Motion In the Presence of Resistive Forces

In summary: To solve the problem, I immediately drew a free-body diagram of the copper ball being pulled upward in the water, with the resistive forces pointing downward, and motion being pointing upward. After that, I asked myself why the problem declared a radius and how this radius could be used in solving the problem. Because the copper ball is a sphere, I thought possibly the area or volume might be involved. One thing I also thought about was what kind of object this is. My professor stated that smaller objects with low speeds use the R = -bv formula and larger objects (airplane, car, etc.) with high speeds (such as through air) use the R = 1/2Dp
  • #1
webren
34
0
Hello,
I am having a difficult time getting far into solving this problem:

"A small piece of Styrofoam packing material is dropped from a height of 2.00 m above the ground. Until it reaches terminal speed, the magnitude of its acceleration is given by a = g - bv. After falling 0.500 m, the Styrofoam effectively reaches terminal speed, and then takes 5.00 s more to reach the ground. (a) What is the value of the constant b? (b) What is the acceleration at t = 0? (c) What is the accleration when the speed is 0.150 m/s?"

The first thing I did is to draw a free-body diagram of the Styrofoam falling, with the resisitive forces pointing upward, and the weight pointing downward. Making downward being positive, the resistive forces are negative (hence the given accleration being a = g - bv).

To find b, I first need to find velocity and I don't see how I could find that. I tried setting mg - bv = m(g -bv) = m(v^2/r). This seems kind of messy, but if it's necessary, I would think velocity and mass would eventually cancel out. Is this the right way of solving this problem?

I also thought about using a free-fall kinematic equation and simply solving for velocity, but I think those are appropriate for problems that neglect air resistance. Am I correct?

Thank you.
 
Physics news on Phys.org
  • #2
webren said:
Hello,
I am having a difficult time getting far into solving this problem:

"A small piece of Styrofoam packing material is dropped from a height of 2.00 m above the ground. Until it reaches terminal speed, the magnitude of its acceleration is given by a = g - bv. After falling 0.500 m, the Styrofoam effectively reaches terminal speed, and then takes 5.00 s more to reach the ground. (a) What is the value of the constant b? (b) What is the acceleration at t = 0? (c) What is the accleration when the speed is 0.150 m/s?"

The first thing I did is to draw a free-body diagram of the Styrofoam falling, with the resisitive forces pointing upward, and the weight pointing downward. Making downward being positive, the resistive forces are negative (hence the given accleration being a = g - bv).

To find b, I first need to find velocity and I don't see how I could find that. I tried setting mg - bv = m(g -bv) = m(v^2/r). This seems kind of messy, but if it's necessary, I would think velocity and mass would eventually cancel out. Is this the right way of solving this problem?

I also thought about using a free-fall kinematic equation and simply solving for velocity, but I think those are appropriate for problems that neglect air resistance. Am I correct?

Thank you.
There is no circular motion here so there is reason to use mv^2/r!

The problem is actually simple because of the information given. You know that after it has reached terminal speed, it takes 5.00 seconds to fall another 1.50 meter, right?

Now, after it has reached terminal speed, the acceleration is zero, right? So [itex] g - b v_{terminal} = 0 [/itex]. So you can relate the terminal speed to b and g. Then, using the 5 seconds for 1.5 m, you can get the terminal speed, right?

It's that easy!

Patrick
 
  • #3
There is no circular motion here so there is reason to use mv^2/r!
I don't know why I was thinking of m(v^2/r). It's probably from doing circular motion problems all day.

I understand your statements regarding the problem and I have solved it.

There is another problem that is in the same category that I don't quite understand as well.

"Calculate the force required to pull a copper ball of radius 2.00 cm upward through a fluid at the constant speed 9.00 cm/s. Take the drag force to be proportional to the speed, with proportionality constant 0.950 kg/s. Ignore the buoyant force."

To solve the problem, I immediately drew a free-body diagram of the copper ball being pulled upward in the water, with the resistive forces pointing downward, and motion being pointing upward.

After that, I asked myself why the problem declared a radius and how this radius could be used in solving the problem. Because the copper ball is a sphere, I thought possibly the area or volume might be involved.

One thing I also thought about was what kind of object this is. My professor stated that smaller objects with low speeds use the R = -bv formula and larger objects (airplane, car, etc.) with high speeds (such as through air) use the R = 1/2DpAv^2, where D is the drag coefficient, A is the cross sectional area, p = density, and v being velocity.

I think this problem relates to the R = -bv equation, because it's a smaller object and obviously going through the low speed of water. The problem states: "Take the drag force to be proportional to the speed, with proportionality constant 0.950 kg/s.," so I made b = 0.950 kg/s.

Finally, I converted the velocity and the drag coefficient (b) to m/s instead of cm/s. After that, I said that the sum of forces equals F - R = 0 (constant speed, so there is no acceleration). I also do not think weight (mg) is involved, because the ball is getting pulled upward. I made F = R, and because R = -bv, the equation became F = -bv. I plugged in the b and v values, and got the force, which came out to be 0.855 N. The book disagrees and claims it is 3.01 N.

Are there any steps I am skipping or doing wrong? Any suggestions would be appreciated. Thanks for taking the time to read my post.
 
  • #4
You need to include the gravitational force. Does the question not give you the density of copper? According to wikipedia, the density of copper near room temperature is 8.96 g/cm³.

With that you should arrive at the correct result.
 
  • #5
webren said:
I don't know why I was thinking of m(v^2/r). It's probably from doing circular motion problems all day.

I understand your statements regarding the problem and I have solved it.

There is another problem that is in the same category that I don't quite understand as well.

"Calculate the force required to pull a copper ball of radius 2.00 cm upward through a fluid at the constant speed 9.00 cm/s. Take the drag force to be proportional to the speed, with proportionality constant 0.950 kg/s. Ignore the buoyant force."

To solve the problem, I immediately drew a free-body diagram of the copper ball being pulled upward in the water, with the resistive forces pointing downward, and motion being pointing upward.

After that, I asked myself why the problem declared a radius and how this radius could be used in solving the problem. Because the copper ball is a sphere, I thought possibly the area or volume might be involved.

One thing I also thought about was what kind of object this is. My professor stated that smaller objects with low speeds use the R = -bv formula and larger objects (airplane, car, etc.) with high speeds (such as through air) use the R = 1/2DpAv^2, where D is the drag coefficient, A is the cross sectional area, p = density, and v being velocity.

I think this problem relates to the R = -bv equation, because it's a smaller object and obviously going through the low speed of water. The problem states: "Take the drag force to be proportional to the speed, with proportionality constant 0.950 kg/s.," so I made b = 0.950 kg/s.

Finally, I converted the velocity and the drag coefficient (b) to m/s instead of cm/s. After that, I said that the sum of forces equals F - R = 0 (constant speed, so there is no acceleration). I also do not think weight (mg) is involved, because the ball is getting pulled upward. I made F = R, and because R = -bv, the equation became F = -bv. I plugged in the b and v values, and got the force, which came out to be 0.855 N. The book disagrees and claims it is 3.01 N.

Are there any steps I am skipping or doing wrong? Any suggestions would be appreciated. Thanks for taking the time to read my post.

I was going to say exactly the same thing as Mute. I don't know why you concluded that the weight is not involved because the motion is upward (think of throwing a baseball upward, even it it is moving upward, the force of gravity is clearly relevant!). So the force you apply on the object must overcome both the drag force and the force of gravity (the weight). (In real life, the buoyant force would "help" you, i.e. it would be acting upward also but they said to neglect it).

and this is why they gave you the *composition* and radius of the ball, so that you may calculate its mass and therefore its weight (mg).
 

1. What is motion in the presence of resistive forces?

Motion in the presence of resistive forces, also known as motion with air resistance or drag, refers to the movement of an object through a fluid medium such as air or water. In this type of motion, the object experiences a resistive force that opposes its motion, making it more difficult for the object to move through the fluid.

2. How does air resistance affect an object's motion?

Air resistance affects an object's motion by creating a force that acts in the opposite direction of the object's motion. This force increases as the object's speed increases, and it can significantly slow down the object's movement. As a result, the object may not be able to reach its maximum potential speed due to the opposing force of air resistance.

3. What factors affect the amount of resistive force an object experiences?

The amount of resistive force an object experiences depends on several factors, including the object's speed, the density of the fluid, the object's surface area, and the fluid's viscosity. As the object moves faster, the resistive force increases. A higher density fluid or a larger surface area also increases the resistive force, while a lower viscosity fluid decreases it.

4. How do you calculate the resistive force on an object?

The resistive force on an object can be calculated using the formula FR = ½CDρAv2, where FR is the resistive force, CD is the drag coefficient, ρ is the density of the fluid, A is the object's cross-sectional area, and v is the object's velocity. The drag coefficient is a dimensionless constant that depends on the shape and surface properties of the object.

5. How can resistive forces be reduced?

There are several ways to reduce resistive forces on an object, such as streamlining the object's shape to decrease its surface area, using a more aerodynamic design, or using a fluid with lower density or viscosity. Additionally, reducing the object's speed can also decrease the resistive force. In some cases, adding a lubricant or coating to the object's surface can also help reduce the resistive force and improve its motion.

Similar threads

  • Introductory Physics Homework Help
Replies
4
Views
14K
  • Introductory Physics Homework Help
Replies
13
Views
1K
  • Introductory Physics Homework Help
Replies
2
Views
647
  • Introductory Physics Homework Help
Replies
20
Views
1K
  • Introductory Physics Homework Help
Replies
10
Views
303
  • Introductory Physics Homework Help
Replies
5
Views
1K
  • Introductory Physics Homework Help
Replies
6
Views
1K
  • Introductory Physics Homework Help
Replies
12
Views
1K
  • Introductory Physics Homework Help
2
Replies
39
Views
2K
  • Introductory Physics Homework Help
Replies
1
Views
1K
Back
Top