#$&* course PHY 201 012. `query 12*********************************************
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Given Solution: `a** The net force on the system is the force of gravity on the suspended weight: Fnet = m2 * 9.8 m/s/s, directed downward. Gravity also acts on m1 which is balanced by the upward force of table on this mass, so the forces on m1 make no contribution to Fnet. Acceleration=net force/total mass = 9.8 m/s^2 * m2 / (m1+m2), again in the downward direction. The change in gravitational PE is equal and opposite to the work done by gravity. This is the definition of change in gravitational PE. If the mass m2 descends distance `dy then the gravitational force m * g and the displacement `dy are both downward, so that gravity does positive work m g `dy on the mass. The change in gravitational PE is therefore - m g `dy. COMMON MISCONCEPTIONS AND INSTRUCTOR COMMENTS: Misconception: The tension force contributes to the net force on the 2-mass system. Student's solution: The forces acting on the system are the forces which keep the mass on the table, the tension in the string joining the two masses, and the weight of the suspended mass. The net force should be the suspended mass * accel due to gravity + Tension. INSTRUCTOR COMMENT: String tension shouldn't be counted among the forces contributing to the net force on the system. The string tension is internal to the two-mass system. It doesn't act on the system but within the system. Net force is therefore suspended mass * accel due to gravity only 'The forces which keep the mass on the table' is too vague and probably not appropriate in any case. Gravity pulls down, slightly bending the table, which response with an elastic force that exactly balances the gravitational force. ** STUDENT COMMENT I don't understand why m1 doesn't affect the net force. Surely it has to, if mass1 was 90kg, or 90g, then are they saying that the force would be the same regardless? INSTRUCTOR RESPONSE m1 has no effect on the net force in the given situation. Whatever the mass on the tabletop, it experiences a gravitational force pulling it down, and the tabletop exerts an equal and opposite force pushing it up. So the mass of that object contributes nothing to the net force on the system. The mass m1 does, however, get accelerated, so m1 does have a lot to do with how quickly the system accelerates. The greater the mass m1, the less accelerating effect the net force will have on the system. Also if friction is present, the mass m1 is pulled against the tabletop by gravity, resulting in frictional force. The greater the mass m1, the greater would be the frictional force. All these ideas are addressed in upcoming questions and exercises. STUDENT COMMENT I understand the first few parts of this problem, but I am still a little unsure about the gravitational PE. I knew what information that was required to solve the problem, but I just thought the solution would be more that (-m2 * 9.8m/s^2 * ‘dy). INSTRUCTOR RESPONSE Only m2 is changing its altitude, so only m2 experiences a change in gravitational PE. Equivalently, only m2 experiences a gravitational force in its direction of motion, so work is done by gravity on only m2. STUDENT COMMENT I forgot that PE = m * g * 'dy. And I did not think that the table exerting force on the mass took it out of the system. I understand the idea though. INSTRUCTOR RESPONSE the table doesn't take the mass out of the system, but it does counter the force exerted by gravity on that mass so the total mass of the system is still the total of the accelerating masses, but the net force is just the force of gravity on the suspended mass, (since the system is said to be frictionless, there is no frictional force to consider) SYNOPSIS The change in gravitational PE is equal and opposite to the work done by gravity. This is the definition of change in gravitational PE. If the mass m2 descends distance `dy then the gravitational force m * g and the displacement `dy are both downward, so that gravity does positive work m g `dy on the mass. The change in gravitational PE is therefore - m g `dy. As you say, `dw_noncons + `dPE + `dKE = 0 If `dW_noncons is zero, as is the case here (since there are no frictional or other nonconservative forces present), then `dPE + `dKE = 0 and `dKE = - `dPE. In this case `dPE = - m g `dy so `dKE = - ( - m g `dy) = m g `dy. The signs are confusing at first, but if you just remember that signs are important these ideas will soon sort themselves out. &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): I am behind in the formula for 'dPE. I know the formula for 'dKE. I must be missing it somewhere in the notes. With the formulas 'dW_nc + 'dPE + 'dKE = 0, I understand it better. ------------------------------------------------ Self-critique Rating: 3
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Given Solution: `a**Friction would act to oppose the motion of the mass m1 as it slides across the table, so the net force would be m2 * g - frictional resistance. ** &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): ------------------------------------------------ Self-critique Rating: ********************************************* Question: `qExplain how you use a graph of force vs. stretch for a rubber band to determine the elastic potential energy stored at a given stretch. YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your solution: The PE can be determined by the graph of force vs. stretch by the calculating the area, trapezoid, under the curve between two data points. confidence rating #$&*: ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
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Given Solution: `a** If we ignore thermal effects, which you should note are in fact significant with rubber bands and cannot in practice be ignored if we want very accurate results, PE is the work required to stretch the rubber band. This work is the sum of all F * `ds contributions from small increments `ds from the initial to the final position. These contributions are represented by the areas of narrow trapezoids on a graph of F vs. stretch. As the trapezoids get thinner and thinner, the total area of these trapezoids approaches, the area under the curve between the two stretches. So the PE stored is the area under the graph of force vs. stretch. ** STUDENT QUESTION I am still a little confused about if the work is done by the rubber bands, or if the work is done one the rubber bands. Would you explain the difference? INSTRUCTOR RESPONSE This example might be helpful: If you pull the end of an anchored rubber band to the right, it exerts a force to the left, in the direction opposite motion, so it does negative work during the process. You, on the other hand, pull in the direction of motion and do positive work on the rubber band. &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): ------------------------------------------------ Self-critique Rating: ********************************************* Question: `q Does the slope of the F vs stretch graph represent something? Does the area under the curve represent the work done? If so, is it work done BY or work done ON the rubber bands? YYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYYY Your solution: The rise equals change in force, the stretch represents the run, therefore the slope = 'dN / 'ds confidence rating #$&*: ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
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Given Solution: `a** The rise of the graph is change in force, the run is change in stretch. So slope = rise / run = change in force / change in stretch, which the the average rate at which force changes with respect to stretch. This basically tells us how much additional force is exerted per unit change in the length of the rubber band. The area is indeed with work done (work is integral of force with respect to displacement). If the rubber band pulls against an object as is returns to equilibrium then the force it exerts is in the direction of motion and it therefore does positive work on the object as the object does negative work on it. If an object stretches the rubber band then it exerts a force on the rubber band in the direction of the rubber band's displacement, and the object does positive work on the rubber band, while the rubber band does negative work on it. ** STUDENT QUESTION Okay, so are you saying that the rubber band could either be doing work or getting work done on it? I believe I understand this, but just wanted to double check. INSTRUCTOR RESPONSE Yes, and that depends on whether the rubber band is being stretched, or contracting. When it is being stretched positive work is being done on the rubber band. After being released the rubber band does positive work on the object to which its force is applied. &&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&& Self-critique (if necessary): ------------------------------------------------ Self-critique Rating: PREVIOUS STUDENT RESPONSE TO REQUEST FOR COMMENTS There is a whole lot of stuff concerning Newton’s laws of motion and there applications to force and acceleration. They will take some serious application to master. I understand what potential energy is, I understand that it is decreasing as kinetic energy increase, but I don’t understand how to measure it. Its like an invisible force, and the only relation to which I can apply it is in the context of gravity. If we have a 1kg object and we hold it 5meters off the ground, then according to the equation above PE = m*g*`dy this would be PE = 1kg * 9.8m/s^2 * 5m = 49 kg * m^2/s^2 my algebra is so bad but I still cant see this contributing to a useful measurement or unit. I don’t know how to swing it so it’ll give me a newton, PE has to be measured in newtons right because it is indeed a force? Ohhh I get it now!! I remember, a kg times a m/s^2 is a newton, and a newton times a meter is a Joule!!! So this is a valid measurement, which would make that equation valid, the potential energy for the above circumstance would be 49 Joules then. INSTRUCTOR RESPONSE Very good. Remember that F_net = m a If you multiply mass m in kg by acceleration a in m/s^2, you get the force in Joules. Of course when you multiply kg by m/s^2 you get kg m/s^2. This is why a Newton is equal to a kg m / s^2. Work being the product of a force and a displacement will therefore have units of Newtons * meters, or kg * m/s^2 * m, which gives us kg m^2 / s^2. Query Add comments on any surprises or insights you experienced as a result of this assignment." Self-critique (if necessary): ------------------------------------------------ Self-critique rating: PREVIOUS STUDENT RESPONSE TO REQUEST FOR COMMENTS There is a whole lot of stuff concerning Newton’s laws of motion and there applications to force and acceleration. They will take some serious application to master. I understand what potential energy is, I understand that it is decreasing as kinetic energy increase, but I don’t understand how to measure it. Its like an invisible force, and the only relation to which I can apply it is in the context of gravity. If we have a 1kg object and we hold it 5meters off the ground, then according to the equation above PE = m*g*`dy this would be PE = 1kg * 9.8m/s^2 * 5m = 49 kg * m^2/s^2 my algebra is so bad but I still cant see this contributing to a useful measurement or unit. I don’t know how to swing it so it’ll give me a newton, PE has to be measured in newtons right because it is indeed a force? Ohhh I get it now!! I remember, a kg times a m/s^2 is a newton, and a newton times a meter is a Joule!!! So this is a valid measurement, which would make that equation valid, the potential energy for the above circumstance would be 49 Joules then. INSTRUCTOR RESPONSE Very good. Remember that F_net = m a If you multiply mass m in kg by acceleration a in m/s^2, you get the force in Joules. Of course when you multiply kg by m/s^2 you get kg m/s^2. This is why a Newton is equal to a kg m / s^2. Work being the product of a force and a displacement will therefore have units of Newtons * meters, or kg * m/s^2 * m, which gives us kg m^2 / s^2. Query Add comments on any surprises or insights you experienced as a result of this assignment." Self-critique (if necessary): ------------------------------------------------ Self-critique rating: #*&!