Particle Hanging by a String is Hit from Below by Another Particle

In summary, the problem involves a light elastic string with a natural length of 1m and a particle P with a mass of 4kg suspended from one end. The particle hangs in equilibrium 1.2m below the fixed point O. To find the modulus of elasticity of the string, the force per unit extension (k) can be calculated by considering the initial equilibrium of the particle and using the formula kx = mg. Conservation of energy can then be used to find the value of u, including the potential energy stored in the string. The potential energy of the string can be found using the formula E = (1/2)kx^2. The problem also mentions a particle Q of mass 2kg traveling vertically
  • #1
jmlibunao
16
0

Homework Statement


A light elastic string has a natural length 1 m. One end of the string is attached to the fixed point O and a particle P of mass 4 kg is suspended from the other end of the string. When hanging in equilibrium, P is 1.2 m below O.

#1 Find the modulus of elasticity of the string.

When P is hanging in equilibrium, it is hit from below by a particle Q, of mass 2 kg, which is traveling vertically upwards. Immediately after the impact, P moves vertically upwards with a velocity u m/s. When the string is just taut, P is still moving vertically upwards with a velocity of √10 m/s.

#2 Find the value of u.

Given that Q is moving with a velocity of 4√3 m/s upwards before it hits P,

#3 show that it is momentarily at rest just after impact.

#4 Find the position of the lowest point, with respect to the equilibrium point, reached by P
in the subsequent motion.

Homework Equations


Young's modulus of elasticity (λ)
λ = (F/A)/(ΔL/Lo)
F - force
A - cross sectional area
ΔL - change in length
Lo - original length

g = 10 m/s^2

I'm also guessing you're going to be using the formulas for Conservation of Energy, Ki + Pi = Kf + Pf, right?

I'm not so sure what other equations can be used

The Attempt at a Solution


So the cross sectional area, A, was not given in the problem. I just assigned a variable A for it so my λ = [(4 kg)(10 m/s^2)/A] / [(0.2)/(1)] = 200A

Sadly this is what I can do for now. Still thinking about the rest. Can anyone help?
 
Last edited:
Physics news on Phys.org
  • #2
To find the force per unit extension (k), consider the initial equilibrium of the ball. Write down the f.b.d. and balance the forces to get k. You don't need the young's modulus.

Once you've obtained that, use conservation of energy to find u and also remember to include the potential energy stored in the string in the equation.
 
  • #3
Sunil Simha said:
To find the force per unit extension (k), consider the initial equilibrium of the ball. Write down the f.b.d. and balance the forces to get k. You don't need the young's modulus.

I'm sorry, I don't quite follow this. How would I be able to get the force per unit extension by considering the initial equilibrium? The modulus of elasticity is being asked by the problem.


Sunil Simha said:
Once you've obtained that, use conservation of energy to find u and also remember to include the potential energy stored in the string in the equation.

I can't recall a formula that gives the potential energy when hanging from a string. I can't use P = mgh since height, h, was not given.
 
  • #4
jmlibunao said:
I'm sorry, I don't quite follow this. How would I be able to get the force per unit extension by considering the initial equilibrium? The modulus of elasticity is being asked by the problem.

You see, the original length of the string was 1m right? When the ball was hung by it , the string was extended to 1.2 m . Assuming that k was the force constant (Elastic Force applied by string due to unit extension), the forces acting on the ball are kx (x is the extension) and mg. So now the ball is in equilibrium, the forces are balanced and thus k can be found.
jmlibunao said:
I can't recall a formula that gives the potential energy when hanging from a string. I can't use P = mgh since height, h, was not given.

When the elastic string is extended, it stores some energy and this energy is called potential energy of the string. Its expression can be found by following the definition of work done to extend the string.

Energy stored E = -∫F.dx where F = -kx. (the integral is a simple exercise :smile:)

Edit: You don't need h to find the gravitational potential energy because you only need the difference in gravitational potential energy in the initial and final state. The difference can be calculated because the change in altitude of the ball is given.
 
Last edited:
  • #5
Sunil Simha said:
You see, the original length of the string was 1m right? When the ball was hung by it , the string was extended to 1.2 m . Assuming that k was the force constant (Elastic Force applied by string due to unit extension), the forces acting on the ball are kx (x is the extension) and mg. So now the ball is in equilibrium, the forces are balanced and thus k can be found.

Okay, thanks for clearing that up! So I can just use kx = mg and just solve for k. But what about the modulus of elasticity? You say I don't need it but the problem is asking for it.





Sunil Simha said:
When the elastic string is extended, it stores some energy and this energy is called potential energy of the string. Its expression can be found by following the definition of work done to extend the string.

Energy stored E = -∫F.dx where F = -kx. (the integral is a simple exercise :smile:)

Edit: You don't need h to find the gravitational potential energy because you only need the difference in gravitational potential energy in the initial and final state. The difference can be calculated because the change in altitude of the ball is given.

Okay, now I remember. The potential energy stored in the string would be E = (1/2)kx^2, the same equation used for springs. The difference that you're talking about would be the Work, right? I also don't get the part where the problem says "When the string is just taut, P is still moving vertially upwards with a velocity of √10 m/s." Why would the string be taut? If P was hit from below then it would move upward, "un-stretching" the string, right? I think I'm having a hard time just understanding what the problem is giving me.
 
  • #6
jmlibunao said:
Okay, thanks for clearing that up! So I can just use kx = mg and just solve for k. But what about the modulus of elasticity? You say I don't need it but the problem is asking for it.

Where?

jmlibunao said:
Okay, now I remember. The potential energy stored in the string would be E = (1/2)kx^2, the same equation used for springs. The difference that you're talking about would be the Work, right? I also don't get the part where the problem says "When the string is just taut, P is still moving vertially upwards with a velocity of √10 m/s." Why would the string be taut? If P was hit from below then it would move upward, "un-stretching" the string, right? I think I'm having a hard time just understanding what the problem is giving me.

The work done on the string is stored as its potential energy. The string would be just taut when there is just a bit of tension (kx) in it. That is, when it just has 0 extension.
 
  • #7
Sunil Simha said:
Where?

It's the #1 question.



Sunil Simha said:
The work done on the string is stored as its potential energy. The string would be just taut when there is just a bit of tension (kx) in it. That is, when it just has 0 extension.

So I computed my k = 200. To compute for u can I use the following equation?

(1/2)(200)(0.2^2) + (1/2)(4 kg)(u^2) = (1/2)(4 kg)(10)

The velocity u is just after the impact so the string would still be stretched at that moment so I included (1/2)(200)(0.2^2) on the left side with u. On the right side it would only be the kinetic energy (1/2)(4 kg)(10) alone since (1/2)(k)(x^2) would be 0
 
  • #8
jmlibunao said:
It's the #1 question.

Sorry, I didn't read it properly. My bad.:redface:
I don't know how to find the modulus of elasticity without the cross-section area. I guess what you did initially (writing it in terms of A) was correct.


jmlibunao said:
So I computed my k = 200. To compute for u can I use the following equation?

(1/2)(200)(0.2^2) + (1/2)(4 kg)(u^2) = (1/2)(4 kg)(10)

The velocity u is just after the impact so the string would still be stretched at that moment so I included (1/2)(200)(0.2^2) on the left side with u. On the right side it would only be the kinetic energy (1/2)(4 kg)(10) alone since (1/2)(k)(x^2) would be 0

I think the equation should be [itex] \frac{kx^2}{2} + \frac{mu^2}{2} = mgx + \frac{mv^2}{2}[/itex]. The ball is gaining gravitational potential energy but is losing kinetic energy the spring potential energy.
 

Related to Particle Hanging by a String is Hit from Below by Another Particle

1. What is the phenomenon of "Particle Hanging by a String is Hit from Below by Another Particle"?

The phenomenon of "Particle Hanging by a String is Hit from Below by Another Particle" is a type of collision in which a stationary particle attached to a string is struck by another particle from below, causing the hanging particle to move and potentially change direction.

2. What factors can affect the outcome of this collision?

The outcome of this collision can be affected by various factors such as the mass, velocity, and angle of the striking particle, as well as the length and tension of the string and the properties of the hanging particle.

3. How does the conservation of momentum apply in this scenario?

The conservation of momentum applies in this scenario as the total momentum of the system before and after the collision remains constant. This means that the combined momenta of the hanging particle and the striking particle before the collision is equal to the combined momenta of the two particles after the collision.

4. Can the hanging particle's motion be predicted using mathematical equations?

Yes, the hanging particle's motion can be predicted using mathematical equations based on the principles of conservation of momentum and energy, as well as the properties of the particles and the string. These equations can be solved to determine the final velocity and direction of the hanging particle after the collision.

5. Are there any real-life applications of this phenomenon?

Yes, this phenomenon has real-life applications in fields such as physics, engineering, and sports. For example, it can be used to study and analyze collisions in particle accelerators, design safer car bumpers, or improve the performance of sports equipment such as golf clubs or tennis rackets.

Back
Top