Will the fire truck stop before running out of water?

[vladimir69]

Homework Statement

A fire department's tanker truck has a total mass of 21000kg, including 15000kg of water. Its brakes fail at the top of a long 3 degree slope and it begins to roll downward, starting from rest. In an attempt to stop the truck, firefighters direct a stream of water parallel to the slope beginning as soon as the truck starts to roll. The water leaves the 6cm diameter hose nozzle at 50m/s. Will the truck stop before it runs out of water? If so, when? If not, what is the minimum speed reached?

Homework Equations

F=ma

F_{net}=\frac{dp}{dt}

\theta=3

The Attempt at a Solution

The rate of loss of mass per second is
\frac{dm}{dt}=50\pi r^2 m^3/s

\frac{dm}{dt}=141 kg/s
So after 15000/141=106 seconds the fire truck will have run out of water.
The only other force acting is gravity. (not sure why friction isn't included)
so
F_{net}=m(t)g\sin\theta-141 \times 50=(21000-141t)g\sin\theta-7050

for 0\leq t\leq 106

Fire truck will stop next when a=0 which occurs at
0=(21000-141t)g\sin\theta-7050

141t=7257

t=51.5s
51.5 < 106

So i say yes the fire truck will stop before it runs out of water
Does my argument sound ok ?

 

[danb]

(not sure why friction isn't included)

Because this is an exercise

Fire truck will stop next when a=0

You mean v=0.

m(t) dv/dt = m(t)g' - v_w dm/dt

where g' = g sin(theta)

You have to integrate to find v(t).

 

[tiny-tim]

Welcome to PF!

Hi danb! Welcome to PF!

Because this is an exercise

Nice one! ​

 

[danb]

Hi danb! Welcome to PF!

Hi tiny-tim, thanks for the welcome

 

[vladimir69]

after having a second look at this problem

F_{net} = \frac{dp}{dt} = ma =m\frac{dv}{dt}=m\frac{dv}{dt}+v\frac{dm}{dt}
this sounds pretty silly but doesn't the m dv/dt cancel from both sides?

moving on
let F= flow rate
M=initial mass of truck and water=21000kg
v_w = velocity of water
initial velocity of truck = 0
F=141kg/s
m(t)=M-Ft
v_w=50
\theta=3

so using Newton we have
m(t) \frac{dv}{dt} = m(t)g\sin\theta-F v_w
\int dv=g\sin\theta\int dt-Fv_w\int \frac{dt}{m(t)}=gt\sin\theta-Fv_w\int \frac{dt}{M-Ft}
v(t)=gt\sin\theta+Fv_w \ln(M-Ft) + C
i can find the constant C by using
v(0)=0
but with the ln(t) and t in the same equation it seems a bit tricky to solve for t when v=0 unless using maple or mathematica
did i go overkill somewhere?

 

[danb]

doesnt the m dv/dt cancel from both sides?

No, it's part of \frac{d}{dt}(mv). F_{net} = \frac{dp}{dt} turns into mg sin \theta = m\frac{dv}{dt}+v\frac{dm}{dt}

 

[danb]

with the ln(t) and t in the same equation it seems a bit tricky to solve for t when v=0

Yea, I'm not sure how the problem can be solved analytically if v goes to zero. I guess you can find v when the water runs out and hope it's positive

 

[tiny-tim]

m(t) \frac{dv}{dt} = m(t)g\sin\theta-F v_w

…
but with the ln(t) and t in the same equation it seems a bit tricky to solve for t when v=0 unless using maple or mathematica
did i go overkill somewhere?

Hi vladimir69!

Since the question asks …

Will the truck stop before it runs out of water? If so, when? If not, what is the minimum speed reached?

… solve for dv/dt = 0 first, and find the speed v then …

if it's positive, and if you've not run out of water, then that's your answer

(only if it's negative do you have a problem with ln(t) )

 

[vladimir69]

ok thanks for the effort guys
greatly appreciated