Wednesday, October 5, 2016

Physics 4A (5/10/16) Work and kinetic Energy

Physics 4A (5/10/16)
Work and kinetic Energy
Brett Mccausland
Lab Partners: Luis Diaz, Bimaya Jayaratne

Purpose

Calculate experimentally kinetic energy and work by a non constant spring force, and model the relationship between work and kinetic energy.

Procedure Experiment 1

As seen in the apparatus we placed a steel cart on a steel track and attached a force sensor to the top of it as well as a plate. we attached steel bar to the end of the table with a clamp and attached  a spring which we also attached  to the force sensor and placed a motion sensor at the opposite side of the track. We zeroed are instruments at the point where the cart sat with no tension in the spring. We connected all are instruments to logger pro . We  wanted to find work and the spring constant so we dragged the cart to the opposite side of the track and using the data on the force from the force sensor and the distance traveled from the motion sensor we created a force to position graph. The slope of this graph was are spring constant and the area under the curve was the work done on the spring.

work kinetic energy.JPG

Procedure Experiment 2
For the second procedure we used the same apparatus and we zeroed the cart at the end of the track in which the cart was attached to the spring and pulled the cart all the way to the opposite side of the track. We measure the mass of the cart and entered the data into logger pro. we released the cart, and using the motion sensor tracked its velocity along its path, and displacement. The motion sensor gave us a data point every 30th of a second. To make sure that the motion sensor was able to track the movement of the cart down the track we placed a square plate to the side of the cart that the motion sensor was directed at as in the first experiments procedure.

Calculations Exp 1

For the first procedure we pulled the cart as mentioned in the procedure exp1 section of this report and using a force sensor connected to logger pro and motion sensor we were able track force to position and graph it as seen below. Since we know that work = F*∆d the area under curve yields the total work done pulling the cart attached to the spring the length of the track. We found this area by using an integral capability on logger pro. Additionally the linear fit of the slope of this curve gave us are spring constant.
Lab 11 area.png

Calculations Exp 2

Are goal was to model both kinetic energy of a system and work of a system and show that they are equivalent . As mentioned in the procedure Exp 2 section of this report we dragged the cart that had the force sensor attached to it to the opposite side of the track and then gathered the data following the release of the cart. This data gave two graphs the top graph is our position to kinetic energy graph, let's talk about it a little. Logger pro calculated the kinetic energy by using the following formula KE= 1/2mV^2. Obviously logger pro didn't know are mass so we measured the mass of are kart and manually entered it into logger pro. The only other variable is velocity, logger pro used the ∆position/∆time gathered from the motion sensor to calculate the velocity. Then using this information logger pro plugged in the values it was gathering into the equation for Ke and graphed it relative to position yielding the top graph.For the Bottom graph logger pro used the data from the force sensor and ∆x from the motion sensor to yield the force to position graph. As I might have already mentioned the work at any given position is the area under the graph to that position  and this should be equal to the kinetic energy which is why we placed these two graphs on top of each other to make comparisons and test this theory experimentally. I will discuss these results in the data analysis and conclusion section.   Work to kinetic energy 2016-10-05 at 9.07.52 AM.png

Conclusion and Data Analysis


The data from are two graph from exp 2 as can be seen in the data analysis boxes do not perfectly match as we would predict, for one position , the closets positional match we had the kinetic energy was .685 J and are work was 0.8473 J .There is several reasons some from random error and 1 systematic that I would like to discuss that might be the cause of these less than convincing results. The first is that while the motion sensor is very precise and creates a data point every 30th of a second the experiment entire length of time is only approximately 0.4s yielding only around 13 data points to track the position and use this to also calculate the velocity. With a more precise device we might see a slight improvement in the difference between these two graphs. One other problem is that we were trying to compare the results for work and kinetic energy at the same point on both graphs however, as can be seen, we could not exactly match the position for both graphs do to a lack in data points in the exact same position on both graphs and had to settle with a difference in position of 0.002 s not a big difference however remember this is a small measurement to begin with so it affects a larger percentage of error than previous experiments. Had I had more control over the experiment there are a couple of ways that the experiment could be made to be more accurate. The easiest two solutions is extend the track maybe by connecting two tracks thus reducing the percentage error from the instruments and also using springs with smaller constants thus lengthening the time and yielding more data points from the motion sensor. Overall despite the fact that we were not able to make a perfect match with are data from are graph for work and for kinetic energy we can still see that even under very small instances kinetic energy is directly connected to work hence the work done on the cart by the spring causes a direct change in its kinetic energy.   

Monday, October 3, 2016

Centripetal Force Physics 4A (03-10-16)

Physics 4A  (03-10-16)
Centripetal Force
Brett Mccausland
Lab Partner:

Purpose

Model the relationship between the angle made by a circular revolving mass and its angular velocity.

Procedure

As seen in the photo of the apparatus we used a tripod stand to hold a meter stick attached to a steel rod with clamps. This steel rod was attached to a motor that caused the meter stick to revolve and the string and mass attached to it. Due to the net force of revolving motion (centripetal force ) the mass while revolving elevated to some angle well call theta . We measured the change in height and the length of the string in order to find this angle . We did this by placing a second stand that had a piece of paper attached to it and raised it to the point at which the mass collided with the paper. We then measured and recorded the height. Before causing the collision between the paper and the mass we recorded 10 revolutions and took the average to find are angular velocity.  centripetal force.JPG

Calculations

As mentioned in the procedure we used experimental data to find a experimental value for angular velocity. The first thing we did is find the angle, we did so by using our measurement of the height of the large tripod stand and the height of the small tripod
angle cpfJPG.JPG
Stand and are length. Now that we had a hypotenuse and a adjacent side we were are to find the angle by taking arccosine as seen in the image labeled find angle.   terminal velocities.After we found are general formula for are angle we next found are general formula for are angular velocity in terms of theta using summations of the forces in the x and y components as seen in the image above in the yellow highlighted box. There was also one more much simpler way for us to find are angular speed and that was with the data we had from the times we recorded on the amount of time it took for the bob to make a complete revolution. This was are angular velocity in terms of rev/sec in which we then used the formulas listed in the green box to convert to rad /sec.  angular velocity.JPGCentripetal force.png

Conclusion and Data Analysis

The data in the excel spreadsheet models  circular velocity with respect to time vs the circular velocity with respect to change in the height or the change in the angle. Very consistent with what

We would hypothesis based on observation there is a linear correlation between the change in angular velocity and the change in the height at which it rotates. This is explainable based on are force summation equations we wrote out in which show that the more tension added to the string the more force is going to exerted in not just the x component but the y component as well. The force of gravity in the y component stays constant however as the bob increases speed its angle due to a net force in the y component increases, which is due to the tension force, until  the point in which it has no net force in the y component and the tension force in the y component is equal to the force of gravity. Inconsistency in the data are evident since there is not a perfect linear fit as seen in the graph of the data. Beyond the propagation of error from the precision of are tools being (+/-) 0.1cm for are lengths and 0.001 seconds in the stopwatch there are several others. The largest error that I observed was that of the apparatus use of a ruler in which was not rigid and was bending due to the force centripetal . This gives more uncertainty in are measurement for the height of the paper on the small stand since the ruler was bending it made for a slightly lower height. Also it could be observed that there was air friction, the disturbed air could be felt if you stood close to the path of the bob as it went by this non negligible force has an effect on are error in are calculations of angular speed.