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leonid [27]
3 years ago
14

A body 'A' of mass 1.5kg travelling along the positive X-axis with speed of 4.5m/s collides with another body 'B' of mass 3.2kg,

which initially is at rest as a result of the collision, 'A' is deflected and moves in a speed of 2.1m/s in a direction which is at an angle of 30 degree below the X-axis. 'B' is set in motion at an angle Φ above the X-axis. calculate the velocity of 'B' after the collision.
Physics
1 answer:
Dominik [7]3 years ago
8 0
We can solve this problem using only the law of conversion of energy. Because you don't need to calculate the angle \phi you don't have to deal with momentum and this makes this problem a lot easier. A good portion of the information about the problem is redundant. We have masses of both bodies and velocity of body A before and after the collision. You can see that it's velocity decreased, that's because some of it's initial energy was transferred to body B. 
Let us write down the law of conversion of energy.
\frac{m_av_a^2}{2} = \frac{m_av'_a^2}{2} + \frac{m_bv_b^2}{2}
m_bv_b^2=m_a(v_a^2-v'_a^2)
v_b= \sqrt{ \frac{m_a(v_a^2-v'_a^2)}{m_b} }
The final answer is: 
v_b=2.72 \frac{m}{s}
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8. An unpowered flywheel is slowed by a constant frictional torque. At time t = 0 it has an angular velocity of 200 rad/s. Ten s
allsm [11]

Answer:

a) \omega = 50\,\frac{rad}{s}, b) \omega = 0\,\frac{rad}{s}

Explanation:

The magnitude of torque is a form of moment, that is, a product of force and lever arm (distance), and force is the product of mass and acceleration for rotating systems with constant mass. That is:

\tau = F \cdot r

\tau = m\cdot a \cdot r

\tau = m \cdot \alpha \cdot r^{2}

Where \alpha is the angular acceleration, which is constant as torque is constant. Angular deceleration experimented by the unpowered flywheel is:

\alpha = \frac{170\,\frac{rad}{s} - 200\,\frac{rad}{s} }{10\,s}

\alpha = -3\,\frac{rad}{s^{2}}

Now, angular velocities of the unpowered flywheel at 50 seconds and 100 seconds are, respectively:

a) t = 50 s.

\omega = 200\,\frac{rad}{s} - \left(3\,\frac{rad}{s^{2}} \right) \cdot (50\,s)

\omega = 50\,\frac{rad}{s}

b) t = 100 s.

Given that friction is of reactive nature. Frictional torque works on the unpowered flywheel until angular velocity is reduced to zero, whose instant is:

t = \frac{0\,\frac{rad}{s}-200\,\frac{rad}{s} }{\left(-3\,\frac{rad}{s^{2}} \right)}

t = 66.667\,s

Since t > 66.667\,s, then the angular velocity is equal to zero. Therefore:

\omega = 0\,\frac{rad}{s}

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3 years ago
Calcium is combined with Nitrogen in a chemical reaction. The formula of the compound created, Calcium Nitride, is
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3 0
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4 years ago
Is it possible to add three vectors of equal magnitude but a different direction to get a null vector?
Sauron [17]

Answer:

Yes, it is possible to add three vectors of equal magnitudes and get zero. This can happen if the resultant of the two vectors are equal and opposite in direction to the third vector.

5 0
4 years ago
What is the upper block's acceleration if the coefficient of kinetic friction between the block and the table is 0.16?
Gekata [30.6K]
(Missing figure is here: https://www.physicsforums.com/attachments/ch05-p070-jpg.149243/ )

Let's call m_1 = 1.0 kg and m_2=2.0 kg the masses of the two blocks. We can write Newton's second law for both blocks (sum of all forces acting on the block = ma). On block 1, we have two forces: the weight m_1 g pointing downwards and the tension of the string T poiting upwards. On block 2, we have the tension of the string going right and the friction \mu m_2 g going left. Therefore

m_1 g - T = m_1 a
T-\mu m_2 g = m_2 a

Summing the two equations, we find
m_1 g - \mu m_2 g = (m_1 + m_2) a
and then using \mu=0.16 we can find the acceleration:
a= \frac{m_1 g - \mu m_2 g}{m_1 + m_2}=2.22 m/s^2


6 0
3 years ago
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