SPEED-MANIA
- r how we measure the velocity in
secondary-school physics nowadays? István Szittyai Szeged-Hódmezővásárhely László Németh School TPI-2015, Budapest
SPEED-MANIA or how we measure the velocity in secondary-school - - PowerPoint PPT Presentation
SPEED-MANIA or how we measure the velocity in secondary-school physics nowadays? Istvn Szittyai Szeged- Hdmezvsrhely Lszl Nmeth School TPI-2015, Budapest Digital measurements Grammar and High School Nmeth Lszl,
secondary-school physics nowadays? István Szittyai Szeged-Hódmezővásárhely László Németh School TPI-2015, Budapest
Grammar and High School „Németh László”,
Hódmezővásárhely
ELTE Physics Education Program (2013- ) Supervisor: prof. István Groma Support: Noise Group (Univ. Of Szeged) Research topic: Digital measurements in the physics
education
Systematically look for „Where? What? How?” can we
use
Favorite: the measurements, that is (nearly) impossible
with traditional (classical?) methods
Romania Serbia Croatia
Observation: this have additonal motivation for students! Main difficulty: usually quite expensive … These devices, instruments and methods are still
spreading:
Öveges-program (renewal of the science education) Geomatech-project (GeoGebra + some new methods) Some other projects and funds There are some cheap solutions, for example EDAQ 530
Developed by „Noise Group”, University of Szeged low-cost, compact and easy-to-use digital measurement
solution for schools
acceleration, Hall-sensor, termistors, …
free
The concept of velocity is not an easy notion in
secondary school
One of the first notions of physics at the age 12-13:
speed=distance/time, 𝑤 = 𝑡 𝑢
Distance, position, displacement … Instantaneous velocity: 𝑤 =
∆𝑦 ∆𝑢, if ∆𝑢 is „very small”
(Velocity is a vector … now irrelevant)
(if d is small enough …)
Group of students (age 12-13), measuring the velocity with photo-gate
Measuring acceleration! (in particular: )
The software generate the velocity-graph from the distance-graph
Collison on the air track (2 gliders, moving in the same direction)
Motion on a slope (air track with a spring on the bottom
WITH LASER DISTANCE MEASURE
Model: Toolcraft LDM 50 T Red laser (𝜇 = 650 nm) Range: 5 cm – 50 m Accuracy: ±1.5 mm Operation: time-of-flight principle
(𝑡 = 𝑑𝑢)
20 results can be stored Continous measurement
The speed of light in air: 𝒅 The inner height of the tube: 𝒆 The height of water: h Flight time: 𝒖 (or 𝒖/𝟑) The value measured by the instrument:
𝒕(> 𝐞 ‼). (Clearly: 𝑡 = 𝑑𝑢)
Refractive index of water: 𝒐 Some computation: 𝒐 =
𝒊+(𝒕−𝒆) 𝒊
𝒕 𝒊 =
𝒅 𝒘 − 𝟐 𝒊 + 𝒆 = 𝒐 − 𝟐 𝒊 + 𝒆
s = 0,3486h + 0,5251
0.450 0.500 0.550 0.600 0.650 0.700 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 S (m) h (m)
s(h) diagram
n=1.3486
DIRECTLY WITH SOUND INTENSITY SENSORS
If you have two sensors, connected to a date-logger The distance: 𝑒 Make some sudden noise from the side Thanks to the high sampling rate we can determine the
delay (Δ𝑢) between the signs
And from this, calculate the speed: 𝑑 = 𝑒/Δ𝑢 Its simple, fast and accurate enough in school In water?? In other gases?
Motion Detector, The Physics Teacher 40, 284 (2002)
𝑡 (at 24℃ )