Respuesta :
Answer:
Let A represent the more massive piece, and B the less massive piece. Thus
Ma = 3 Mb
In the explosion, momentum is conserved. We have
Va = V2 = 0
Pin = Pfinal
0 = MaVa + Mb Vb
= 3MbVa + Mb Vb
Va = - 1/3 x Vb
For each block, the kinetic energy gained during the explosion is lost to negative work done by friction on the block.
Wfr = KEf - KEi = -1/2 mbv^2
But work is also calculated in terms of the force doing the work and the distance traveled.
Mfr = Ffr delta x cos 180 degrees
= -Uk Fn x delta x = -Ukmg x delta x
Equate the two work expressions, solve for the distance traveled, and find the ratio of distances.
_-1/2mv^2 = -Uk mg x delta x
Delta x = v^2 / gUx
Delta Xa / delta Xb = (- 1/3 x Vb)^2 / Vb ^2 = 1/9
And so
(Delta x)heavy / (delta x ) light = 1/9
The energy and momentum of the sliding blocks are assumed to be conserved
- The ratio of the distances traveled by the blocks m₁, and m₂, is 1 : 9
Reason:
Known parameters;
Mass of one piece of the wooden block, m₁ = 3 × Mass of other piece, m₂
Location of firecracker = Depression made in the pieces
Required:
The ratio of the distances traveled by each block when the fire cracker slide apart
Solution:
Let v₁ and v₂ represent the speed with which the blocks m₁ and m₂ slide apart, we have;
(m₁ + m₂) × v = m₁·v₁ + m₂·v₂
The initial velocity of the blocks, v = 0, therefore;
(m₁ + m₂) × 0 = 0 = m₁·v₁ + m₂·v₂
m₁·v₁ = -m₂·v₂
m₁ = 3·m₂, therefore;
3·m₂ × v₁ = -m₂·v₂
3·v₁ = -v₂
Distance = Velocity, v × Time, t
The distance traveled by each block in the same time, t, d₁, and d₂, are given as follows;
The kinetic energy of the block, m₁, K.E.₁ = 0.5·m₁·v₁²
Work done by friction for block, m₁ = μ·m₁·g·d₁
The kinetic energy of the block, m₂, K.E.₂ = 0.5·m₂·v₂²
Work done by friction for block, m₂ = μ·m₂·g·d₂
Where;
μ = Coefficient of dynamic friction
Therefore, by the law of conservation of energy, we have;
0.5·m₁·v₁² = μ·m₁·g·d₁
0.5·m₂·v₂² = 0.5·m₁/3·(-3·v₁)² = 3·0.5·m₁·v₁²
[tex]\dfrac{1}{2} \cdot m_2 \cdot v_2^2 = \dfrac{1}{2} \cdot \dfrac{m_1}{3} \cdot 9 \cdot v_1^2 = \dfrac{3}{2} \cdot {m_1} \cdot v_1^2[/tex]
[tex]\dfrac{3}{2} \cdot {m_1} \cdot v_1^2 = \mu \cdot m_2 \cdot g \cdot d_2 = \dfrac{\mu}{3} \cdot m_1 \cdot g \cdot d_2[/tex]
From 0.5·m₁·v₁² = μ·m₁·g·d₁, we have;
[tex]\dfrac{3}{2} \cdot {m_1} \cdot v_1^2 = 3 \cdot \mu \cdot m_1 \cdot g \cdot d_1[/tex]
Therefore;
[tex]3 \cdot \mu \cdot m_1 \cdot g \cdot d_1 = \dfrac{\mu}{3} \cdot m_1 \cdot g \cdot d_2[/tex]
9·d₁ = d₂
[tex]\dfrac{d_2}{d_1} = \dfrac{9}{1}[/tex]
Therefore, the ratio of the distances the blocks m₁, and m₂ travels, which is d₁ : d₂ = 1 : 9
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