courses:phy101l:1
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| courses:phy101l:1 [2023/06/03 02:28] – [2. Experimental Setup] asad | courses:phy101l:1 [2023/09/30 20:02] (current) – asad | ||
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| ====== 1. Trajectory of a projectile ====== | ====== 1. Trajectory of a projectile ====== | ||
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| The report should have the following five sections. Each section must be written by a separate student. The whole report must be in a single Google Colab file and attached from Google Drive into the associated Google Classroom assignment. | The report should have the following five sections. Each section must be written by a separate student. The whole report must be in a single Google Colab file and attached from Google Drive into the associated Google Classroom assignment. | ||
| ===== - Introduction and Theory ===== | ===== - Introduction and Theory ===== | ||
| - | A projectile | + | Any object projected in the gravitational field is called a **projectile** and its motion a **projectile motion**. |
| - | ===== - Experimental Setup ===== | + | {{:courses: |
| - | For this experiment you have to use the following apparatus: a table, a bench, a ramp, some marble balls, 3 white recording papers, 3 carbon papers, some adhesive tape for fixing the papers on the table or bench, a long meter scale to measure long heights and lengths, a short meter scale for measuring short distances on the recording papers, and a weight scale to measure the mass of a ball. | + | |
| - | {{: | + | For such a motion, the magnitude of net acceleration $a=a_y=-g$, the gravitational acceleration, |
| - | The setup is briefly sketched through the following points (elaborate in the report). | + | $$ x = x_0 + v_x t $$ |
| - | - A bench is placed on a table. There must be enough space in front of the bench for the balls to bounce. | + | and for the vertical motion |
| - | - A ramp is placed on the bench. | + | |
| - | ===== - Method and Data ===== | + | |
| - | ^ Quantity ^ Symbol ^ Value ^ Error ($\delta$) | | + | |
| - | | Height of the release point | $H$ | $11$ cm | $\delta H$ = 0.1 cm | | + | |
| - | | Height of the end of the ramp | $h$ | cm | $\delta h = $ cm | | + | |
| - | | Height of the second bounce | $h'$ | cm | $\delta h' = $ cm | | + | |
| - | | Position of the first bounce | $s$ | cm | $\delta s=$ cm | | + | |
| - | | Position of the second bounce | $s'$ | cm | $\delta s'=$ cm | | + | |
| - | | Mass of the marble ball | $m$ | cm | $\delta m=$ g | | + | |
| - | ===== - Analysis and Results ===== | + | $$ y = y_0 + \overline{v_y} t, $$ |
| - | Using the six measurements you will have to calculate the following quantities. | + | $$ y = y_0 + v_y t - \frac{1}{2} gt^2, $$ |
| + | $$ v_y = v_{0y} - gt, $$ | ||
| + | $$ v_y^2 = v_{0y}^2 | ||
| - | ==== - Time and velocity ==== | + | where $\overline{v_y}$ is the average vertical velocity within a duration |
| - | Time for the ball to leave the ramp and reach point A | + | |
| - | $$ t = \sqrt{\frac{2h}{g}} $$ | + | The magnitude and direction of the velocity vector can always be found remembering the fact that $v_x=v\cos\theta$ and $v_y = v\sin\theta$ which means that the net velocity $v=\sqrt{v_x^2+v_y^2}$ and the angle of the velocity vector $\theta=\tan^{-1}(v_y/v_x)$. |
| - | where gravitational acceleration $g=981\pm 1$ cm s$^{-2}$. | + | From these equations of motion we can find three important quantities: maximum height, range and the trajectory. Maximum height of a projectile |
| - | Horizontal component of the acceleration of the ball $a_x=?$ | + | $$ h = \frac{v_{0y}^2}{2g} = \frac{v_0^2\sin^2\theta}{2g}, |
| - | The unchanging horizontal velocity of the ball $ v_x = s/t$. | + | the range (maximum horizontal distance) |
| - | Vertical velocity of the ball just before it hits the table at point A $ v_y = gt = -\sqrt{2gh}$. | + | $$ R = \frac{v_0^2 \sin 2\theta_0}{g} $$ |
| - | The time the ball takes to reach point B from point A $ t_{AB} = (s' | + | where $\theta_0$ is the initial angle, and the trajectory of the projectile is described as |
| - | Vertical component of the velocity of the ball after it leaves point A $ v_y' | + | $$ y = (\tan\theta)x - \frac{g}{2v_0^2\cos^2\theta} x^2 $$ |
| - | Net velocity | + | which is the equation |
| - | Net velocity | + | In this experiment, you will create such a parabolic path twice by releasing a marble ball from a ramp. The first part of the parabolic path will be from the end of the ramp to a point where the ball bounces, and the second part will be between the points of the first and second bounces. |
| - | ==== - Angle and height | + | You will measure different parameters of this trajectory, for example, the height of the ramp, the positions of the bounces |
| - | Maximum height | + | |
| - | $$ h' | + | ===== - Experimental Setup ===== |
| + | For this experiment you have to use the following apparatus: a table, a bench, a ramp, some marble balls, 3 white recording papers, 3 carbon papers, some adhesive tape for fixing the papers on the table or bench, a long meter scale to measure long heights and lengths, a short meter scale for measuring short distances on the recording papers, and a weight scale to measure the mass of a ball. | ||
| - | The angle of the trajectory before reaching A | + | {{: |
| - | $$ \theta = \arctan{\frac{v_y}{v_x}} $$ | + | Describe how you set up the apparatus on the table. |
| - | and after leaving A | + | ===== - Method |
| + | ^ Quantity ^ Symbol ^ Value ^ Error ($\delta$) | | ||
| + | | Mass of the marble ball | $m$ | g | $\delta m=$ g | | ||
| + | | Height of the end of the ramp | $y$ | cm | $\delta y = $ cm | | ||
| + | | Position of the first bounce at A | $s$ | cm | $\delta s=$ cm | | ||
| + | | Position of the second bounce at B | $s'$ | cm | $\delta s'=$ cm | | ||
| + | | Maximum height between A and B | $h$ | cm | $\delta h = $ cm | | ||
| + | |||
| + | Describe how collected these data. | ||
| + | |||
| + | ===== - Analysis and Results ===== | ||
| + | Using the five measurements you will have to calculate the following quantities. | ||
| + | |||
| + | ==== - Velocity ==== | ||
| + | First, calculate the time for the ball to leave the ramp and reach point A which is $t = \sqrt{2y/ | ||
| + | |||
| + | Horizontal component of the acceleration of the ball $a_x=0$, so the horizontal velocity of the ball $ v_x = s/t$. The vertical velocity of the ball just before it hits the table at point A would be $ v_y = -gt = -\sqrt{2gh}$. | ||
| + | |||
| + | From the maximum height $h$, you can calculate the time it took for the marble to go from points A to B ($t' | ||
| + | |||
| + | So the net velocity of the ball before it impacts at A is $v = \sqrt{v_x^2+v_y^2}$. And the net velocity of the ball after it impacts at A is $v' = \sqrt{v_x' | ||
| - | $$ \theta' | + | The angle of the trajectory before reaching A is $ \theta = \tan^{-1}(v_y/ |
| ==== - Kinetic energy ==== | ==== - Kinetic energy ==== | ||
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| Vertical component of the momentum before reaching A $P_y=mv_y$ and after leaving A $P'_y = mv' | Vertical component of the momentum before reaching A $P_y=mv_y$ and after leaving A $P'_y = mv' | ||
| - | Horizontal | + | Vertical |
| - | Net momentum before reaching A $p = mv$. | + | So the net momentum before reaching A $p = mv$ and the net momentum after leaving A is $p' = mv'$. |
| - | + | ||
| - | Net momentum after leaving A $p' = mv'$. | + | |
| ==== - Impulse ==== | ==== - Impulse ==== | ||
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| ==== - Discussion ==== | ==== - Discussion ==== | ||
| + | Answer the following questions: | ||
| + | - What is the difference between systematic and stochastic error? Which errors in this experiment are systematic and which are stochastic? | ||
| + | - Why is $\delta s' > \delta h > \delta s$? | ||
| + | - Which velocity is greater, before reaching point A or after leaving A? | ||
| + | - Is the impulse positive or negative? Why? | ||
| ==== - Conclusion ==== | ==== - Conclusion ==== | ||
| - | |||
| - | ===== Report sample ===== | ||
| - | < | ||
| - | <script src=" | ||
| - | </ | ||
courses/phy101l/1.1685780937.txt.gz · Last modified: by asad
