Title: Continuous%20Mass%20Flow%20Rockets%208.01%20W08D1
1Continuous Mass Flow Rockets8.01W08D1
2Juno Lift-Off
http//anon.nasa-global.edgesuite.net/HD_downloads
/juno_launch_1080i.wmv
3Todays Reading Assignment W08D1
- Young and Freedman 8.6
- Class Notes Continuous Mass Flow
4Worked Example Stream Bouncing off Wall
- A stream of particles of mass m and separation d
hits a perpendicular surface with speed v. The
stream rebounds along the original line of motion
with the same speed. The mass per unit length of
the incident stream is l m/d. What is the
magnitude of the force on the surface? -
-
5Category 1 Adding Mass But Not Momentum
- There is a transfer of material into the object
but no transfer of momentum in the direction of
motion of the object. Consider for example rain
falling vertically downward into a moving cart. A
small amount of rain has no component of
momentum in the direction of motion of the cart.
6Concept Question
- Suppose rain falls vertically into an open cart
rolling along a straight horizontal track with
negligible friction. As a result of the
accumulating water, the speed of the cart - increases.
- does not change.
- decreases.
- not sure.
- not enough information is given to decide.
7Fire Plane Scooping up Water
8Category 2 Losing Mass But Not Momentum
- The material continually leaves the object but
it does not transport any momentum away from the
object in the direction of motion of the object.
For example, consider an ice skater gliding on
ice holding a bag of sand that is leaking
straight down with respect to the moving skater.
9Category 3 Impulse
- The material continually hits the object
providing an impulse resulting in a transfer of
momentum to the object in the direction of
motion. For example, suppose a fire hose is used
to put out a fire on a boat. The incoming water
continually hits the boat impulsing it forward.
10Category 4 Recoil
- The material continually is ejected from the
object, resulting in a recoil of the object. For
example when fuel is ejected from the back of a
rocket, the rocket recoils forward.
11Rocket Equation
12(No Transcript)
13Worked Example Rocket Motion
- A rocket at time t is moving with speed vr,0 in
the positive x-direction in empty space. The
rocket burns the fuel at a rate dmf,out /dt b gt
0. The fuel is ejected backward with speed u
relative to the rocket. - a) What is the relationship between the time
rate of change of exhaust mass dmf /dt, and the
time rate of change of rocket mass dmr /dt? - b) Find an equation for the rate of change of
the speed of the rocket in terms mr (t) ,u, and
dmr /dt and solve for v. - c) Find the differential equation describing the
motion of the rocket if it is in a constant
gravitational field of magnitude g
14Strategy Rocket Motion
- Goal Determine velocity of rocket as function of
time as mass is continuously ejected at rate dmf
/dt with speed u relative to rocket. - System consider all elements that undergo
momentum change rocket and fuel - Using Momentum flow diagram, apply
- to find differential equation that describes
motion.
15Rocket Motion
- A rocket at time t 0 is moving with speed vr,0
in the positive x-direction in empty space. The
rocket burns the fuel at a rate dmf /dt b gt0.
The fuel is ejected backward with speed u
relative to the rocket. The goal is to find an
equation for the rate of change of the speed of
the rocket in terms mr (t) ,u, and dmr /dt and
solve for v. -
16State at time t
- Rocket with total mass mr(t) moves with speed
vr(t) in positive x-direction according to
observer - 2. Total mass consists of mass of rocket mr,0
and fuel mf (t) - 3. Fuel element with mass ?mf, moves with speed
of rocket vr (t) at time t, is ejected during
interval t, t?t - 4. x-component of momentum at time t
17State at t ?t
- Rocket is propelled forward by ejected fuel with
new rocket speed - Fuel is ejected backward with speed u relative
to rocket. Relative to observers frame, ejected
fuel element has speed - x-component of systems momentum at time t?t
18Rocket Equation
- Are there any external forces at time t? Two
cases - Taking off
-
- (2) Negligible gravitational field
- Apply Momentum Principle
19Rocket Equation Conservation of Mass and Thrust
- Conservation of mass Rate of decrease of mass
of rocket equals rate of ejection of mass -
- Rocket equation
- Fuel Ejection Thrust force
20Solution Rocket Motion in Gravitational Field
- Rocket Equation
- Fuel ejection term can be interpreted as thrust
force - Relative fuel ejection velocity
- External force
- Rocket equation
- Integrate with respect to time
- Solution
21Concept Question Rocket Fuel Burn Time
- When a rocket accelerates in a constant
gravitational field, will it reach a greater
final velocity if the fuel burn time is -
- as fast as possible?
- as slow as possible?
- The final speed is independent of the fuel burn
time? - Im not sure.
22Answer Rocket Equation in Gravitational Field
- Fuel ejection term can be interpreted as thrust
force - Solution shorter the burn time, the greater the
velocity
23Concept Question Rocket with Constant Thrust
- If a rocket in gravity-free outer space has a
constant thrust at all times while burning fuel,
is its acceleration - constant?
- increasing?
- decreasing?
24Table Problem Rocket Sled
- A rocket sled ejects gas backwards at a speed u
relative to the rocket sled. The mass of the fuel
in the rocket sled is equal to one half the
initial total mass mr,0 (including fuel) of the
sled. The rocket sled starts from rest on a
frictionless track. You may ignore air
resistance. - Derive a relation between the differential of
the speed of the rocket sled, dvr , and the
differential of the total mass of the rocket, dmr
- Integrate the above relation to find the speed
of the rocket sled as a function of mass, vr(m),
as the rocket sled speeds up. - What is the final speed of the rocket sled after
all the fuel has been burned? Express your
answers in terms of the quantities u, and mr,0
as needed. - After reaching its final speed, the sled enters a
rough portion of the track that begins at x 0
with a coefficient of kinetic friction that
varies with distance - µk(x)bx where b is a positive constant.
How far D did the sled slide before it came to
rest in that portion of the track? Express your
answers in terms of the quantities u, b, g, and
mr,0 as needed.
25Next Class W08D2Test Two ReviewCircular Motion,
Energy, Momentum, and Collisions
26Next Reading Assignment W09D1
- Young and Freedman 1.10 (Vector Products)
9.1-9.6, 10.5