GFreeman64
- 4
- 0
Hello everyone,
This is my first time in Physics forums so forgive me if I stray from the convention for asking questions. Me and a friend are completely stumped on our first assignment for the year and we are not sure where else to turn!
A particle of mass m can move in a straight line. The only force acting on the particle opposes its motion, and depends only on its speed. The time T taken for the particle to come to rest after it is set into motion with speed u is given by the formula T=klog(1+au) for all u, where k and a are positive constants. Find the force acting on the particle during the interval 0\leq t\leq T as a function of its speed v. Find also the distance the particle travels in time T.
Hint: Recall that the first fundamental theorem of calculus states that \frac{\mathrm{d} }{\mathrm{d} x} \int_{a}^{x}f(w)dw=f(x).
T=klog(1+au), \frac{\mathrm{d} }{\mathrm{d} x}, \int_{a}^{x}f(w)dw=f(x)
F(v)=m\frac{\mathrm{d}v }{\mathrm{d} t}
As far as I can see the best thing to do is take Newton's second law stated above, and separate the variables to give:
m\int \frac{dv}{F(v)}=\int_{0}^{T}dt
Which would give simply T on the RHS, so substituting for T would give:
m\int \frac{dv}{F(v)}=klog(1+au)
Now I am not sure how to proceed. I am tempted to try and take F(v) out of the integral to the other side of the equation, but I'm not sure whether this is allowed:
m\int \frac{dv}{klog(1+au)}=F(v)
If so, then my answer would simply be \frac{mv}{klog(1+au)}=F(v). Any ideas as if this is correct?
For the second part I think I need to modify our starting point with Newton's second law to say:
mv\frac{\mathrm{d} v}{\mathrm{d} x}=F(v)
But after that I am a bit lost. If I have the equation for F(v) perhaps I can separate variables again and then express v as dx/dt and integrate again. Unfortunately i cannot see far enough ahead to see how this would work.
Thanks everyone in advance for taking a look at this!
This is my first time in Physics forums so forgive me if I stray from the convention for asking questions. Me and a friend are completely stumped on our first assignment for the year and we are not sure where else to turn!
Homework Statement
A particle of mass m can move in a straight line. The only force acting on the particle opposes its motion, and depends only on its speed. The time T taken for the particle to come to rest after it is set into motion with speed u is given by the formula T=klog(1+au) for all u, where k and a are positive constants. Find the force acting on the particle during the interval 0\leq t\leq T as a function of its speed v. Find also the distance the particle travels in time T.
Hint: Recall that the first fundamental theorem of calculus states that \frac{\mathrm{d} }{\mathrm{d} x} \int_{a}^{x}f(w)dw=f(x).
Homework Equations
T=klog(1+au), \frac{\mathrm{d} }{\mathrm{d} x}, \int_{a}^{x}f(w)dw=f(x)
F(v)=m\frac{\mathrm{d}v }{\mathrm{d} t}
The Attempt at a Solution
As far as I can see the best thing to do is take Newton's second law stated above, and separate the variables to give:
m\int \frac{dv}{F(v)}=\int_{0}^{T}dt
Which would give simply T on the RHS, so substituting for T would give:
m\int \frac{dv}{F(v)}=klog(1+au)
Now I am not sure how to proceed. I am tempted to try and take F(v) out of the integral to the other side of the equation, but I'm not sure whether this is allowed:
m\int \frac{dv}{klog(1+au)}=F(v)
If so, then my answer would simply be \frac{mv}{klog(1+au)}=F(v). Any ideas as if this is correct?
For the second part I think I need to modify our starting point with Newton's second law to say:
mv\frac{\mathrm{d} v}{\mathrm{d} x}=F(v)
But after that I am a bit lost. If I have the equation for F(v) perhaps I can separate variables again and then express v as dx/dt and integrate again. Unfortunately i cannot see far enough ahead to see how this would work.
Thanks everyone in advance for taking a look at this!