Skip to main content

Lab 3- Non-Constant acceleration problem

Purpose
Solve non-constant acceleration problem by both numerical approach and analytical approach. Here is the question.
A 5000-kg elephant on frictionless roller skates is going 25 m/s when it gets to the bottom of a hill and arrives on level ground. At that point a rocket mounted on the elephant’s back generates a constant 8000 N thrust opposite the elephant’s direction of motion. The mass of the rocket changes with time (due to burning the fuel at a rate of 20 kg/s) so that the m(t) = 1500 – 20t. Find how far the elephant goes before coming to rest.


Numerical Approach
1.     Put appropriate values in for Vo and Xo.
2.     Set Δt to be 1 second. Put in the other appropriate values in cell B1 through B4. (Recall that the force is negative here, since it points in the negative x-direction.)
3.     Input a formula into cell A9 that will calculate the appropriate time, and that you can fill down. Use $B$5 in our formula, so the cell doesn't change as I fill down.
4.     Input a formula into cell B8 that will let me calculate the acceleration at any time. Fill down
5.     In cell C9 calculate the average acceleration for that first Δt interval.
6.     In cell D9 calculate the change in velocity for that first time interval.
7.     In cell E9 calculate the speed at the end of that time interval.
8.     In cell F9 calculate the average speed at the end of that time interval.
9.     In cell G9 calculate the change in position of the elephant during that time internal.
10.   In the H9 calculate the position of the elephant. 

11.   Change the time interval from 1 second to 0.1s and see if it makes a difference.
12.   Change the time interval to 0.05s instead of 0.1s and see if it makes a difference.

So we can derive the conclusion that if we change the interval from 1s to 0.1s, it makes a huge difference. But if we change the interval from 0.1s to 0.05s, it makes a quite small difference.

Questions
1.     When the interval equals to 0.05s, the result of numerical approach approximately equals to the result of analytical approach.
2.     Choose smaller time interval until the result stops changing. That time interval is small enough.
3.     Using the numerical approach with a 0.05s interval, the result is 164.0363m. 

Comments

Popular posts from this blog

8-May, 15-May-2017: Lab 16: Angular acceleration

Purpose: Learn the angular acceleration. Find out how the changing of hanging mass, rotating mass and the torque radius will influence on the angular acceleration. Introduction: In the angular acceleration lab, we usually use a disk. The changing of hanging mass, rotating mass and the torque radius affect on the angular acceleration. By changing one of those parameters and remaining others, we can find out how the chosen parameter will change the angular acceleration. For example, we can derive the influence of radius change by change the pulley’s size, which is made of the same material. After determining every parameters, we can finally find out how the changing of hanging mass, rotating mass and the torque radius will influence on the angular acceleration and verify it by the equation I*α=Torque where α stands for the angular acceleration. Setup: Set experiment devices as the following photo. Procedure: Measure the required parameters. Here are these para...

22-May-2017: Lab 17: PHYSICCS 4A LAB--Finding the moment of inertia of a uniform triangle.

Lab 17 Purpose: To determine the moment of inertia of a right triangular thin plate around its center of mass, for two perpendicular orientations of the triangle. Introduction: In this lab, we will examine the parallel axis theorem with a special case. We will determine the moment of inertia of a right triangular at its edge. Then we will use parallel axis theorem to determine the moment of inertia around its center of mass. Comparing the result with the result of calculating the triangular part by evaluating the whole system’s moment of inertia. By comparing these two results, we can derive the conclusion that these two concepts are equal to each other in this lab. Setup Set the equipment up like the figure below. Mount the triangle on a holder and disk. The upper disk floats on a cushion of air. Process: Using LoggerPro to collect data when the apparatus is in the angular acceleration. Use the equation from Lab 16 as told in the guidance to derive the mom...

Lab 8- Deriving a Model from Friction

Purpose:  The purpose of this lab is create a model to determine the behavior of an object when friction is involved. Purpose In this lab, we did five different experiments involving friction: static friction, kinetic friction, static friction friction from a sloped surface, kinetic friction from sliding block down an incline and predicting the acceleration of a two-mass system. We used the derivation and measurement and capture the appropriate graphs to explain how we can get the friction from each section of the lab in order to find each friction of experimental values compared to the theoretical values. (1) Static Friction Static friction describes the friction force acting between two bodies when are not moving relative to one another. The coefficient of static friction is defined as: procedure: In this static friction experiment, we added the mass m to the bottom shown a bit of time until the block just starts to slip. We run the experiment and record the a...