By Tom Schuster, Peter Park, and Jason Schachter - PowerPoint PPT Presentation

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By Tom Schuster, Peter Park, and Jason Schachter

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By Tom Schuster, Peter Park, and Jason Schachter. In loving memory of: Todd Greenberg ... The compressed spring is released, firing the first ball into a ... – PowerPoint PPT presentation

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Title: By Tom Schuster, Peter Park, and Jason Schachter


1
The Completion of a Circuit Using the Potential
Energy of a Spring Lab
  • By Tom Schuster, Peter Park, and Jason Schachter
  • In loving memory of
  • Todd Greenberg

2
The Setup
3
What We Want
  • To determine the spring constant using the
    concepts of conservation of energy, conservation
    of momentum, and projectile motion.
  • To determine the resistance of a bulb using Ohms
    Law.

4
The Way it Works
  • The compressed spring is released, firing the
    first ball into a collision with the second ball
    of equal mass.
  • In order to conserve momentum, the second ball is
    sent accelerating down the track.
  • The ball goes over a ramp into projectile motion
    with an initial velocity of both vertical and
    horizontal components.
  • The ball drops into a funnel lined with aluminum
    foil that is connected to a circuit, which is
    then completed.
  • When the circuit is completed, the bulb becomes
    illuminated.

5
What We Need (part 1)
  • Mass of each metal ball (m1, m2) (Triple-beam
    balance)
  • Distance between the top of the track and the
    ground (yi) (meter stick)
  • Distance between the top of the ramp and the
    ground (yf) (meter stick)
  • Horizontal distance between the ramp and the
    bottle (?x) (meter stick)
  • Time for the ball to travel from the ramp to the
    bottle (t) (stopwatch)
  • Angle of the slope of the ramp (?) (protractor)
  • Stretch distance of spring (x) (meter stick)

6
What We Need (part 2)
  • Voltage of the battery (Vt) (voltmeter)
  • Current of the circuit (it) (ammeter)
  • Resistance of the ball (Rball) (resistance meter)

7
The Physics (part 1)
  • Vx?x/t
  • VrVxcos?
  • .5mVi2mgyi .5mVf2mgyf
  • (m1m2, Vi20 m/s, Vf10m/s)
  • mVi1mVi2mVf1mVf2
  • .5kx2 .5mVf2
  • k?

8
The Physics (part 2)
  • VtitRt
  • RtRballRammeterRbulb
  • Rbulb?

9
What We Got
10
The Physics Again (part 1)
  • Vx(0.74 m)/(.14 s)
  • VxVcos(35º)
  • .5(0.0671 kg)Vi2(0.0671 kg)(9.8 m/s2)(0.916 m)
    .5(0.0671 kg)Vf2(0.0671 kg)(9.8 m/s2)(0.17 m)
  • (m1m2, Vi20 m/s, Vf10m/s)
  • (0.0671 kg)Vi1(0.0671 kg)(0 m/s)
  • (0.0671 kg)(0 m/s)(0.0671 kg)Vf2
  • .5k(0.028 m)2 .5(0.0671 kg)Vf2
  • k?

11
The Physics Again (part 2)
  • (1.4 V)(0.12 A)Rt
  • Rt(4.5 ohms)(5.1 ohms)Rbulb
  • Rbulb?

12
The Procedure is Answered!
  • Vx.51 m/s
  • Vr.62 m/s
  • V23.97m/s
  • V13.97 m/s
  • k 2312.15 N x M
  • Rbulb2.1 ohms

13
What Could Have Went Wrong
  • Collision between the two balls may not have been
    perfectly elastic, as the surface may have been
    sloped during the collision.
  • The ball experienced friction that was not
    accounted for on the track.
  • Human error when using the stopwatch.
  • -Because the time being determined was so
    small, the possibility of error is high.
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