Multiple Choice Kinematics Problem

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Vibhor
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Homework Statement



attachment.php?attachmentid=71151&stc=1&d=1404893091.gif


Homework Equations





The Attempt at a Solution




## α = v\frac{dv}{ds} ## and K is the kinetic energy .


In all the four cases ## α = v\frac{dv}{ds} = mgsinθ ## where θ is the angle which the normal to the body makes with the vertical .

Fig 1) K increases and tangential acceleration α decreases ,so matches with P)

Fig 2) K decreases and tangential acceleration α also decreases ,so matches with S)

Fig 3) K increases and tangential acceleration α also increases ,so matches with R)

Fig 4) K decreases and tangential acceleration α increases ,so matches with Q)

According to me the correct option is (C)

Is this the correct option ?

Many thanks
 

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Vibhor said:

Homework Statement



attachment.php?attachmentid=71151&stc=1&d=1404893091.gif


Homework Equations





The Attempt at a Solution




## α = v\frac{dv}{ds} ## and K is the kinetic energy .


In all the four cases ## α = v\frac{dv}{ds} = mgsinθ ## where θ is the angle which the normal to the body makes with the vertical .
I think you accidentally added an [itex]m[/itex] in there that doesn't belong.

Fig 1) K increases and tangential acceleration α decreases ,so matches with P)

Fig 2) K decreases and tangential acceleration α also decreases ,so matches with S)

Fig 3) K increases and tangential acceleration α also increases ,so matches with R)

Fig 4) K decreases and tangential acceleration α increases ,so matches with Q)

According to me the correct option is (C)

Is this the correct option ?

Yes, your choice looks correct to me. :approve:

In case you missed it though, there is another way to express the [itex]\alpha = v \frac{dv}{ds}[/itex]. Can you represent [itex]v[/itex] in terms of [itex]ds[/itex] and [itex]dt[/itex]? if so, replace [itex]v[/itex] with that in your equation and see what happens. It should then be quite clear why the [itex]g \sin \theta[/itex] makes perfect sense. :wink:
 
collinsmark said:
Yes, your choice looks correct to me. :approve:

Thanks :)

collinsmark said:
In case you missed it though, there is another way to express the [itex]\alpha = v \frac{dv}{ds}[/itex]. Can you represent [itex]v[/itex] in terms of [itex]ds[/itex] and [itex]dt[/itex]? if so, replace [itex]v[/itex] with that in your equation and see what happens. It should then be quite clear why the [itex]g \sin \theta[/itex] makes perfect sense. :wink:

[itex]v = \frac{ds} {dt}[/itex] and [itex]α = \frac{dv}{dt}[/itex] which is the tangential acceleration .

Is this what you are suggesting ?
 
Vibhor said:
[itex]v = \frac{ds} {dt}[/itex] and [itex]α = \frac{dv}{dt}[/itex] which is the tangential acceleration .

Is this what you are suggesting ?

That's it. :smile: It was just to point out that [itex]\alpha[/itex] is the ball's acceleration.
 
And yes, just to avoid ambiguity, [itex]\alpha[/itex] is the tangential component of acceleration, as you have correctly suggested. :smile: (There's also a normal component, but that's not relevant for this problem.)