Newtons second law and kinematics

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Homework Help Overview

The discussion revolves around two physics problems: one involving the kinematics of a rock dropped from a cliff and the other concerning the motion of a box sliding on a surface with friction. The first problem focuses on the time taken for the rock to fall different distances, while the second problem addresses the distance a box slides before coming to rest due to friction.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the kinematic equations relevant to the rock's motion, questioning the setup and assumptions regarding initial velocities and distances. They discuss the implications of starting from rest and the need for multiple equations to solve for unknowns. For the box problem, there is a consideration of constant acceleration and its relation to similar projectile motion problems.

Discussion Status

Some participants have provided insights into the relationships between the variables involved, particularly in the rock problem, suggesting that ratios may simplify the analysis. Others have attempted to derive equations based on the initial conditions and have noted the quadratic nature of the equations involved. The box problem has prompted discussions about determining acceleration and its effects on motion.

Contextual Notes

Participants are working under the constraints of typical homework guidelines, which may limit the amount of direct assistance provided. There are ongoing discussions about the assumptions made in both problems, particularly regarding initial conditions and the effects of forces acting on the objects in motion.

nadinelyab
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1)A rock is dropped off a cliff and falls the first half of the distance into the ground in t1 seconds. If it falls the second half of the distance in t2 seconds, what is the value of t2/t1?

Relevant equations: I think the kinematics equations of d=vt+(1/2)at^2
I have no idea how to solve this please help! I tried to find t1 with the equation above and god t1=sq.rt(d/5) but i don't know if this is right :)

2)a bos of mass m slides on a horizontal surface with initial speed v. I feels no forces other than gravity and the force from the surface. If the coefficient of kinetic friction between the box and the surface is mu how far does the box slide before coming to rest?
Relevant equations: f=ma Ff=Fn*mu,
I basically drew a free body diagram so far

Thanks so much for any help!
 
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1.
You are using correct kinematics equations of d=vt+(1/2)at^2.
As you see here we have 2 unknowns, d and t with v=0
You need 2 equations to solve for unique solution.
 
Well you're asked for a ratio, t1/t2. Whenever you're asked for a ratio, chances are that something will cancel from both the numerator and the denominator. And I suspect this may just be the unknown distance/height the rock travels, d.

The equation for d is correct as azizlwl pointed out, but since the rock starts from rest, initial speed is zero. So you have d=1/2*at^2.

Okay, you go like this:

1. how long does in take for the rock to fall the first half?

\dfrac{d}{2}=\dfrac{gt^2}{2}\quad\Rightarrow\quad t=\sqrt{\dfrac{d}{g}}

and actually this is your t1.

2. how long does it take for the rock to fall down the other half?

You repeat the procedure again but you note that the free fall in the second half of the distance starts with non-zero initial velocity (that's obvious since the rock will have accumulated velocity by the time it is halfway to the ground).

That means the equation for distance traveled is this one now:

\dfrac{d}{2}=\dfrac{gt^2}{2}+v_0t

What's v_0?
 
OK, since there has been no activity here for quite some time, I'll finish this one off just for the fun of it.

Continuing from my previous post, v0 is the initial velocity for the second half of the free fall. It is non-zero and is the same as the final velocity the stone will have accumulated by the time it is halfway to the ground. The first half of the free fall started from rest and continued for t_1=\sqrt{\frac{d}{g}} seconds (see my post above). Then the speed accumulated over this many seconds is,

v_0=gt_1
v_0=g\sqrt{\dfrac{d}{g}}=\sqrt{gd}

Then

\dfrac{d}{2}=\dfrac{gt^2}{2}+\sqrt{gd}t

This is a quadratic equation (with respect to t). Its solution gives us the time t2.

gt^2+2\sqrt{gd}t-d=0
t^2+2\sqrt{\dfrac{d}{g}}t-\dfrac{d}{g}=0
t_{1,2}=-\sqrt{\dfrac{d}{g}}\pm\sqrt{2}\sqrt{\dfrac{d}{g}}

We disregard the negative solution. Then we are left with

t_2=\sqrt{\dfrac{d}{g}}\left(\sqrt{2}-1\right)

Ultimately,

\dfrac{t_2}{t_1}=\sqrt{2}-1
 
The box problem is one of constant acceleration. Determine the acceleration. Since the problem is one of constant acceleration, it is very similar to an object being projected vertically. How high does it go?
 
Last edited:
\frac {1}{2}d=\frac {1}{2}at{_1}^2...(1)
d=\frac {1}{2}a(t_1+t_2)^2...(2)

from (1)
d=at_1^2
sub. in (2)

at_1^2=\frac {1}{2}a(t_1+t_2)^2

2t_1^2=t_1^2+2t_1t_2+t_2^2

t_1^2=2t_1t_2+t_2^2

1=2\frac {t_2}{t_1} +\frac{t_2^2}{t_1^2}

let \ \frac{t_2}{t_1}=x

x^2+2x-1=0

Taking positive root.
x= -1+ √2
 

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