Conservation of Energy of a pendulum

In summary: I had no idea this was here.The radial component times cos(30°) is the centripetal component. It is equal to the centripetal force. The tangential component is T sin(30°) = Tb. The sum of the two is the centripetal force Fcp, Fcp= T cos(30°)+mg-Ft= T cos(30°)+mg-(T sin(30°))tan(30°)= T cos(30°)+mg-(T sin(30°))(2/cos(30°))= T cos(30°)+mg-2T sin(30°)= T cos(30°)+mg-2T sin(30°)
  • #1
knowNothing23
35
0
A pendulum consists of a 2.0-kg bob attached to a light 3.0-m-long
string. While hanging at rest with the string vertical, the bob is struck a sharp
horizontal blow, giving it a horizontal velocity of 4.5 m/s. At the instant the string
makes an angle of 30° with the vertical, what is (a) the speed, (b) the gravitational
potential energy (relative to its value is at the lowest point), and (c) the tension in
the string? (d) What is the angle of the string with the vertical when the bob
reaches its greatest height?

My problem is with the answer of c.)
The book shows a different answer.
Thank you.

The Attempt at a Solution


I have taken the free body diagram of the pendulum and the string, when the string forms 30 degrees with the vertical.
The net force sum of the "y" component:
[itex]\sumF[/itex]=Tcos(30)-mg=m(v^(2) )/ L , where "L" is the length of the string.

Solving for T:
T=(m/cos(30) )( v^(2)/L +g)

My answer is 32N.
 
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  • #2
knowNothing23 said:
A pendulum consists of a 2.0-kg bob attached to a light 3.0-m-long
string. While hanging at rest with the string vertical, the bob is struck a sharp
horizontal blow, giving it a horizontal velocity of 4.5 m/s. At the instant the string
makes an angle of 30° with the vertical, what is (a) the speed, (b) the gravitational
potential energy (relative to its value is at the lowest point), and (c) the tension in
the string? (d) What is the angle of the string with the vertical when the bob
reaches its greatest height?

My problem is with the answer of c.)
The book shows a different answer.
Thank you.

The Attempt at a Solution


I have taken the free body diagram of the pendulum and the string, when the string forms 30 degrees with the vertical.
The net force sum of the "y" component:
[itex]\sumF[/itex]=Tcos(30)-mg=m(v^(2) )/ L , where "L" is the length of the string.

Solving for T:
T=(m/cos(30) )( v^(2)/L +g)

My answer is 32N.

Provided you have used that equation correctly it should get the right answer - assuming you had part (a) correct.

In case it is the way you are using the formula poorly - evaluate this

T = [mg + (m.v^2)/L]/cos30
 
  • #3
My answer in part a.) is equal to the one provided by the book. The answer is 3.5171 m/s.

The book's answer of problem c.) is 25N.
 
  • #4
knowNothing23 said:
My answer in part a.) is equal to the one provided by the book. The answer is 3.5171 m/s.

The book's answer of problem c.) is 25N.

I think you [and me] were looking at this incorrectly.

T = (mv^2 / L) + mgcos(theta) not (mv^2 / L) + mg/cos(theta)

The mv^2 / L part we agree with, I shall ignore that.

The mg/cos(theta) parts comes from analysing a conical pendulum situation, when the acceleration is horizontal.
HOWEVER, this time the bob is merely swinging - and importantly slowing down.
The net force for this part of the analysis is tangential to the arc, not horizontal.

Draw a "free body diagram" for that situation and you will see what is happening.

I don't know how to attach diagrams or pictures to this page - so I have tried to describe it.
 
  • #5
I'm not sure, what you mean. In a conic situation there is a centripetal acceleration as well as a tangential. Also, the equation I proposed is not the one you mentioned.
T=(m/cos(30) ) ( v^(2)/L) +g), the cosine of 30 degrees divides mv^(2)/L as well.

There are more than two ways to analyze the sum of vectors at the angle of 30 degrees and both ways should give the same result. We can either take the component of T or the component of Weight and sum them. In my approach I took the component of T and subtracted Weight from it.
 
  • #6
knowNothing23 said:
I have taken the free body diagram of the pendulum and the string, when the string forms 30 degrees with the vertical.
The net force sum of the "y" component:
[itex]\sumF[/itex]=Tcos(30)-mg=m(v^(2) )/ L , where "L" is the length of the string.

The direction of the centripetal force is the same as that of the tension in the string. It is not vertical.

The usual procedure is to write the force components parallel and perpendicular to the string. The parallel component of gravity is mgcos(30°). The centripetal force is equal to the resultant of the tension and the radial component of gravity:

Mv^2/L = T-mgcos(30°) Use v=3.5171 m/s.

ehild
 
  • #7
Thank you, ehild.
That was my question. Why take the component of the weight, when one can do it for the tension.
 
  • #8
See attached figures. The one on the left shows the forces acting on the bob: tension and gravity. The resultant is shown by blue. It is not parallel with the string as the bob has both velocity and acceleration along the arc. The resultant force is equal to the centripetal force (along the string) + the tangential force, tangent to the arc T+G = Fcp+Ft (all vectors).Writing this equation in x and y components, you get:

T cos(30°)-mg=Fcp cos(30°)-Ft sin(30°)
-T sin(30°) = -Fcp sin(30°)-Ft cos(30°)

Solve. If you do it correctly, you get T=Fcp+mgcos(30°). A bit more complicated than the other one, with radial and tangential components, is not it?

ehild
 

Attachments

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  • #9
PeterO said:
The net force for this part of the analysis is tangential to the arc, not horizontal.
The net force is neither horizontal nor tangential: it has a component along the arc and also the radial component: the centripetal force.

PeterO said:
I don't know how to attach diagrams or pictures to this page - so I have tried to describe it.

When writing a post, scroll down, click on "Manage Attachments"

ehild
 
  • #10
Thank you!
 

1. What is the law of conservation of energy?

The law of conservation of energy states that energy cannot be created or destroyed, but can only be transformed from one form to another. This means that the total amount of energy in a system remains constant over time.

2. How does this law apply to a pendulum?

In a pendulum, the law of conservation of energy applies because the pendulum's potential energy is converted into kinetic energy as it swings back and forth. The total energy of the pendulum remains the same, even as it continuously transforms between potential and kinetic energy.

3. What factors affect the conservation of energy in a pendulum?

The conservation of energy in a pendulum is affected by the length of the pendulum, the mass of the bob, and the amplitude of its swing. These factors determine the potential energy and the maximum kinetic energy of the pendulum, which ultimately affect its total energy.

4. Can the energy of a pendulum ever be completely conserved?

In theory, the energy of a pendulum can be completely conserved if there is no friction or air resistance present. However, in real-world scenarios, some energy will always be lost due to these external factors, resulting in a decrease in the pendulum's total energy over time.

5. How does the conservation of energy in a pendulum relate to other physical laws?

The conservation of energy in a pendulum is related to other physical laws, such as the law of gravity and the laws of motion. These laws work together to determine the behavior of the pendulum and ensure that its energy remains constant over time.

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