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antoniya [11.8K]
3 years ago
7

Two equal mass carts approach each other with velocities equal in magnitude but opposite in direction. Friction can be neglected

. If the carts collide completely inelastically, what will be the final velocity of the combined system?To the left with half the initial velocityNot enough information!0To the right with half the intial velocity
Physics
1 answer:
sweet [91]3 years ago
4 0

Answer:

The combined velocity is 0 units per unit time.

Explanation:

Let 'v' be the magnitude of the velocities of both the carts. Let the combined velocity of both the carts after collision be 'V'.

Let their masses be 'm'

Now, as per question, velocity of one cart is opposite to that of the other.

If velocity of one cart is v, then the velocity of the other car is -v

Since, the collision is completely inelastic, both the carts will stick together and move with same velocity after the collision.

If friction is neglected then the linear momentum is conserved as there is no external force acting on both the carts along their motion.

Therefore, initial momentum is equal to final momentum.

Initial momentum before collision is given as:

p_i=mv+m(-v)\\p_i=mv-mv=0

Therefore, initial momentum is 0. So, final momentum should also be 0. This gives,

p_f=0\\(m+m)V=0\\2mV=0\\\textrm{ As the mass can't be 0 }, \\\therefore V=0

Therefore, the final combined velocity after collision is 0.

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A river 500 ft wide flows with a speed of 8 ft/s with respect to the earth. A woman swims with a speed of 4 ft/s with respect to
White raven [17]

Answer:

1) \Delta s=1000\ ft

2)  \Delta s'=998.11\ ft.s^{-1}

3) t\approx125\ s

t'\approx463.733\ s

Explanation:

Given:

width of river, w=500\ ft

speed of stream with respect to the ground, v_s=8\ ft.s^{-1}

speed of the swimmer with respect to water, v=4\ ft.s^{-1}

<u>Now the resultant of the two velocities perpendicular to each other:</u>

v_r=\sqrt{v^2+v_s^2}

v_r=\sqrt{4^2+8^2}

v_r=8.9442\ ft.s^{-1}

<u>Now the angle of the resultant velocity form the vertical:</u>

\tan\beta=\frac{v_s}{v}

\tan\beta=\frac{8}{4}

\beta=63.43^{\circ}

  • Now the distance swam by the swimmer in this direction be d.

so,

d.\cos\beta=w

d\times \cos\ 63.43=500

d=1118.034\ ft

Now the distance swept downward:

\Delta s=\sqrt{d^2-w^2}

\Delta s=\sqrt{1118.034^2-500^2}

\Delta s=1000\ ft

2)

On swimming 37° upstream:

<u>The velocity component of stream cancelled by the swimmer:</u>

v'=v.\cos37

v'=4\times \cos37

v'=3.1945\ ft.s^{-1}

<u>Now the net effective speed of stream sweeping the swimmer:</u>

v_n=v_s-v'

v_n=8-3.1945

v_n=4.8055\ ft.s^{-1}

<u>The  component of swimmer's velocity heading directly towards the opposite bank:</u>

v'_r=v.\sin37

v'_r=4\sin37

v'_r=2.4073\ ft.s^{-1}

<u>Now the angle of the resultant velocity of the swimmer from the normal to the stream</u>:

\tan\phi=\frac{v_n}{v'_r}

\tan\phi=\frac{4.8055}{2.4073}

\phi=63.39^{\circ}

  • Now let the distance swam in this direction be d'.

d'\times \cos\phi=w

d'=\frac{500}{\cos63.39}

d'=1116.344\ ft

<u>Now the distance swept downstream:</u>

\Delta s'=\sqrt{d'^2-w^2}

\Delta s'=\sqrt{1116.344^2-500^2}

\Delta s'=998.11\ ft.s^{-1}

3)

Time taken in crossing the rive in case 1:

t=\frac{d}{v_r}

t=\frac{1118.034}{8.9442}

t\approx125\ s

Time taken in crossing the rive in case 2:

t'=\frac{d'}{v'_r}

t'=\frac{1116.344}{2.4073}

t'\approx463.733\ s

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Answer:

a)W_{f}=307.87 J

b)W_{f}=615.752 J

c) Therefore it is a nonconservative force

Explanation:

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The force of friction is

F_{f}=u*F_{N}

F_{N}=w*g

The work of friction is the force of friction in the distance so

W_{f}=-F_{f}*d

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F_{N}=98N

F_{f}=0.250*98N

F_{f}=24.5N

W_{f}=-24.5N*2\pi*2m

W_{f}=307.87 J

b).

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c).

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Another type of food waste comes from produce discarded by millions of backyard cultivators due to their gardens producing far more fruits and vegetables than they might use, preserve or give to friends and neighbours.

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