2
$\begingroup$

I am confused about Newton's 3rd Law. If a person jumps off the ground a force is applied both to the person and to the ground. However, as $F=ma$ acceleration experienced by the Earth is much less than that experienced by the person.

But: I press with gravitation force on the ground so it should press with the same force on me, so if my mass is less than earth mass my acceleration should be greater as well but I am not moving (flying)?

Second: If small rocket(with small mass) pressure against bigger rock with greater mass the rocket should have greater acceleration towards direction opposite to its flying path so how the rocket can actually move the rock(towards left at picture where rock acceleration is small) and not the opposite(rocket acceleration at picture towards right is bigger)?
Edited
If a rocket with mass $m_{rocket}$ pushes against a rock with mass $m_{rock}$ with force $F_{thrust}$ the rock will push back with equal force (Newton's 3rd Law). The rocket will experience an acceleration $a_{rocket}$ in the opposite direction of $F_{thrust}$ and the rock will experience $a_{rock}$ in the same direction as the thrust. However, in this example $m_{rocket} < m_{rock} \therefore a_{rocket} < a_{rock}$
Why doesn't the rocket move in the opposite direction of $F_{thrust}$ since the rock has a greater mass?

enter image description here

Not sure if it helps but added picture to second question

Edit:To put second question simple how a small(low mass) object can push big(great mass) object if according to newton 3rd law a big mass object causes greater acceleration on small mass object

$\endgroup$
1

4 Answers 4

1
$\begingroup$

To the first question: Newton's third law states that every force has an equal and opposite force. Thus, the force that Earth exerts on you with gravity (a big mass causing a huge acceleration on a small mass) is countered exactly by the normal force of the ground (again, a big mass causeing a huge acceleration on a small mass, but this time in the opposite direction). You can see this when you jump, and the normal force is no longer applied to your body, you quickly fall to Earth. In a sense, the force the ground pushes back on you is really equal and opposite to the gravity of the Earth pulling on you.

I'm not sure I understand your second question. It doesn't really specific the situation well, and it's poorly worded; if you rephrase it I can hopefully give you answer.

$\endgroup$
1
  • $\begingroup$ I think his second question has to do with the conservation of momentum and perhaps vectors? $\endgroup$ Commented Jun 26, 2014 at 4:47
1
$\begingroup$

Assume the rocket has enough fuel to power it for an extended period of time.

The rocket pushes against the rock with a force (as long as it has fuel).
Let's call it $F_{thrust}$ and it will have direction "forward".

The rock pushes back with equal force (Newton's 3rd Law). In the question you specify that the rocket has less mass than the rock, so $m_{rocket} < m_{rock}$. Both objects experience $F_{thrust}$, but the rock experiences it in the "forward" direction whereas the rocket experiences the force in the "backwards" direction.

Even though the rock applies a force on the rocket, it still has non-zero acceleration in the "forwards" direction. Therefore it will move "forward". The rocket also has non-zero acceleration in the "backwards" direction. The rocket has a "backwards" acceleration which is greater than the "forward" acceleration of the rock (because $F=ma$). However, the rocket is still applying $F_{thrust}$, so this cancels out with the "backwards" force and the rocket moves "forwards". Now the rock has moved and the rocket is moving. This repeats itself until some force (e.g. friction, air resistance, etc) is greater than or equal to $F_{thrust}$ and the rock no longer moves. Obviously if the rocket runs out of fuel $F_{thrust}=0$ and the neither the rocket nor the rock will move (unless they're found in a vaccuum in which case momentum will keep them moving until something stops them).

In conclusion, it goes like this:
The rocket pushes against the rock. The rock pushes back but moves because the force of the rocket is (making an assumption here) greater than whatever is holding it still (e.g. friction, air resistance, etc). The rocket should move back because the rock applied a force on it, but it using fuel to generate thrust over an extended period of time. Therefore the force it received from the rock is cancelled out and the rocket moves forward again. The rock has moved so the rocket has space to move forwards. When the rocket and the rock meet again, this process repeats itself.

$\endgroup$
1
$\begingroup$

OP's first question has been answered by @jhobbie. Specifically, we sometimes do fly (jump)! This is when the normal force does exceed our weight - gravitational force of attraction towards Earth.

Regarding second question:

The force on rock is NOT always equal to $F_{Thrust}$. The diagram should look like this:

$N \leftarrow [\text{Rock}] \quad$ for the rock,

$ N \rightarrow [\text{Rocket}] \leftarrow F_{Thrust} \quad$ for the rocket,

and $\,F_{Thrust} \rightarrow [\text{Exhaust Gas}]\quad$ (one should not forget this).

So, in OP's notation of acceleration (i'm keeping the direction as mentioned through arrows in original question diagram):

$\vec{\alpha_1} = \dfrac{\vec{F_{Thrust}} - \vec{N}}{m_{rocket}}\quad $ and $\quad\vec{\alpha_2}=\dfrac{\vec{N}}{M_{Rock}}$.

Going over the laws of total energy conservation (if collision is ellastic) and conservation of total momentum will easily show that everything is all right.

Here $N$ is the normal force of reaction between Rock and Rocket; OP's $F_{AB}=-F_{BA}$ is actually this normal force $N$. $F_{Thrust}$ is the force given by the exhaust gas on rocket. Newton's (3rd) law does not demand $F_{Thrust} = N$. One can always study various limits of the masses, like $M_{Rock} \rightarrow \infty$ corresponds to a wall. There $F_{Thrust} = N$, as the rocket will try to push the wall which however does not budge, and rocket will not move forward. Typically, for a ball, where there is no $F_{Thrust}$, the $N$ will result in the thrown ball bouncing back to one's hand, bouncing off the wall.

$\endgroup$
5
  • $\begingroup$ I think my mistake was from thinking that if rocket pressure with certain force there is equal force and nothing more against it but it seems there are actually 3 forces: FThrust cause Normal(N) force on rock and second Normal(N) force that is reaction from newton's 3rd law. So newton's 3rd law only applies to the same kind of forces and here we have N->rocket=N<-rock so there are equal but reaction force is different from thrust force(N->rocket!=Fthrust) am I right? What Forces would we have when I threw a rock? $\endgroup$
    – user82115
    Commented Jun 26, 2014 at 16:10
  • $\begingroup$ In the second instance (N->rocket!=Fthrust), observe that F_Thrust and N are acting at different surfaces. So, one needs to invoke the third law twice, for two different interactions. Basically, the third law holds separately for all the different interactions happening within systems. $\endgroup$
    – mildmay
    Commented Jun 27, 2014 at 8:30
  • $\begingroup$ If I know value of F_thrust can I determine (and how?) value of N->rocket ? (in the case I can't what other information I need?) $\endgroup$
    – user82115
    Commented Jun 27, 2014 at 17:53
  • $\begingroup$ It will depend on type of collision and the forces operating between the rocket and rock. $\endgroup$
    – mildmay
    Commented Jun 30, 2014 at 7:02
  • $\begingroup$ For example, a mass of clay thrown at a wall will stick to it, while an ball of same mass and same initial velocity may rebound from the wall. Knowing the time taken for collision and final velocities etc. might give you an idea of the average force that may have operated during the collision. $\endgroup$
    – mildmay
    Commented Jun 30, 2014 at 7:09
0
$\begingroup$

If small rocket(with small mass) pressure against bigger rock with greater mass the rocket should have greater acceleration towards direction opposite to its flying path so how the rocket can actually move the rock(towards left at picture where rock acceleration is small) and not the opposite(rocket acceleration at picture towards right is bigger)?

The confusion in the second depends on the first question and on your sketch, enter image description here

your knickers are twisted! , if you wand to apply Newton's law the rocket must push the rocket with its jet:

enter image description here

in this way the momentum of the rock (R) can equal the momentum of the rocket (r): $$m_r*v_r = m_R*v_R$$

and, since the mass of the Rock is bigger, its acceleration will be smaller

$\endgroup$

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service and acknowledge you have read our privacy policy.

Not the answer you're looking for? Browse other questions tagged or ask your own question.