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Umnica [9.8K]
3 years ago
8

Two wooden boxes of equal mass but different density are held beneath the surface of a large container of water. Box A has a sma

ller average density than box B. When the boxes are released, they accelerate upward to the surface. Which box has the greater acceleration?
Physics
2 answers:
Novay_Z [31]3 years ago
5 0

Answer:

Box A

Explanation:

Let mass of each wooden box =m

Density of box A=\rho_A

Density of box B =\rho_B

\rho_A

Density,\rho=\frac{m}{V}

V_A=\frac{m}{\rho_A}

V_B=\frac{m}{\rho_B}

Density of inversely proportional to volume.

The volume of box with smaller density is larger than the volume of box with large density.

V_A>V_B

When the boxes are submerged under water.

Then, the buoyant force=\rho_l Vg

Where V=Volume of displace fluid.

\rho=Density of fluid

Buoyant force of box A=\rho_lV_Ag

Buoyant force of box  B=\rho_lV_Bg

Force=Buoyant force

ma_A=\rho_lV_Ag

ma_B=\rho_lV_Bg

Acceleration is directly proportional to volume.

Therefore,the box with large volume has greater acceleration.

Hence, the box A has greater acceleration.

Crank3 years ago
3 0

Answer:

Explanation:

Let boxes A and B has equal mass of M and volume be Va and Vb

their density be da and db

given da < db

M / Va < M/Vb

Va> Vb

Buoyant force on box A in water = weight of displaced water

= volume of displaced water x density of water x g

= Va x d x g , d is density of water

Aa  = acceleration on box A

= buoyant force on A  / mass of A  

= Va x d x g / M

Similarly acceleration on box B

Ab = Va x d x g / M

Since Va > Vb

Aa > Ab

So box A will have greater acceleration.

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You have a pendulum clock made from a uniform rod of mass M and length L pivoting around one end of the rod. Its frequency is 1
drek231 [11]

The new oscillation frequency of the pendulum clock is 1.14 rad/s.

     

The given parameters;

  • <em>Mass of the pendulum, = M </em>
  • <em>Length of the pendulum, = L</em>
  • <em>Initial angular speed, </em>\omega _i<em> = 1 rad/s</em>

The moment of inertia of the rod about the end is given as;

I_i = \frac{1}{3} ML^2

The moment of inertia of the rod between the middle and the end is calculated as;

I_f = \int\limits^L_{L/2} {r^2\frac{M}{L} } \, dr = \frac{M}{3L} [r^3]^L_{L/2} =  \frac{M}{3L} [L^3 - \frac{L^3}{8} ] = \frac{M}{3L} [\frac{7L^3}{8} ]= \frac{7ML^2}{24}

Apply the principle of conservation of angular momentum as shown below;

I _i \omega _i = I _f \omega _f\\\\\frac{ML^2}{3} (1 \ rad/s)= \frac{7ML^2}{24} \times \omega _f\\\\\frac{24 \times ML^2}{3 \times 7 ML^2} (1 \ rad/s)= \omega _f\\\\1.14 \ rad/s = \omega _f

Thus, the new oscillation frequency of the pendulum clock is 1.14 rad/s.

Learn more about moment of inertia of uniform rod here: brainly.com/question/15648129

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