A MATERIAL POINT WITH MASS M SLIPS FRICTIONLESS OVER THE SURFACE OF A FIXED HALF-CYLINDER WITH RADIUS R. WE DENOTE BY g THE ACCELERATION O.... A material point with mass M slips frictionless over the surface of a fixed half-cylinder with radius R. We denote by g the acceleration of gravity. The material point M is initially at point A (cylinder top). It is launched gently with an initial horizontal velocity Vo. We suppose that the material point keeps contact with the surface of the cylinder. The relationship between the velocity V of the mass M and the angle that defines its position is: M V²-V2-2gR(1-cose) None of the above answers V² = V²+2gR(1 — cose) V² = V²+2gR(1 + cose) V² = V² -2gR(1 + cose)

Elements Of Electromagnetics
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A MATERIAL POINT WITH MASS M SLIPS FRICTIONLESS OVER THE SURFACE OF A FIXED HALF-CYLINDER WITH RADIUS R. WE DENOTE BY g THE ACCELERATION O...
y
A material point with mass M slips frictionless over the surface of a fixed half-cylinder with radius R. We denote by g the acceleration of gravity. The material point M is initially at point
A (cylinder top). It is launched gently with an initial horizontal velocity Vo. We suppose that the material point keeps contact with the surface of the cylinder. The relationship between
the velocity V of the mass M and the angle that defines its position is:
0
V² = V2 -2gR(1 - cose)
None of the above answers
V² = V² + 2gR(1 - cose)
V² = V² + 2gR(1 + cose)
V² = V² - 2gR(1 + cose)
+1
R
Transcribed Image Text:A MATERIAL POINT WITH MASS M SLIPS FRICTIONLESS OVER THE SURFACE OF A FIXED HALF-CYLINDER WITH RADIUS R. WE DENOTE BY g THE ACCELERATION O... y A material point with mass M slips frictionless over the surface of a fixed half-cylinder with radius R. We denote by g the acceleration of gravity. The material point M is initially at point A (cylinder top). It is launched gently with an initial horizontal velocity Vo. We suppose that the material point keeps contact with the surface of the cylinder. The relationship between the velocity V of the mass M and the angle that defines its position is: 0 V² = V2 -2gR(1 - cose) None of the above answers V² = V² + 2gR(1 - cose) V² = V² + 2gR(1 + cose) V² = V² - 2gR(1 + cose) +1 R
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