Impulsive delta v hyperbolic and elliptical orbit

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Homework Help Overview

The problem involves calculating the impulsive ΔV required for the Cassini spacecraft to transition from a hyperbolic trajectory to an elliptical orbit around Saturn. The spacecraft approaches Saturn with a hyperbolic excess velocity of 5.5 km/s and is to be captured into a 116-day elliptical orbit with a periapsis distance of 80,680 km.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the physical meaning of hyperbolic excess velocity and its implications for the spacecraft's total energy. Questions arise about the relationship between the given excess velocity and the conditions for capture by Saturn's gravity.
  • Some participants attempt to derive orbital parameters using equations related to orbital mechanics, such as the semi-major axis and eccentricity, while expressing uncertainty about the initial approach and the interpretation of the velocity terms.
  • There is a focus on energy equations and how they relate to the spacecraft's velocity at periapsis, with participants seeking clarification on the correct application of these concepts.

Discussion Status

The discussion is active, with participants exploring different interpretations of the problem and engaging in mathematical reasoning. Some guidance has been offered regarding the understanding of hyperbolic excess velocity and its implications for energy calculations. There is no explicit consensus yet, as participants continue to clarify their approaches and assumptions.

Contextual Notes

Participants are navigating through the complexities of orbital mechanics, including the definitions of hyperbolic and elliptical orbits, and the implications of energy conservation in the context of the problem. There is an acknowledgment of potential confusion regarding the definitions and calculations involved.

orbitsnerd
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Homework Statement


On July 1, 2004, the Cassini spacecraft approached
Saturn with hyperbolic excess velocity 5.5 km/s to
swing by the planet at the closest approach distance
rp = 80,680 km. Compute the impulsive ΔV
required for a maneuver performed at the closest
approach to Saturn to transfer the Cassini spacecraft
into a 116-day elliptical orbit having the same
periapsis point as the approach (hyperbolic)
trajectory.
rp=80,680 km
vinf=5.5 km/s
T=116 days
GMsaturn=3.7931187e7 km^3/s^2



Homework Equations


vinf=sqrt(GMsaturn/a)



The Attempt at a Solution


I know it is an in-plane maneuver going from a hyperbolic approach to an ecliptic approach. If the vinf=sqrt(GM/a) is correct, I get a=1,253,923 km.
I am pretty much lost on how to complete this problem. I have done previous examples of Hohmann transfers and heliocentric orbits including the various velocities involved. Any help would be appreciated.
Thanks!
 
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Hi orbitsnerd, welcome to PF!:smile:

What does vinf physically represent? Does that really correspond to the value of 5.5km/s excess velocity you are given?

What must be true of the total energy (kinetic plus gravitational potential) of Cassini for it to be captured by Saturn's gravity? If Cassini is traveling at 5.5km/s in excess velocity, doesn't that mean it is traveling 5.5km/s too fast to be captured? What does that tell you it's total energy is? What would its total energy be if it were traveling in a 116 Day elliptical orbit having the same
periapsis point as the approach (hyperbolic)? What is the difference in these two energies? What chance in speed would account for this difference?
 
I was able to begin the problem (so I hope) this way:
T=2Pi sqrt(a^3/mu) where a=299290 km
e=1-(rp/a) so e=.7304
a=ra+rp/2 where ra=517900 km
vp=sqrt((2mu/rp)-(2mu/rp+ra))=28.53 km/s
I am using mu=musaturn=3,7931187e7 km^3/s^2.

Is this this correct initial approach? I am still a bit lost by what you meant by 5.5 km/s not being vinf.

For the energy equation are you referring to the E=(v^2/2)-(mu/r)?
Thanks.
 
orbitsnerd said:
I was able to begin the problem (so I hope) this way:
T=2Pi sqrt(a^3/mu) where a=299290 km
e=1-(rp/a) so e=.7304
a=ra+rp/2 where ra=517900 km
vp=sqrt((2mu/rp)-(2mu/rp+ra))=28.53 km/s
I am using mu=musaturn=3,7931187e7 km^3/s^2.

Is this this correct initial approach?

I haven't checked your numbers, but your approach looks good.:approve:

This tells you what final speed you want the satellite to have at the periapsis point. Now you need to find its initial speed at that point...

I am still a bit lost by what you meant by 5.5 km/s not being vinf.

If I told you that the velocity of the spacecraft was 5.5km/s in excess of 100km/s, would you tell me its velocity was 5.5kms or 105.5km/s?

In this case, the "hyperbolic excess velocity of 5.5km/s" tells you that the spacecraft is traveling 5.5km/s faster than the maximum velocity it could have if it were in a bounded orbit. You'll need to figure out what that maximum velocity is if you want to find the velocity of the spacecraft .

For the energy equation are you referring to the E=(v^2/2)-(mu/r)?
Thanks.

Close, shouldn't the mass of the satellite be in that equation as well?
 

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