A 300 kg crate is dropped vertically onto a conveyor belt that is moving at 1.20
m/s. A motor maintains the belt’s constant speed. The belt initially slides under
the crate, with a coefficient of friction of 0.400. After a short time, the crate is
moving at the speed of the belt. During the period in which the crate is being
accelerated, find the work done by the motor which drives the belt.
This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try
refreshing the page, (b) enabling javascript if it is disabled on your browser and,
finally, (c)
loading the
non-javascript version of this page
. We're sorry about the hassle.
Nice explanation thumbs up for you.
That was really a great thinking bro!
i got 216 only half of your answer
I solved it this way. Though it has been a long time since I had solved some mechanics, so I don't know whether my solution is logically right or wrong. I leave it to you to judge it.
When the block touches the bed, the frictional force acting on the block will be f=300 10 0.4=1200; Now we don't know the time for which the slipping took place. Therefore, by Impulse-momentum principle we have f t=m v-m u here f=1200N,u=0, m=300 and v=1.2; therefore t=0.3 sec; Now power of the motor will be P= F.v=1200 1.2=1440 W Therefore, work of the motor will be W=P . t = 1440*0.3 = 432J
Yes,its correct only there are few assumptions to keep in mind. the most imp one is that the block is dropped from a height that tends to zero
@Shivam Singh Does that assumption make a lot of difference? What it it?
@Pranjal Bhor Those assumptions make the solution easy or else...it would be much more tough...;)
The acceleration of the block is μ g . Since v f = v 0 + a t , we solve for t . The distance travelled is equal the velocity of the belt times time: d = μ g v b e l t 2 . W = F f ⋅ d W = μ m g μ g v b e l t 2 W = m v b e l t 2 Plug in the values to get 432 Joules.
where does the 2 go...in your newtons third equation
Problem Loading...
Note Loading...
Set Loading...
I have 2 methods, i would state the 2nd one, which is very simple and conceptual.
Concept: Whatever the work belt did, it must have gone somewhere, where?? Ans: To increase the kinetic energy of the block and some lost in friction, while the time the block was slipping
In ground frame the energy gained is the energy the block attains finally. In the frame of belt friction does its work on the block, the work energy equivalence holds so in belt frame the initial velocity of the block in not zero(find the relative velocity) initially but finally it gets to zero(same as that of the belt so relative zero), the work done is used up in taking away that energy..
We can work out the amount of energy involved in each case 1. In the ground frame, the block starts at rest and eventually moves at speed v. The kinetic energy gained is 1/2 m(v^2) 2. By moving to the frame of the conveyor belt, we can find the amount of energy lost to friction. In that frame, the block originally has energy v and then slows down to rest, with all the original energy dissipated to friction. In total, the energy lost to friction is 1/2 m (v^2) The total work down by the belt is then 2* 1/2 *m *(v^2) 432J