Nonuniform circular motion refers to the motion of an object in a circular path at varying speeds. In this case, the student is swinging a rock in a horizontal circle, which means the motion is in the x-y plane.
To solve this problem, we need to use the equation for centripetal acceleration, which is given by:
a = v^2/r
Where v is the tangential velocity and r is the radius of the circle. In this case, the radius is equal to the length of the string, which is 1.0 m.
Next, we need to consider the forces acting on the rock. The only force acting on the rock is the tension in the string, which provides the centripetal force to keep the rock in circular motion. This force can be broken down into its x and y components, with the x component being responsible for the tilting of the string.
We can use the equation for the x component of the tension force, given by:
Tx = T*sin(θ)
Where θ is the angle of the string with respect to the horizontal. In this case, we know that the angle is 10 degrees, so we can substitute that into the equation.
Now, we can set the x component of the tension force equal to the centripetal force, and solve for the tangential velocity:
T*sin(10) = m*v^2/r
Where m is the mass of the rock, which is given as 500g or 0.5 kg.
Solving for v, we get:
v = sqrt(T*sin(10)*r/m)
Substituting in the known values, we get:
v = sqrt(T*0.1745/0.5)
Next, we need to find the tension force, which we can do by setting the y component of the tension force equal to the weight of the rock:
Ty = T*cos(θ) = mg
Where g is the acceleration due to gravity, equal to 9.8 m/s^2.
Solving for T, we get:
T = mg/cos(θ)
Substituting in the known values, we get:
T = 0.5*9.8/cos(10) = 4.97 N
Finally, we can substitute this value for T into our equation for the tangential velocity:
v = sqrt(4.97*0.1745/0.5) = 1