What is the equation for the velocity of a rocket as a function of time?

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The discussion focuses on deriving the velocity of a rocket as a function of time, starting from the conservation of momentum principles. The key equations involve the relationship between the rocket's mass, the mass of fuel burned, and the exhaust velocity. Participants express confusion about the transition from momentum equations to the final velocity equation, particularly regarding the integration process and the role of constants. The conversation highlights the need for clarity in defining terms and ensuring correct application of calculus in the derivation. Ultimately, the thread emphasizes the importance of understanding the underlying physics and mathematics in rocket propulsion dynamics.
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I am stuck on how my teacher got to the last equation in #4.

Problem Statement:

A 2,000 kg rocket carrying 3000 kg of fuel is drifting in space when it fires its engine. While operating, the rocket engine burns 20 kg of fuel per second and the exhaust gasses leave the rocket at an exhaust velocity of Ve =300 m/s relative to the rocket.

Relative equations:

p = mv

Work done:

1) At some moment while the engine is firing, the rocket has mass M and is moving at velocity v, as is all the fuel it contains. After a short time Δt, the rocket has burned an amount of fuel Δm which leaves the rocket at velocity ve relative to the rocket. Write expressions for the total momentum before Δm is burned and after Δm is exhausted.

pi = MVi
pf = (M - ∆M)(Vi + ∆V) + ∆M(Vi –Ve)

2) Set the two expressions in (1) equal and expand any products of sums and differences.

(M - ∆M)(Vi + ∆V) + ∆M(Vi –Ve) = MVi →
M Vi - Vi∆M + M∆V +∆M∆V + ∆M Vi - ∆MVe = M Vi →
- Vi∆M + M∆V +∆M∆V + ∆M Vi - ∆MVe = 0 →
M∆V +∆M∆V - ∆MVe = 0

3) Delete any terms which are a product of two factors of Δm, Δv in any combination (they will be much smaller than other terms as Δt shrinks to zero).

M∆V +∆M∆V - ∆MVe = 0 →
M∆V - ∆MVe = 0 →
M∆V = ∆MVe

4) Now take a limit as Δt shrinks to zero and integrate from t = 0 to t to find an expression for the velocity of the rocket as a function of time.

M∆V = ∆MVe →

(M∆V)/(M∆t) = (∆MVe)/(M∆t) →

∆V/∆Vt = (∆MVe)/(M∆t) →

∆V/∆Vt = (Ve/M) (∆M/∆t) - Not entirely sure how he came to this or to the next equation:

V = Kt + Vi

5) Integrate from Δm = 0 to 3000 kg (t= 0 to [3000 kg/20kg/s]). to find the change in the velocity of the rocket.
 
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Samuelriesterer said:
∆V/∆Vt = (∆MVe)/(M∆t) →

∆V/∆Vt = (Ve/M) (∆M/∆t) - Not entirely sure how he came to this
It's a simple rearrangement of terms:
##\frac{\Delta M V_e}{M \Delta t} =
\frac{V_e \Delta M }{M \Delta t}= \frac{V_e}{M} \frac{\Delta M }{ \Delta t}##
But don't you mean
##\frac{\Delta V}{ \Delta t} = \frac{V_e}{M} \frac{\Delta M }{ \Delta t}##?
Samuelriesterer said:
or to the next equation:
V = Kt + Vi
Are you sure you've quoted that correctly? What is K here? That equation looks like uniform acceleration, which is not what will happen.
 
Sorry, the K I believe is a constant
 
Samuelriesterer said:
Sorry, the K I believe is a constant
Well, as I said, that'd be wrong.
You have ##
\frac{d V}{d t} = \frac{V_e}{M} \frac{d M }{d t}##
What do you get by integrating that?
 
##tV + C = (tVe)/(M) + C## ?
 
Samuelriesterer said:
##tV + C = (tVe)/(M) + C## ?
No. You have
##\int \frac{d V}{d t}dt = \int \frac{V_e}{M} \frac{d M }{d t}dt##
Simplify both sides.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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