Answer:
 250Nm
Explanation:
Given parameters: 
Length of the long pry bar  = 1m 
Force acting on it  = 250N 
Angle  = 90° 
Unknown: 
Amount of torque applied  = ? 
Solution: 
Torque is the turning force on a body that causes the rotation of the body. 
The formula is given as: 
  Torque  = Force x r Sin Ф  
r is the distance 
  So; 
    Torque  = 250 x 1 x sin 90  = 250Nm
 
        
             
        
        
        
The kinetic energy with which the hammer strikes the ground 
is exactly the potential energy it had at the height from which it fell.  
Potential energy is (mass) x (gravity) x (height) .... directly proportional 
to height.
Starting from double the height, it starts with double the potential 
energy, and it reaches the bottom with double the kinetic energy.
        
                    
             
        
        
        
Answer:
 w = √[g /L (½ r²/L2 + 2/3 ) ]
When the mass of the cylinder changes if its external dimensions do not change the angular velocity DOES NOT CHANGE
Explanation:
We can simulate this system as a physical pendulum, which is a pendulum with a distributed mass, in this case the angular velocity is
           w² = mg d / I
In this case, the distance d to the pivot point of half the length (L) of the cylinder, which we consider long and narrow
          d = L / 2
The moment of inertia of a cylinder with respect to an axis at the end we can use the parallel axes theorem, it is approximately equal to that of a long bar plus the moment of inertia of the center of mass of the cylinder, this is tabulated
         I = ¼ m r2 + ⅓ m L2
         I = m (¼ r2 + ⅓ L2)
now let's use the concept of density to calculate the mass of the system
         ρ = m / V
         m = ρ V
the volume of a cylinder is
          V = π r² L
           m =  ρ π r² L
let's substitute
         w² = m g (L / 2) / m (¼ r² + ⅓ L²)
         w² = g L / (½ r² + 2/3 L²)
         L >> r
          w = √[g /L (½ r²/L2 + 2/3 ) ]
When the mass of the cylinder changes if its external dimensions do not change the angular velocity DOES NOT CHANGE
 
        
             
        
        
        
Explanation:
We have,
Semimajor axis is 
It is required to find the orbital period of a dwarf planet. Let T is time period. The relation between the time period and the semi major axis is given by Kepler's third law. Its mathematical form is given by :

G is universal gravitational constant
M is solar mass
Plugging all the values,

Since,
 
So, the orbital period of a dwarf planet is 138.52 years.