Phys1101 - Introductory Physics 1
Phys1101 - Introductory Physics 1
College of Liberal Arts & Sciences

  • Introduction
  • Lecture 01
  • Lecture 02
    • Lecture 2, Part 1: Announcements
    • Lecture 2, Part 2: Units
    • Lecture 2, Part 3: Vector Introduction
    • Lecture 2, Part 4: Adding Vectors Graphically
    • Lecture 2, Part 5: Vector Addition Examples
    • Lecture 2, Part 6: Vector Component Introduction
    • Lecture 2, Part 7: Trigonometry
  • Lecture 03
    • Lecture 3, Part 1: Introduction
    • Lecture 3, Part 2: Where Were We
    • Lecture 3, Part 3: Vector Components in Detail
    • Lecture 3, Part 4: Scalar Component Description
    • Lecture 3, Part 5: Example of Finding Scalar Components
    • Lecture 3, Part 6: Scalar Component Addition
    • Lecture 3, Part 7: Scalar Addition Example
    • Lecture 3, Part 8: Motion Diagrams
  • Lecture 04
    • Lecture 4, Part 1: Introduction
    • Lecture 4, Part 2: Where Were We
    • Lecture 4, Part 3: Location Location Location …
    • Lecture 4, Part 4: How Fast ??? What Direction ???
    • Lecture 4, Part 5: Speeding Up? Slowing Down?
    • Lecture 4, Part 6: What Happens at a Turning Point?
  • Lecture 05
    • Lecture 5, Part 01: Introduction
    • Lecture 5, Part 02: Where Were We
    • Lecture 5, Part 03: Big Picture:  1D Kinematics
    • Lecture 5, Part 04: Kinematic Problem Solving Steps
    • Lecture 5, Part 05: Example 1
    • Lecture 5, Part 06: Example 2
    • Lecture 5, Part 07: Example 3
    • Lecture 5, Part 08: Free Fall
    • Lecture 5, Part 09: Free Fall and Kinematic Equations
    • Lecture 5, Part 10: Example 4
    • Lecture 5, Part 11: Example 5
  • Lecture 06
    • Lecture 6, Part 1: Introduction
    • Lecture 6, Part 2: Where Were We
    • Lecture 6, Part 3: Reading Quiz
    • Lecture 6, Part 4: Graph Basics
    • Lecture 6, Part 5: Practice Makes Perfect…
    • Lecture 6, Part 6: The Tangent Line
  • Lecture 07
    • Lecture 7, Part 1: Introduction
    • Lecture 7, Part 2: Where Were We
    • Lecture 7, Part 3: 2D Motion Diagrams
    • Lecture 7, Part 4: Trajectories
    • Lecture 7, Part 5: Why Work With Components…
    • Lecture 7, Part 6: Key Vectors in 2D
    • Lecture 7, Part 7: Watching 2D Motion
    • Lecture 7, Part 8: Dropping Versus Firing…
  • Lecture 08
    • Lecture 8, Part 1: Introduction
    • Lecture 8, Part 2: Where Were We
    • Lecture 8, Part 3: 2D Kinematic Problems:  The Big Picture
    • Lecture 8, Part 4: 2D Kinematic Problem Solving Steps
    • Lecture 8, Part 5: Example – Part a
    • Lecture 8, Part 6: Example – Part b
    • Lecture 8, Part 7: Your Turn
  • Lecture 09
    • Lecture 9, Part 1: Introduction
    • Lecture 9, Part 2: Where Were We
    • Lecture 9, Part 3: What is Special About Projectile Motion?
    • Lecture 9, Part 4: Example Part a
    • Lecture 9, Part 5: Example Part b
    • Lecture 9, Part 6: Example Part c
    • Lecture 9, Part 7: Your Turn
  • Lecture 10
    • Lecture 10, Part 1: Introduction
    • Lecture 10, Part 2: Where Were We
    • Lecture 10, Part 3: Dynamics:  Why Does Velocity Change?
    • Lecture 10, Part 4: Physical Interpretation of Newton’s Laws
    • Lecture 10, Part 5: What is a Force?
    • Lecture 10, Part 6: Mathematics of Newton’s 2nd Law
  • Lecture 11
    • Lecture 11, Part 1: Introduction
    • Lecture 11, Part 2: Where Were We
    • Lecture 11, Part 3: Free Body Diagram and Vector Nature of Newton’s 2nd Law
    • Lecture 11, Part 4: Common Forces:  Weight
    • Lecture 11, Part 5: Common Forces:  Tension
    • Lecture 11, Part 6: Common Forces:  Normal Force
    • Lecture 11, Part 7: Common Forces:  Friction
    • Lecture 11, Part 8: Problem Solving Steps
    • Lecture 11, Part 9: Example
  • Lecture 12
    • Lecture 12, Part 1: Introduction
    • Lecture 12, Part 2: Where Were We
    • Lecture 12, Part 3: Example 1
    • Lecture 12, Part 4: Example 2
    • Lecture 12, Part 5: Example 3
  • Lecture 13
    • Lecture 13, Part 1: Introduction and Where Were We?
    • Lecture 13, Part 2: Why/When Do We Need Newton’s Third Law?
    • Lecture 13, Part 3: Newton’s 3rd Law
    • Lecture 13, Part 4: Changes To Our Problem-Solving Steps
    • Lecture 13, Part 5: Example 1
    • Lecture 13, Part 6: Ropes and Pulleys
    • Lecture 13, Part 7: Example 2
    • Lecture 13, Part 8: Your Turn
  • Lecture 14
    • Lecture 14, Part 01: Introduction
    • Lecture 14, Part 02: Where Were We ?
    • Lecture 14, Part 03: Uniform Circular Motion:  What You Need To Know
    • Lecture 14, Part 04: Example 1
    • Lecture 14, Part 05: Example 2
    • Lecture 14, Part 06: Example 3
    • Lecture 14, Part 07: Optional Roller Coaster Example
    • Lecture 14, Part 08: Satellite Example
    • Lecture 14, Part 09: The Universal Law of Gravitation
    • Lecture 14, Part 10: Satellite Example Continued
  • Lecture 15
    • Lecture 15, Part 1: Introduction and Where Were We?
    • Lecture 15, Part 2: Energy Conservation:  The Basics
    • Lecture 15, Part 3: How Do You Calculate the Net Work?
    • Lecture 15, Part 4: New Problem Solving Steps
    • Lecture 15, Part 5: Example 1
    • Lecture 15, Part 6: Example 2
    • Lecture 15, Part 7: Last Example
    • Lecture 15, Part 8: Final Quiz Questions…
  • Lecture 16
    • Lecture 16, Part 1: Introduction and Where Were We?
    • Lecture 16, Part 2: Defining Our New “Energy Conservation Starting Equation”
    • Lecture 16, Part 3: Defining Mechanical Energy
    • Lecture 16, Part 4: New Problem Solving Steps
    • Lecture 16, Part 5: First Example
    • Lecture 16, Part 6: Second Example
    • Lecture 16, Part 7: Last Example
    • Lecture 16, Part 8: Redo Example From Last Lecture
  • Lecture 17
    • Lecture 17, Part 1: Lecture
  • Lecture 18
    • Lecture 18, Part 1: Introduction and Where Were We?
    • Lecture 18, Part 2: Momentum Change of a Single Object
    • Lecture 18, Part 3: Conservation of Momentum
  • Lecture 19
    • Lecture 19, Part 1: Introduction and Where Were We?
    • Lecture 19, Part 2: Let’s Start With Another Example
    • Lecture 19, Part 3: Elastic Collisions
    • Lecture 19, Part 4: Remaining Quiz Questions
  • Lecture 20
    • Lecture 20, Part 1: Introduction and Where Were We?
    • Lecture 20, Part 2: Rotational Kinematics:  The Basics
    • Lecture 20, Part 3: Examples
  • Lecture 21
    • Lecture 21, Part 1: Introduction and Where Were We?
    • Lecture 21, Part 2: Describing Motion ALONG the Circular Path…
    • Lecture 21, Part 3: Examples
    • Lecture 21, Part 4: Rolling Motion
  • Lecture 22
    • Lecture 22, Part 1: Introduction and Where Were We?
    • Lecture 22, Part 2: A Net Torque Causes Angular Acceleration
    • Lecture 22, Part 3: Torque Example
    • Lecture 22, Part 4: Equilibrium Example
    • Lecture 22, Part 5: Moment of Inertia
    • Lecture 22, Part 6: Non-Equilibrium Example
    • Lecture 22, Part 7: Another Example
  • Lecture 23
    • Lecture 23, Part 1: Introduction and Where Were We?
    • Lecture 23, Part 2: The Basics of Oscillatory Motion
    • Lecture 23, Part 3: Hooke’s Law
    • Lecture 23, Part 4: Kinematics of Simple Harmonic Motion
    • Lecture 23, Part 5: Example
  • Lecture 24
    • Lecture 24, Part 1: Lecture
  • Lecture 25
    • Lecture 25, Part 1: Introduction
    • Lecture 25, Part 2: The Basics of Wave Motion
    • Lecture 25, Part 3: Motion of a Particle on a Wave
    • Lecture 25, Part 4:  Motion of The Wave Crest
    • Lecture 25, Part 5: Examples
Lecture 06 » Lecture 6, Part 5: Practice Makes Perfect…

Lecture 6, Part 5: Practice Makes Perfect…

https://youtu.be/2qwgz3OPjEU

PHYS 1101: Lecture Six, Part Five

Okay. Let’s just practice, practice, practice now. Go through several examples, and we’re going to make these quiz questions, and I’m going to help you through the first ones as we start.

One of the first tricks I want to point out is perhaps something you can sketch along your graph to help you picture the motion. I’m going to make this a little bit smaller, so I have room. We’re used to looking at these motion diagrams now. Usually, for x, for example, we’re looking at that horizontal motion. So, imagine that you turn your page. If you printed out your notes, do a rough sketch of this graph, and then rotate your page so that this line is horizontal.

When that line is horizontal, then above this, I’m going to think of sketching in my motion diagram for that object. Well, what do I know? What do I know? At the initial time, the object was at +2 meters. At the initial time, here’s my origin, the object is here. Then, I know one second later, it’s moved to the next position, 3. Another second later, it’s moved to 4. Another second, looks like it’s about up to 5.

Well, then what happens? In the next second, it now goes back to near the origin. It’s now heading back toward the origin, and it looks like in the next second, I travel pretty far. I travel 1, 2, 3 meters. So, in the next second, let me just repeat this point right up here, so I double back on myself. In the next second, I travel all the way back to this point.

Looks like for the next second, I stand there. So, that would be another point there. Now, I continue heading back to the origin. In fact, I continue heading now in the direction of negative x values.

So, if I go in and add some velocity vectors between my motion diagram, it really helps me to tie this plot to more of a visual picture of what that object is doing. If I do that, I think it’s a lot easier than to answer these questions. So, given this motion diagram, I started here. Here was t equals 0. I did something like this. I’ve even been able to convey the rough size of the velocity at different intervals. Does that object ever turn around? And if so, when?

Okay. Next question. You’re looking at the same plot. Here, it’s asking you about the velocity, and is the velocity ever negative. Well, if you’ve gone through that exercise to do a quick motion diagram, you could go back and look at these velocity vectors, and you could say to yourself, “Okay. A negative velocity means that this vector has to point in the negative direction. And you know what? It does point in the negative direction for part of this motion. Let’s see. When did that start? That started here, after the first three seconds when the object turned around.”

Another way to recognize the sign of velocity is just to think about the slope again. You glance at this plot, x versus time, and you look at the slope of these segments. It’s telling you the velocity. This is a positive slope, positive velocity. The slope here, negative, velocity in the negative direction, etc. Okay. So, that should help you with Question 7.

Okay, question 8, at first, appears to be a question that we’ve already answered. But, here’s where I ask you to slow down. This is a plot now of velocity versus time. To help orient yourself to this, I might just suggest that you start out drawing some velocity vectors, this is velocity versus time, to then help you somewhat picture what’s going on.

The first velocity vector I need to draw is kind of small, has a length of about 2 meters per second, but it’s positive. Let’s make that represent 2 meters per second. The next second later, the velocity has increased to 3 meters per second. As time continues on, it increases further and further. At this highest point, the velocity, note it’s still positive. We’re still above the origin. It’s just getting smaller. Velocity keeps getting slower.

Eventually, it gets even less than, looks like it’s starting less than where we started, so slightly shorter than where we started. And now, the velocity keeps getting smaller, goes to 0. Now, the graph is telling me that for these times . . . Let me highlight that in orange maybe. For example, at this time, my curve is below the line. That means my velocity is now in the negative region. So, on my plot, that means my velocity did this. It eventually went to 0, and then it flipped sign. Okay. That might help you there.

Question 9. Does the object ever stand still? And if so, during what segment? Again, slow down. We’re back to thinking about x versus time. Go back or do your motion diagram here, and see if you can then answer this question.

Okay, question 10. When is the object going the fastest? You’re asked that question, and you’re looking at the direct velocity versus time. Remember the value of velocity. That is a number that represents how fast you’re going. When is it going the fastest?

Question 11. You have two objects here. You’re looking at the plot of the position versus time for these two objects. You’re asked about the speed. Remember, speed is the magnitude of velocity. How is velocity related to a plot of x versus t? You got to think slow. I’ll leave that to you to answer that one now.

Alright. I want you to now try to go in the other direction, and I don’t know how to ask you to practice this other than what I’ve done here. You now have some practice of looking at a graph and reading the graph and trying to interpret what the motion looks like. Can you go the other direction? If I describe some motion to you, can you generate a graph that represents that motion?

So, read this discussion here, this description of motion, and then generate that graph on a piece of paper. I can’t think of a good way of having you submit that to me electronically, unless all of you have scanners, which you may not. The next best thing is to ask you to, using text, to just describe that graph to me in words. Be as specific as you can. You’re looking at your graph. Tell me what direction your axes are, what numbers are at various positions on your graph, and what does your line look like that you’ve drawn on your graph. Be as specific as you can.

Okay. To again further your skill in being able to graph something, given the physical description, for the same motion, now instead of graphing x versus t, graph the velocity versus time for me, for that object, for that four-second interval. Describe that graph, and again, be as specific as you can.

Okay. The last three questions here have to do with getting a feeling for acceleration and how you can look at a graph and say something about the object, whether the object is speeding up or slowing down. You’ve got four questions to ask about that, to answer about that. The only reminder I’m going to give you is that the acceleration is v minus v0 over Δt. It’s the slope on a v versus t curve.

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