Missile Agency, Redstone, Jupiter, Pershing, Saturn, Apollo, Iterative Guidance Mode, IGM, linear tangent steering, optimal control, launch vehicle guidance

Cross-references: scalar, formula, phase, stack, parameters, vector, magnitude, position, injection, testing, type, concept, computers, acceleration, systems, work, mechanics, program, velocity, drag, thrust, resistance, function, speed, computation, ballistic, algorithm, mass

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 02.30.Xx (Calculus of variations)
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