Rocket Net Force: Understanding Internal & External Forces

In summary, the conversation discusses the motion of a rocket emitting exhaust in the opposite direction of its motion. The net external force on the rocket is equal to the change in momentum, which is equal to the thrust minus the momentum of the exhaust. This leads to the equation F_net_ext=0 implying F_net_r=thrust+vdm/dt=udm/dt, which may seem counterintuitive but is consistent with the rocket's acceleration increasing with time. However, this raises the question of whether this equation is correct, as it is not found in textbooks.
  • #1
inkliing
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Some of the following is more or less Halliday & Resnick, 4th Ed., section 9.8 (not the whole section and I added a lot):

Assume motion in a stright line. Therefore, for position, velocity, acceleratiom, force, momentum, etc., d/dt|vector|=|d/dt(vector)|. This is not true in general for motion along a curved path. Assume we have an idealized rocket of mass m and speed |v| at time t traveling in the forward direction relative to an inertial reference frame. The rocket then instantaneously begins to emit a constant stream of exhaust in the backwards direction.

let:
F_net_ext = net external force = net force on (rocket + exhaust) = sum of gravity, atmospheric drag, etc.
F_net_r = net force on the rocket
P = momentum of (rocket + exhaust)
p = momentum of rocket
u = velocity of exhaust (as it leaves the rocket) pointing backwards.
v_rel = velocity of exhaust (as it leaves the rocket) relative to rocket = u - v = vector pointing back and is constant for an idealized rocket.
Note F_net_ext, F_net_r, P, p, v, u, v_rel, dv, a, etc. are all vetors. Their lengths are |vector|.

In time interval dt the rocket emits a mass -dm. Note that dm < 0 and |dm/dt| = constant for an idealized rocket = mass flow rate of exhaust backwards from the rocket. So at time t+dt we now have a bit of exhaust of mass -dm moving backwards with velocity u and the rocket, now of mass m+dm, moving forward at velocity v+dv. Note dv clearly points forward: the rocket's acceleration, a, points forward.

(1) F_net__ext = dP/dt = [1/dt)][(m+dm)(v+dv)+(-dm)u - mv] = mdv/dt + vdm/dt - udm/dt (note (dv)dm/dt ->0 in the limit of the derivative)

This equation is standard for rockets. There are generally 2 ways it is rewritten:

(2) F_net_ext = mdv/dt + vdm/dt - udm/dt = dp/dt - udm/dt
(3) F_net_ext = mdv/dt + vdm/dt - udm/dt = mdv/dt - (u-v)dm/dt = ma - (v_rel)dm/dt

F_net_ext is not the force that propels the rocket. The force that propels the rocket is an internal force within the (rocket+exhaust) system. If F_net_ext = 0 then P remains constant but the rocket experiences a thrust which changes its momentum. The change in p in time dt is equal and opposite to the momentum, udm, carried away by the exhaust. for a rocket (u-v)dm/dt = thrust = (v_rel)dm/dt = forward pointing vector since u-v points back and dm/dt < 0. The thrust is the rate at which momentum enters the rocket. For an idealized rocket with constant v_rel and constant dm/dt, the thrust is a constant.

This is pretty much the extent of Halliday & Resnick on this subject, but every time I read it I'm struck by the seeming inconsistency that thrust is clearly constant yet the rate of change of the rocket's momentum, dp/dt, is not.

I hope you won't mind if I walk you thru my reasoning. By (3), F_net_ext=0 implies ma=thrust. thrust is constant and points forward implies ma is therefore a forward pointing constant vector. ma is constant and m is decreasing with time implies |a| is increasing with time. Therefore as long as thrust exits the rocket backwards, then the rocket will not only accelerate in the forward direction, but the rate at which it accelerates increases with time. dm/dt < 0 and v always points forward implies the term vdm/dt is a backwards pointing vector which is not constant but grows in length as v grows. At time t_0 when the exhaust initially begins to flow back from the rocket, u is a backwards pointing vector of length |v_rel| since v=0. u then shrinks in length as the rocket moves faster, but v_rel remains constant. At some point |v| = |v_rel| and u=0, and after this |v| > |v_rel| and u points forward, tho still shorter than v by |v_rel|. By (2), F_net_ext=0 implies dp/dt = udmdt. dm/dt<0 implies the term udm/dt points forward until |v|>|v_rel|, then it points back. Therefore dp/dt points forward and then, after |v|>|v_rel|, dp/dt points back.

This is one of the major counterintuitive things about rockets that confuses me (and presumably most people, unless my calculations are incorrect). When |v|>|v_rel|, dp/dt of the rocket points back, meaning the net force on the rocket (not F_net_ext) points backwards, opposite the forward motion of the rocket. The momentum of the rocket always points forward in this example, but it's getting shorter at the rate of dp/dt, and tho the net force on the rocket points back after |v| exceeds |v_rel|, nevertheless the rocket not only continues to accelerate forward, but the rate of forward acceleration increases with time!

Many books and websites claim that, in the absence of external forces such as gravity, friction, etc., the net force on a rocket is equal to the thrust. I've even seen this on some NASA websites. But the net force on a rocket does not seem to be equal to the thrust. Assuming F_net_ext = 0 then F_net_r = dp/dt = udm/dt by (2) = udm/dt + vdm/dt - vdm/dt = (u-v)dm/dt + vdm/dt = thrust + vdm/dt. So the net force on a rocket, absent external forces, does not seem to be equal to the thrust, but rather equal to the thrust + vdm/dt.

Hopefully, at this point, you're saying to yourself "what's the problem?" If so, then there probably is no problem. But I'm bothered by the equations:

(4) F_net_ext=0 implies F_net_r = thrust + vdm/dt = u dm/dt

Both equations seem counterintuitive even tho I've reasoned thru the details. It bothers me that many books and websites set F_net_r = thrust + external forces and ignore the vdm/dt term. It makes me wonder whether eqn (4) is correct. I haven't found either of the equations (4) in Halliday & Resnick or Marion & Thornotn's Classical Dynamics or Goldstein's Classical Mechanics, but I haven't found anything in those texts that disputes eqns (4) either.

I would like to know if eqns (4) are correct? Is there something simple here that I'm missing? Thanks in advance.
 
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  • #2
F_net_r = thrust already takes into account vdm/dt. That is how you calculate the thrust. T=dm/dt*v. Where did you get (u-v)dm/dt?
I'm not familiar with rocketry and most of this, so forgive me if I am asking something stupidly simple.

Edit: If F_net_ext is the drag and such on the rocket, I don't follow where your equations 1-4 come into play, especially if we say F_net_ext = 0. If it is zero, then everything else in the equation is 0 too as well correct?
 
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  • #3
Drakkith said:
F_net_r = thrust already takes into account vdm/dt. That is how you calculate the thrust. T=dm/dt*v.

v is the velocity of the rocket, v_rel is the velocity of the exhaust relative to the rocket. Thrust is not dm/dt*v, rather thrust=(v_rel)dm/dt.

Where did you get (u-v)dm/dt?

u-v=v_rel and (u-v)dm/dt=(v_rel)dm/dt=thrust.

If F_net_ext is the drag and such on the rocket, I don't follow where your equations 1-4 come into play, especially if we say F_net_ext = 0. If it is zero, then everything else in the equation is 0 too as well correct?

F_net_ext=0 implies, by (1), mdv/dt+vdm/dt-udm/dt=0, by (2), dp/dt-udm/dt=0, and by (3), ma-(v_rel)dm/dt=0.
 
  • #4
Sorry, I wish I could help! I just don't really understand this well enough.
 
  • #5


I appreciate your thorough analysis and questioning of these equations. It is always important to critically examine and understand the equations we use to describe physical phenomena.

First, let's address the equation F_net_r = thrust + vdm/dt. This equation is correct, as it takes into account the change in momentum of the rocket due to the ejection of exhaust mass. This term, vdm/dt, is often referred to as the "momentum flux" and it represents the change in momentum of the rocket per unit time due to the exhaust mass leaving the rocket. In the absence of external forces, this term must be included in the net force on the rocket.

Now, let's look at the equation F_net_ext = 0 implies F_net_r = thrust + vdm/dt = u dm/dt. This equation is also correct, as it takes into account the fact that in the absence of external forces, the net force on the rocket is equal to the thrust (internal force) plus the momentum flux term. This equation is essentially a restatement of the first equation, but it explicitly states that in the absence of external forces, the net force on the rocket is equal to the thrust.

I understand your concern about the seeming inconsistency of the rate of change of momentum, dp/dt, pointing in the opposite direction of the rocket's motion after a certain point. However, this is simply a result of the fact that the rocket's velocity is increasing while the exhaust velocity is decreasing. This does not violate any physical laws and is a perfectly valid result.

In summary, both equations (4) are correct and are just different ways of expressing the same concept. The key takeaway is that in the absence of external forces, the net force on the rocket is equal to the thrust plus the momentum flux term. I hope this helps clarify any confusion you may have had. Keep questioning and analyzing, that's what being a scientist is all about!
 

FAQ: Rocket Net Force: Understanding Internal & External Forces

1. What is Rocket Net Force and why is it important to understand?

Rocket Net Force is the combination of all the forces acting on a rocket, both internal and external. It is important to understand because it determines the motion and stability of the rocket during launch and flight.

2. What are internal forces in a rocket?

Internal forces in a rocket are the forces that act within the rocket itself, such as the force of the rocket engines, the weight of the rocket, and the force of air resistance inside the rocket's structure.

3. What are external forces in a rocket?

External forces in a rocket are the forces that act on the rocket from the outside, such as gravity, air resistance, and wind. These forces can affect the motion and stability of the rocket during launch and flight.

4. How do internal and external forces affect the trajectory of a rocket?

The combination of internal and external forces determine the net force acting on the rocket, which in turn affects its trajectory. If the net force is greater than the weight of the rocket, it will accelerate upwards. If the net force is less than the weight of the rocket, it will decelerate or fall back to Earth.

5. How can we calculate the net force on a rocket?

The net force on a rocket can be calculated by adding all the internal and external forces acting on it together. This can be done using Newton's Second Law of Motion (F=ma), where the mass of the rocket and its acceleration are known, or by using force diagrams to visually represent the forces acting on the rocket.

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