Constant 1 g acceleration problem

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Discussion Overview

The discussion revolves around the implications of traveling to the Moon under constant 1 g acceleration, addressing both the time required for such a journey and the complexities of fuel consumption in this context. Participants explore kinematic equations, energy requirements, and the effects of changing mass during acceleration.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants inquire about the time it would take to reach the Moon at constant 1 g acceleration, with one suggesting approximately 2 hours and 25 minutes.
  • There is a discussion on how fuel consumption works with constant acceleration, with some arguing that less fuel is needed as the spacecraft loses mass during propulsion.
  • One participant notes that while less force is required as mass decreases, the initial fuel requirements must be significantly high for a fixed payload.
  • Another participant raises a concern about the energy needed for increasing velocity, questioning whether more fuel is required for each increment in speed despite the loss of mass.
  • Participants discuss the relationship between kinetic energy and velocity, with one clarifying that the factor of four applies to the transition from 0 to 2 m/s, not from 1 to 2 m/s.
  • One participant humorously points out that experiencing 1 g acceleration does not equate to moving closer to the Moon.
  • There is a mention of the complexities of power requirements during acceleration, suggesting that more power is needed as speed increases, particularly in the latter stages of a journey.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the specifics of fuel consumption and energy requirements during constant acceleration, indicating multiple competing views and unresolved questions regarding the implications of changing mass and energy dynamics.

Contextual Notes

Participants express varying assumptions about the nature of acceleration, energy, and fuel consumption, highlighting the complexities involved in space travel dynamics. The discussion reflects a range of interpretations of kinematic principles and their application to real-world scenarios.

kelmcguir
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Multipart question:

1) How long would it take to travel to the moon from Earth at a constant 1 g acceleration?

2) How does fuel consumption work with constant 1 g acceleration or acceleration in general? I read that "it doesn't take a constant amount of energy to maintain a constant acceleration...it takes twice as much energy to go from 1 to 2 m/s as it does to go from 0 to 1 m/s". Is this true and why?
 
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kelmcguir said:
Multipart question:

1) How long would it take to travel to the moon from Earth at a constant 1 g acceleration?

2) How does fuel consumption work with constant 1 g acceleration or acceleration in general? I read that "it doesn't take a constant amount of energy to maintain a constant acceleration...it takes twice as much energy to go from 1 to 2 m/s as it does to go from 0 to 1 m/s". Is this true and why?

I guess you are not familiar with the basic kinematic equations:
$$x = ut + \frac 1 2 at^2, \ \ \text{and} \ \ KE = \frac 1 2 mv^2$$
The first tells you how far you have traveled (##x##) in time ##t## with initial velocity ##u## and constant acceleration ##a##. If the initial speed is zero (##u = 0##) then it's just ##x = \frac 1 2 at^2##.

Could you use that to answer 1) for yourself? You could look up the value of ##g## and the distance to the Moon.

The second tells you the kinetic energy (KE) of an object of mass ##m## moving with speed ##v##. You can see that KE increases with the square of the velocity. Hence it takes four times as much energy to go from ##1## to ##2m/s## as it does to go from ##0## to ##1m/s##.

PS Although, in terms of space travel and rocket engines, things are not so simple.
 
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kelmcguir said:
How long would it take to travel to the moon from Earth at a constant 1 g acceleration?
About 2h and 25minutes.

Is that answer satisfying?
 
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kelmcguir said:
2) How does fuel consumption work with constant 1 g acceleration or acceleration in general?

Conventional space travel involves ejecting mass (propellant) out the back of a rocket engine, and you have to carry this mass with you. So a spacecraft would actually use less and less fuel to maintain a constant acceleration since its mass is falling as it expends propellant. Less mass requires less force to accelerate and thus less propellant expenditure.
 
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I guess the ##1\text{g}## here is a coordinate acceleration, because I'm undergoing ##1\text{g}## g-force/proper acceleration right now and I'm not getting any closer to the moon :wink:
 
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kelmcguir said:
1) How long would it take to travel to the moon from Earth at a constant 1 g acceleration?
If the constant 1g is measured by an acceloromter on board, then you never leave the launch pad.
 
Drakkith said:
Conventional space travel involves ejecting mass (propellant) out the back of a rocket engine, and you have to carry this mass with you. So a spacecraft would actually use less and less fuel to maintain a constant acceleration since its mass is falling as it expends propellant. Less mass requires less force to accelerate and thus less propellant expenditure.
Well, there is good news and bad news. The good news is that it takes less and less force as you burn fuel. The bad news is that for a fixed payload, you need to have started with an exponentially large tank full.
 
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jbriggs444 said:
Well, there is good news and bad news. The good news is that it takes less and less force as you burn fuel. The bad news is that for a fixed payload, you need to have started with an exponentially large tank full.
The really bad news is that you'll crash into the Moon at about ##90,000m/s##.
 
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Drakkith said:
Conventional space travel involves ejecting mass (propellant) out the back of a rocket engine, and you have to carry this mass with you. So a spacecraft would actually use less and less fuel to maintain a constant acceleration since its mass is falling as it expends propellant. Less mass requires less force to accelerate and thus less propellant expenditure.

But PeroK made an interesting point above. "The second tells you the kinetic energy (KE) of an object of mass m moving with speed v. You can see that KE increases with the square of the velocity. Hence it takes four times as much energy to go from 1 to 2m/s as it does to go from 0 to 1m/s." So, even though you are losing mass, wouldn't you still need more fuel for every increase in velocity gained during the acceleration because more energy is required for every step in velocity increase ?
 
  • #10
kelmcguir said:
But PeroK made an interesting point above. "The second tells you the kinetic energy (KE) of an object of mass m moving with speed v. You can see that KE increases with the square of the velocity. Hence it takes four times as much energy to go from 1 to 2m/s as it does to go from 0 to 1m/s." So, even though you are losing mass, wouldn't you still need more fuel for every increase in velocity gained during the acceleration because more energy is required for every step in velocity increase ?
That's for a fixed mass. If you start ejecting mass and reducing the mass of the object you call your rocket, then it's not so simple.
 
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kelmcguir said:
2) How does fuel consumption work with constant 1 g acceleration or acceleration in general? I read that "it doesn't take a constant amount of energy to maintain a constant acceleration...it takes twice as much energy to go from 1 to 2 m/s as it does to go from 0 to 1 m/s". Is this true and why?
You are missing the concept of power somewhere. Let's imagine you are driving a car with negligible resistance (aerodynamic drag & rolling resistance) and with negligible fuel mass with respect to the car mass ##m##. The car is going from point A to point B, separated by a distance ##x##, at a constant acceleration ##a## and the trip lasts 60 minutes in total.

How much energy is required for the trip? That would be based on the required work:
$$E = max$$
Time, thus speed, has no say in this. Twice the acceleration means twice the required energy. And twice the distance traveled means twice the energy needed too. So half-way on our trip we spent half of our energy (i.e. fuel):
$$E_{@x_{\frac{1}{2}}} = ma\frac{x}{2}$$
But how much time does it take to travel half-way? We know it takes 60 minutes for the total trip, so this holds up:
$$t = \sqrt{\frac{2x}{a}}$$
and half-way, it will be:
$$t_1 = \sqrt{\frac{2\frac{x}{2}}{a}} = \sqrt{\frac{x}{a}} = \frac{t}{\sqrt{2}}$$
If ##t## is 60 minutes, then it will take 42 minutes to travel the first half (##t_1##) and 17 minutes to travel the second half (##t - t_1##). This is true because during the second half we are driving a lot faster.

What is not constant throughout our trip is the power ##P## needed which, for a certain period of time, averages to:
$$P = \frac{E}{t}$$
For both halves of the trip, we have the same value for ##E##. But the time elapsed is different:
$$\frac{P_2}{P_1} = \frac{t_1}{t - t_1} = \frac{1}{\frac{t}{t_1} - 1} = \frac{1}{\sqrt{2} - 1} = 2.4$$
So, if you need, say, 100 hp on average during the first half of the trip, you will need an engine producing 240 hp on average during the second half of the trip. Of course, the actual power requirement is totally dependent on the speed of the car (##P = \frac{ma\Delta x}{\Delta t} = mav##).

In conclusion, distance-wise, you will need as much fuel to travel the first meter of the trip as for traveling the last one. But time-wise, you will need a lot more fuel to travel the last minute of the trip compared to what you will need for the first minute of your trip.
 
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  • #12
PeroK said:
The second tells you the kinetic energy (KE) of an object of mass ##m## moving with speed ##v##. You can see that KE increases with the square of the velocity. Hence it takes four times as much energy to go from ##1## to ##2m/s## as it does to go from ##0## to ##1m/s##.
Not to be nit-picky, but can we agree the factor of four would apply to going from zero m/s to 2 m/s, vs. 0 to 1 m/s?
:-)
 
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