Berkas:Rolling_Racers_-_Moment_of_inertia.gif
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Rolling_Racers_-_Moment_of_inertia.gif (480 × 270 piksel, ukuran berkas: 1,6 MB, tipe MIME: image/gif, melingkar, 126 frame, 4,2 d)
Berkas ini berasal dari Wikimedia Commons dan mungkin digunakan oleh proyek-proyek lain. Deskripsi dari halaman deskripsinya ditunjukkan di bawah ini.
DeskripsiRolling Racers - Moment of inertia.gif |
The objects are, from back to front:
At any moment in time, the forces acting on each object will be its weight, the normal force exerted by the plane on the object and the static friction force. As the weight force and the normal force act on a line through each object's center of mass, they result in no net torque. However, the force due to friction acts perpendicular to the contact point, and therefore it does result in a torque, which causes the object to rotate. Since there is no slipping, the object's center of mass will travel with speed , where r is its radius, or the distance from a contact point to the axis of rotation, and ω its angular speed. Since static friction does no work, and dissipative forces are being ignored, we have conservation of energy. Therefore: Solving for , we obtain: Since the torque is constant we conclude, by Newton's 2nd Law for rotation , that the angular acceleration α is also constant. Therefore: Where, v0 = 0 and d is the total distance traveled. Therefore, we have: For a ramp with inclination θ, we have sin θ = h / d. Additionally, for a dimensionless constant k characteristic of the geometry of the object. Finally, we can write the angular acceleration α using the relation : This final result reveals that, for objects of the same radius, the mass the object are irrelevant and what determines the rate of acceleration is the geometric distribution of their mass, which is represented by the value of k. Additionally, we observe that objects with larger values of k will accelerate more slowly. This is illustrated in the animation. The values of k for each object are, from back to front: 2/3, 2/5, 1, 1/2. As predicted by the formula found above, the solid ball will have a larger acceleration, reaching the finish line first. |
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Tanggal | ||||
Sumber | Karya sendiri | |||
Pembuat | Lucas Vieira | |||
Izin (Menggunakan kembali berkas ini) |
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Versi lainnya | OGG Theora Video: small and [[:File:Rolling Racers - Moment of inertia (HD).ogv|large (HD) and for classroom educational purposes a static image of the finish at File:Rolling Racers - Moment of inertia Photofinish.jpg ]] |
POV-Ray source code
Available at the video version's description page.
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Items portrayed in this file
menggambarkan
23 Desember 2012
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Riwayat berkas
Klik pada tanggal/waktu untuk melihat berkas ini pada saat tersebut.
Tanggal/Waktu | Miniatur | Dimensi | Pengguna | Komentar | |
---|---|---|---|---|---|
terkini | 16 Juni 2021 21.01 | 480 × 270 (1,6 MB) | TomFryers | Improve render quality and increase resolution and framerate slightly | |
23 Desember 2012 03.10 | 444 × 250 (1,49 MB) | LucasVB | {{Information |Description=... |Source={{own}} |Date=2012-12-23 |Author= Lucas V. Barbosa |Permission={{PD-self}} |other_versions=OGG Theora video }} |
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