Aero 319 Flashcards

1
Q

Five assumptions of a circular orbit

A
  1. Small satellite orbits a massive body on a circular orbit
  2. m«M
  3. Acceleration of massive body is negligible
  4. Massive body is spherically symmetrical
  5. The only force acting is Newtonian gravity.
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2
Q

Equation for gravitational force, F

A

GMm/r^2, where r is the distance between the bodies, and G is the universal gravitational constant.

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3
Q

Equation for centripetal acceleration, a

A

(v^2)/r

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4
Q

Period of motion, T

A

2πr/v = 2π*√(r^3/GM), where r is replaced by a, the semi-major axis, for elliptical orbits.

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5
Q

What is µ?

A

GM

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6
Q

Kepler’s three laws

A
  1. The planets orbit the sun on elliptical orbits - the sun is at one of the foci of each planet’s ellipse.
  2. A line drawn between a planet’s centre and the sun’s centre sweeps out an area at a constant rate as the planets orbit.
  3. The ratio of (orbital period)^2/(mean distance from sun)^3 is constant.
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7
Q

Angular velocity, omega

A

2π/T

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8
Q

What do the stars of a binary system orbit?

A

A common centre of mass.

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9
Q

Mass centre equation for binary system circular orbit

A

M1R1 = M2R2, where R1 + R2 = D, the distance between the stars (measured from their centres).

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10
Q

In Keplerian orbits, L/r = 1 + eCostheta. What do L and e represent?

A

L is a length parameter that defines the size of the orbit, and e is the eccentricity.

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11
Q

e = 0

A

Circular orbit

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12
Q

0 < e < 1

A

Elliptical orbit

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13
Q

e = 1

A

Parabola - escape trajectory; orbit no longer closed.

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14
Q

e > 1

A

Hyperbola

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15
Q

Equation for L

A

(h^2)/µ, where h is the specific angular momentum.

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16
Q

When does the minimum value of r occur, and what’s it called.

A

It occurs when theta = 0. It’s called the periapsis.

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17
Q

Gravitational potential per unit mass at r, V(r)

A

-µ/r

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18
Q

Equation for escape velocity, v

A

√(2GM/r)

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19
Q

Tsiolkovsky’s equation

A

∆V = Velnµ, where ∆V is the achievable velocity increment, Ve is the effective exhaust velocity, and µ is the mass ratio.

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20
Q

Mass ratio, µ

A

M0/(M0-mf), where M0 is the total initial mass and mf is the mass of propellant.

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21
Q

Total initial mass, M0

A

mf + ms + mp

22
Q

Effective exhaust velocity, Ve

A

Isp*g0, where Isp is the specific impulse.

23
Q

Structural coefficient

A

ms/(ms + mf)

24
Q

Burnout velocity, Vbo

A

VeLnµ - gtbo, where tbo is the burnout time.

25
Q

Height above launch as a function of burn time, H(tb)

A

((Vetbµ)/(µ-1))(1-(1/µ)(1 + Lnµ)) - 0.5g*tb^2

26
Q

Assuming constant burn rate, burn time, tb

A

((µ-1)Ve)/(µphig0), where phi is the thrust to weight ratio.

27
Q

Total energy, E

A

((M0Ve^2)/µ)[(1/phi)(1-(1/µ)(1+Lnµ)) - 0.5((µ-1)/(µphi))^2 + 0.5(Lnµ - ((µ-1)/(µphi)))^2]

28
Q

Mach, M

A

v/a

29
Q

Gamma

A

cp/cv

30
Q

Conservation of energy

A

h1 + 0.5v1^2 = h2 + 0.5v2^2, where h is enthalpy.

31
Q

Change in enthalpy, ∆h (ideal gas only)

A

cp∆T

32
Q

Isentropic flow

A

Flow is adiabatic and reversible (constant entropy)

33
Q

P/rho^gamma

A

Constant

34
Q

p1/p2

A

(rho1/rho2)^gamma

35
Q

T1/T2

A

(rho1/rho2)^gamma-1 = (p1/p2)^(gamma-1/gamma)

36
Q

Important to note about shockwaves

A

Flow is irreversible, so isentropic relationships can’t be used.

37
Q

Exit velocity formula

A

Ve/a0 = √(2/(gamma-1))(1-(pe/p0)^(gamma-1)/gamma

38
Q

Maximum possible exit plane velocity, Vemax

A

a0*√(2/(gamma-1)) = √(2cpT0)

39
Q

Choked mass flow rate, mdot

A

rho0a0At*(2/(gamma+1))^(gamma + 1)/2(gamma-1))

40
Q

F/mdot*a0

A

Ve/a0 + a0/(gammaVe)(pe/p0 - pb/p0)(pe/p0)^-1/gamma

41
Q

Maximum F/mdot*a0

A

√(2/gamma-1)(1 - (pb/p0)^(gamma-1)/gamma)

42
Q

Rocket motor thrust coefficient, Cf

A

F/p0At = (mdot/p0At)*(Ve + (a0^2/gammaVe)(pe/p0 - pb/p0)(pe/p0)^-1/gamma

43
Q

mdot/p0At

A

(gamma/a0^2)(2/(gamma+1))^(gamma+1)/2(gamma-1)

44
Q

Characteristic velocity, C*

A

p0At/mdot

45
Q

Specific impulse, Isp

A

F/(mdot*g0) = Ve/g0

46
Q

Hohmann transfer

A

Used to transfer a spacecraft from one circular orbit up to a higher circular orbit.

47
Q

How does a Hohmann transfer work?

A

An elliptical transfer using two tangential burns, which are assumed to be impulsive and produce a ∆v that’s tangent to the original orbit.

48
Q

Eccentricity formula

A

(Rmax - Rmin)/(Rmax + Rmin)

49
Q

Semi-major axis formula

A

0.5(Rmax + Rmin)

50
Q

Specific orbital energy formula, E

A

0.5((h/L)^2)(e^2 - 1)

51
Q

Circular orbit orbital velocity, v

A

√(µ/r)