Work, Energy and Power
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New answer posted
2 months agoContributor-Level 9
a = k2rt2
? tangential force, Ft = mat = mkr
Note ® Power delivered by centripetal force will be zero.
New answer posted
2 months agoContributor-Level 10
According to conservation of energy, we can write
Gain in kinetic energy = Loss in potential energy
Kf – Kin = Uin - Uf
K - = mgy – mg (y – y0) = mgy0
New answer posted
2 months agoContributor-Level 10
ΔW = area under P — t graph
= (1/2) (4 + 6) * 7 = 35 J
Work done = change in KE ⇒ 35 = (1/2) * 2 * v² - (1/2) * 2 * (1)² ⇒ v = 6 m/s
New answer posted
2 months agoContributor-Level 10
U = kr² ⇒ F = -dU/dr = -2kr ; 2kr = mv²/r ⇒ v = √ (2k/m) or T = 2πr/v = 2π√ (m/2k)
New answer posted
2 months agoContributor-Level 10
To reach at point A particle must cross the peak point.
Loss in KE = gain in PE
v2 = 100
v = 10 m/s
New answer posted
2 months agoContributor-Level 10
From conservation of momentum
2 * 4 + 4 * 2 = 2v1 + 4v2
8 = v1 + 2v2 ….(1)
From conservation of energy
….(ii)
On solving
New answer posted
2 months agoContributor-Level 10
When relative sliding stops, both move with same velocity.
Only friction acts in horizontal direction.
∴ for system no external force, we can apply conservation of momentum.
1 * 12 + 5 * 0 = 6 * v
v = 2 m/s
Now work done by friction on block = change in kinetic energy of block
w = (1/2)m (2² - 12²) = (1/2) (1) (4 - 144) = (1/2) (-140) = -70 J
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