A 0.060 ???????? tennis ball, moving with a speed of 5.28 m/???? , has a head-on collision with a 0.080 ???????? ball initially moving in the same direction at a speed of 3.00 m/ ???? . Assume that the collision is perfectly elastic. Determine the velocity (speed and direction) of both the balls after the collision.

Answers

Answer 1
Answer:

Explanation:

It is given that,

Mass of the tennis ball, m_1=0.06\ kg

Initial speed of tennis ball, u_1=5.28\ m/s

Mass of ball, m_2=0.08\ kg

Initial speed of ball, u_2=3\ m/s

In case of elastic collision, the momentum remains conserved. The momentum equation is given by :

m_1u_1+m_2u_2=m_1v_1+m_2v_2

v_1\ and\ v_2 are final speed of tennis ball and the ball respectively.

0.06* 5.28+0.08* 3=0.06v_1+0.08v_2

0.06v_1+0.08v_2=0.5568..............(1)

We know that the coefficient of restitution is equal to 1. It is given by :

(v_2-v_1)/(u_1-u_2)=1

(v_2-v_1)/(5.28-3)=1

{v_2-v_1}=2.28.................(2)

On solving equation (1) and (2) to find the values of velocities after collision.

v_1=5.28\ m/s

v_2=3\ m/s

So, the speed of both balls are 5.28 m/s and 3 m/s respectively. Hence, this is the required solution.


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e. All three have zero pressure at the bottom.

Answers

Answer:

d

Explanation:

Pressure of the fluid in any container is a function of density of the fluid in the container, and depth of the fluid.

The static pressure of fluid in a container with depth h is given by:

P = p * g* h

Where p : density of fluid

g: gravitational constant 9.81 m/s^2

h : depth of the fluid

Since, all the glasses filled have same Area base, same depth and same density of fluid and g is constant. The pressure at the bottom of each drinking glass is equal for all cases. As supported by the relationship given above.  

A small ball of mass m is held directly above a large ball of mass M with a small space between them, and the two balls are dropped simultaneously from height H. (The height is much larger than the radius of each ball, so you may neglect the radius.) The large ball bounces elastically off the floor and the small ball bounces elastically off the large ball. a) For which value of the mass m, in terms of M, does the large ball stop when it collides with the small ball? b) What final height, in terms of H, does the small ball reach?

Answers

a) The large sphere has 3 times the mass of the small sphere

b)   The final height at which small ball reach y = 4H

What will be the mass of the sphere and height covered by the small ball?

We must start this problem by calculating the speed with which the spheres reach the floor

V_f^2=V_o^2-2gy      

As the spheres are released v₀ = 0

V_f^2=2gH      

V_f=√(2gH)      

The two spheres arrive at the same speed to the floor.

The largest sphere clashes elastically so that with the floor it has a much higher mass, the sphere bounces with the same speed with which it arrived, the exit speed of the  spheres

V_(10)=\sqrt2gH    

The big sphere goes up and the small one down, the two collide, let's form a system that contains the two spheres, let's use moment conservation

Let's call

V_h=\sqrt2gH

Small sphere m₂ and  V_(20)=-\sqrt2gH=-V_h

Large sphere m₁ and  V_(10)=√(2gH)=V_h  

Before crash

P_o=m_1V_(10)+m_2V_(20)      

After the crash

P_f=m_1V_(1f)+m_2V_(2f)    

   

P_o=P_f  

   

m_1V_(10)+m_2V_(20)=m_1V_(1f)+m_2V_(2f)  

The conservation of kinetic energy

K_o=(1)/(2) m_1V_(10)^2+(1)/(2) m_2V_(20)^2      

K_f=(1)/(2) m_1V_(1f^2)+(1)/(2) m_2V_(2f)^2    

K_o=K_f  

K_o=(1)/(2) m_1V_(10)^2+(1)/(2) m_2V_(20)^2  =  K_f=(1)/(2) m_1V_(1f^2)+(1)/(2) m_2V_(2f)^2    

Let's write the values

-m_1V_h+m_2V_h=m_1V_(1f)+m_2V_(2f)    

 m_1V_h^2+m_2V_h^2=m_1V_(1f)^2+m_2V_(2f)^2

 

The solution to this system of equations is

m_t=m_1+m_2    

V_(1f)=((m_1-m_2))/(m_tV_(10)) +(2m_2)/(m_tV_2)      

V_(2f)=(2m_1)/(m_tV_(10)) +(m_2-m_1)/(m_tV_2)        

The large sphere is labeled 1, we are asked for the mass so that  V_(1f) = 0, let's clear the equation

V_(1f)=(m_1-m_2)/(m_tV_(10)) +(2m_2)/(m_tV_(20))      

0=(m_1-m_2)/(m_tV_h) +(2m_2)/(m_t(-V_h))      

 

(m_1-m_2)/(m_tV_h) =(2m_2)/(m_tV_h)      

(m_1-m_2)=2m_2    

m_1=3m_2      

The large sphere has to complete 3 times the mass of the sphere1 because it stops after the crash.

b) Let us calculate with the other equation the speed with which the sphere comes out2 (small)

  V_(2f)=(2m_1)/(m_tV_(10)) +(m_2-m_1)/(m_tV_(20))    

 

V_(2f)=(2m_1)/(m_tV_h) +(m_2-m_1)/(m_t(-V_h))

In addition, we know that m₁ = 3 m₂

m_t=3m_2+m_2  mt = 3m2 + m2

m_t=4m_2    

     

V_(2f)=(2* 3m_2)/(4m_2V_h-(m_2-3m_2)4m_2V_h)  

   

V_(2f)=(3)/(2) V_h+(1)/(2) V_h  

       

V_(2f)=2V_h

V_(2f)=2\sqrt{2gh        

This is the rate of rising of sphere 2 (small. At the highest point, it zeroes velocity V_f= 0

V^2=V_(2f)^2-2gy  

0=(2√(2gh))^2-2gy        

       

y=4H

Thus

a) The large sphere has 3 times the mass of the small sphere

b)   The final height at which small ball reach y = 4H

To know more about the Laws of collisions follow

brainly.com/question/7538238

Answer:

a) the large sphere has 3 times the mass of the small sphere

b)     y = 4H

Explanation:

We must start this problem by calculating the speed with which the spheres reach the floor

       vf² = vo² - 2g y

As the spheres are released v₀ = 0

      vf² = - 2g H

      vf = √ (2g H)

The two spheres arrive with the same speed to the floor.

The largest sphere clashes elastically so that with the floor it has a much higher mass, the sphere bounces with the same speed with which it arrived, the exit speed of the  spheres

     V₁₀ = √2gH

The big sphere goes up and the small one down, the two collide, let's form a system that contains the two spheres, let's use moment conservation

Let's call vh = √2gH

Small sphere m₂ and v₂o = - √2gH = -vh

Large sphere m₁ and v₁o = √ 2gh = vh

Before crash

        p₀ = m₁ v₁₀ + m₂ v₂₀

After the crash

      pf = m₁ v₁f + m₂ v₂f

      po = pf

      m₁ v₁₀ + m₂ v₂₀ = m₁ v₁f + m₂ v₂f

The conservation of kinetic energy

      Ko = ½ m₁ v₁₀² + ½ m₂ v₂₀²

      Kf = ½ m₁ v₁f² + ½ m₂ v₂f²

      Ko = KF

      ½ m₁ v1₁₀² + ½ m₂ v₂₀² = ½ m₁ v₁f² + ½ m₂ v₂f²

Let's write the values

      -m₁ vh + m₂ vh = m₁ v₁f + m₂ v₂f

       m₁ vh² + m₂ vh² = m₁ v₁f² + m₂ v₂f²

The solution to this system of equations is

       mt = m₁ + m₂

       v1f = (m₁-m₂) / mt v₁₀ + 2m₂ / mt v₂

       v₂f = 2m₁ /mt v₁₀ + (m₂-m₁) / mt v₂

The large sphere is labeled 1, we are asked for the mass so that v1f = 0, let's clear the equation

       v₁f = (m₁-m₂) / mt v₁₀ + 2m₂ / mt v₂₀

        0 = (m₁-m₂) / mt vh + 2 m₂ / mt (-vh)

       (m₁-m₂) / mt vh = 2 m₂ / mt vh

       (m₁-m₂) = 2m₂

        m₁ = 3 m₂

The large sphere has to complete 3 times the mass of the sphere1 because it stops after the crash.

b) Let us calculate with the other equation the speed with which the sphere comes out2 (small)

        v₂f = 2m₁ / mt v₁₀ + (m₂-m₁) / mt v₂₀

        v₂f = 2 m₁ / mt vh + (m₂-m₁) mt (-vh)

In addition, we know that m₁ = 3 m₂

        mt = 3m2 + m2

         mt= 4m2

        v₂f = 2 3m₂ / 4m₂ vh - (m₂-3m₂) 4m₂ vh

        v₂f = 3/2 vh +1/2 vh

        v₂f = 2 vh

        v₂f = 2 √ 2gh

This is the rate of rise of sphere 2 (small. At the highest point its zero velocity vf = 0

        V² = v₂f² - 2 g Y

          0 = (2√2gh)² - 2gy

        2gy = 4 (2gH)

         y = 4H

A hydrogen atom contains a single electron that moves in a circular orbit about a single proton. Assume the proton is stationary, and the electron has a speed of 7.5 105 m/s. Find the radius between the stationary proton and the electron orbit within the hydrogen atom.

Answers

Answer:

450 pm

Explanation:

The electron is held in orbit by an electric force, this works as the centripetal force. The equation for the centripetal acceleration is:

a = v^2 / r

The equation for the electric force is:

F = q1 * q2 / (4 * π * e0 * r^2)

Where

q1, q2: the electric charges, the charge of the electron is -1.6*10^-19 C

e0: electric constant (8.85*10^-12 F/m)

If we divide this force by the mass of the electron we get the acceleration

me = 9.1*10^-31 kg

a = q1 * q2 / (4 * π * e0 * me * r^2)

v^2 / r = q1 * q2 / (4 * π * e0 * me * r^2)

We can simplify r

v^2 = q1 * q2 / (4 * π * e0 * me * r)

Rearranging:

r = q1 * q2 / (4 * π * e0 * me * v^2)

r = 1.6*10^-19 * 1.6*10^-19 / (4 * π * 8.85*10^-12 * 9.1*10^-31 * (7.5*10^5)^2) = 4.5*10^-10 m = 450 pm

A 84-kg man stands on a spring scale in an elevator. Starting from rest, the elevator ascends, attaining its maximum speed of 1.2 m/s in 0.73 as. The elevator travels with this constant speed for 5.0 s, undergoes a uniform negative acceleration for 1.4 s, and then comes to rest.What does the spring scale register During the first 0.80s of the elevator’s ascent?

Answers

Answer:

SR=949.2N

Explanation:

From the question we are told that:

Mass M=84kg

Speed V=1.2m/s

Acceleration Time t_a=0.73

Constant speed Timet_s=5.0s

Deceleration time t_d=1.4s

Generally the equation for Acceleration is mathematically given by

a=(v)/(t)

Therefore acceleration for the first 0.80 sec is

a=(1.2)/(0.80)

a=1.5m/s^2

Therefore

Spring Reading=Normal force -Reaction

SR=m(g+a)

SR=84(9.8+1.5)

SR=949.2N

What is the difference between V(peak voltage) and Vrms (root-mean-square) of AC voltage source?

Answers

Answer:

V(peak voltage) is the highest voltage that the waveform will ever attain and the Vrms(root-mean-square) is the effective voltage of the total waveform representing the AC source.

A rabbit is moving in the negative x-direction at 1.10 m/s when it spots a predator and accelerates to a velocity of 13.9 m/s along the negative y-axis, all in 1.20 s. Determine the x-component and the y-component of the rabbit's acceleration. (Enter your answers in m/s2. Indicate the direction with the signs of your answers.) HINT

Answers

Answer:

Explanation:

Initial velocity u = -1.1 i  m /s ( along - ve direction )

final velocity = - 13.9 j

change in velocity = -13.9 j + 1.1 i

rate of change of velocity

acceleration

= (-13.9 j + 1.1 i) / 1.2

= -11.58 j + 0.916 i

x component

= 0.916 m /s²

y component

= - 11.58 m / s²