Archimedes Principle and bouyant force

In summary: Yes, you are correct. The volume of the casting without holes can be found by dividing the weight of the casting in air (6000 N) by the density of iron (7.87 g/cm^3) and then dividing by the acceleration due to gravity (9.8 m/s^2). This will give you the total volume of the casting. Then, you can subtract the volume of the casting without holes from the total volume to get the volume of the cavities in the casting.For 2, you are also correct. The three forces (buoyant force, weight of the car, and the upward force from the air in the front and rear wheels) must be balanced at the point of sinking. As water enters
  • #1
bodensee9
178
0
Hello:

Can someone help with the following 2 questions?

1. An iron casting containing a number of cavities weighs 6000 N in air and 4000 N in water. What's the total volume of all cavities in casting? The density of iron without cavities is 7.87 g/cm^3. The density of water is 988 kg/m^3.

Wouldn't the bouyant force = the mass of displaced water * g. So here, bouyant force = 6000 - 4000 = 2000. So wouldn't mass of displaced water = 2000/9.8. And doesn't this need to equal to the mass of the cavities? There seems to be something I'm missing.

2. The volume of air space in the passenger compartment of an 1800 kg car is 5 m^3. The volume of motor and front wheels is 0.750 m^3. The volume of the rear wheels, gas tank and trunk is .8 m^3. Water can't enter into the last 2 compartments (only the passenger compartment can water enter). As water enters, the car sinks. How many cubic meters of water are in the car as the car sinks?

To sink, the force must be greater than mg (1800*g). But I don't see the significance of the point of sinking? Since water can't enter into the rear wheels and front wheels, does this mean that there's an upward force equal to (.750+.8)*density of air*g? If anyone has any hints, that would be great.

Thanks.
 
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  • #2
bodensee9 said:
1. An iron casting containing a number of cavities weighs 6000 N in air and 4000 N in water. What's the total volume of all cavities in casting? The density of iron without cavities is 7.87 g/cm^3. The density of water is 988 kg/m^3.

Wouldn't the bouyant force = the mass of displaced water * g. So here, bouyant force = 6000 - 4000 = 2000. So wouldn't mass of displaced water = 2000/9.8. And doesn't this need to equal to the mass of the cavities? There seems to be something I'm missing.
You were on the right track, but mass of the displaced water does not equal to the mass of the cavities. But the volume of the casting equals to the volume of the displaced water. Try to continue from there.

bodensee9 said:
2. The volume of air space in the passenger compartment of an 1800 kg car is 5 m^3. The volume of motor and front wheels is 0.750 m^3. The volume of the rear wheels, gas tank and trunk is .8 m^3. Water can't enter into the last 2 compartments (only the passenger compartment can water enter). As water enters, the car sinks. How many cubic meters of water are in the car as the car sinks?

To sink, the force must be greater than mg (1800*g). But I don't see the significance of the point of sinking? Since water can't enter into the rear wheels and front wheels, does this mean that there's an upward force equal to (.750+.8)*density of air*g? If anyone has any hints, that would be great.

I don't really understand what this question is asking exactly, so I'll leave someone else to help you with it. How many cubic meters of water are in the car as the car sinks? At what point? If the car sinks, then the entire passenger compartment will be filled with water...
 
  • #3
Hi bodensee9,

bodensee9 said:
2. The volume of air space in the passenger compartment of an 1800 kg car is 5 m^3. The volume of motor and front wheels is 0.750 m^3. The volume of the rear wheels, gas tank and trunk is .8 m^3. Water can't enter into the last 2 compartments (only the passenger compartment can water enter). As water enters, the car sinks. How many cubic meters of water are in the car as the car sinks?

To sink, the force must be greater than mg (1800*g).

If you're talking about the buoyant force, don't you mean it must be less than the weight for the car to sink?

But I don't see the significance of the point of sinking? Since water can't enter into the rear wheels and front wheels, does this mean that there's an upward force equal to (.750+.8)*density of air*g?

No, the .75 and .8 is not the volume of the air in the tires; it's the total volume of the car that the water can't enter. (metal, rubber, etc.) What would the buoyant forces on them be?

The point of the passenger compartment is that as water enters, there is less and less water displaced by the passenger compartment, and so the buoyant force arising from the passenger compartment decreases as the water enters.

Right when the car is actually beginning to sink, what has to be true about the three buoyant forces? From that, you can tell how much air is still in the passenger compartment. What do you get?
 
  • #4
Hello

Thanks for the hints.

But for 1, if I know the volume of the casting 2000/(9.8*998 kg/m^3), I don't know how to find the volume of the holes in the casting? Should I find what the volume of a 6000 N casting without holes should be (6000/9.8*7.87) and then find the difference between the volume of the casting and the casting without holes?

For 2, should the three forces be balanced at the point of sinking? So we still have the upward force from .75 and .8, but we have downward force from whatever portion of the compartment with water?

Thanks.
 
  • #5
bodensee9 said:
But for 1, if I know the volume of the casting 2000/(9.8*998 kg/m^3), I don't know how to find the volume of the holes in the casting? Should I find what the volume of a 6000 N casting without holes should be (6000/9.8*7.87) and then find the difference between the volume of the casting and the casting without holes?

That sounds about right. First you have the volume of pure iron (assuming the holes don't weigh anything ;) ) and then you have the actual volume. The difference should be the volume of non-iron stuff.
 
  • #6
bodensee9 said:
For 2, should the three forces be balanced at the point of sinking? So we still have the upward force from .75 and .8, but we have downward force from whatever portion of the compartment with water?

That's fine to keep track of the weight of the water inside the compartment; but don't forget that there is an upward buoyant force dut to the 5 m^3 passenger compartment.
 
  • #7
Hello:

Okay ... thanks. So for the problem, does this mean that before the car sinks, the bouyant force will equal to mg? So if x cubic meter of the passenger's compartment is full of water, does this mean that x*(density of water = 998)*g + 1800*g = bouyant force of the car? So since water can't get into the wheels, does this mean that there is an upward force from .75+.8 volumes of air *density of air * mg? And they must be equal?

Thanks.
 
  • #8
bodensee9 said:
Hello:

Okay ... thanks. So for the problem, does this mean that before the car sinks, the bouyant force will equal to mg? So if x cubic meter of the passenger's compartment is full of water, does this mean that x*(density of water = 998)*g + 1800*g = bouyant force of the car?

This will work out fine if you are consistent with the buoyant force on the passenger compartment.

So since water can't get into the wheels, does this mean that there is an upward force from .75+.8 volumes of air *density of air * mg? And they must be equal?

Thanks.

This formula for the buoyant force is not right. The buoyant force on a submerged tire would be the same no matter what's inside it. The buoyant force on a tire filled with lead would be the same as the buoyant force on a tire filled with air (if the volumes were the same). So here, the mass of the air in the tires in included in the 1800 kg mass of the car, and the weight of the air is helping to pull the car down.

So you should not have (density of air) in the water's buoyant force expression. (Also, those volumes are more than just the tires--it's the entire car except for the passenger compartment.)


Also, the total buoyant force on the car arises from the total volume of water displaced by the car. You have the volume of the front of the car (.75 m^3), and you have the volume of the back of the car (0.8 m^3). What about the passenger compartment?
 
  • #9
Oh okay .. thanks!
 

Related to Archimedes Principle and bouyant force

What is Archimedes Principle and buoyant force?

Archimedes Principle and buoyant force are concepts in physics that explain how objects float in fluids. Archimedes Principle states that the buoyant force acting on an object submerged in a fluid is equal to the weight of the fluid displaced by the object. Buoyant force is the upward force exerted on an object by a fluid that opposes the weight of the object.

How does Archimedes Principle and buoyant force apply to real life?

Archimedes Principle and buoyant force are applicable to various real-life scenarios, such as why ships and boats float in water, why helium balloons rise in air, and why some objects sink while others float in water. They also play a crucial role in the design and construction of ships, submarines, and other floating structures.

What factors affect the buoyant force on an object?

The buoyant force on an object is affected by the density of the fluid, the volume of the object, and the gravitational force acting on the object. The higher the density of the fluid, the greater the buoyant force. The larger the volume of the object, the greater the buoyant force. And the stronger the gravitational force, the greater the buoyant force.

How is buoyant force related to an object's weight?

According to Archimedes Principle, the buoyant force is equal to the weight of the fluid displaced by the object. This means that for an object to float in a fluid, the buoyant force must be equal to or greater than the weight of the object. If the buoyant force is less than the weight of the object, the object will sink.

Can the buoyant force be negative?

No, the buoyant force can never be negative. It always acts in the upward direction and is equal to the weight of the fluid displaced by the object. If the weight of the fluid displaced is greater than the weight of the object, the buoyant force will be greater than the weight of the object and the object will float. If the weight of the fluid displaced is less than the weight of the object, the object will sink.

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