8.01 MIT OCW PS1.4: Throw and Catch (Kinematics)

  • #1
giodude
30
1
Homework Statement
A ball is thrown over the head of a person who is standing a horizontal distance d from the point where the ball was thrown. The initial ball's velocity is at an angle theta with respect to the groun and has a magnitude v0. As soon as the ball is thrown, the person runs with a time-varying acceleration whose component along the x-axis is given by Bt, where B is a positive constant. The person catches the ball at exactly the same height it was thrown from. Assume that the air resistance is negligible and that the gravitational acceleration is directed downward and has magnitude g. Find the constant B.
Express your answer in terms of some or all of the given variables. Use theta, g, d, and v0 as needed.
Relevant Equations
xp0 = d, vp0 = 0, ap0 = 0
xp(t) = d + (1/6)*B*(t^3)
vp(t) = B*(t^2)/2
ap(t) = B*t

xb0 = 0, vb0 = v0, ab0 = 0
xb(t) = v0*cos(theta)*t
vb(t) = v0*cos(theta)
ab(t) = 0
1) Using "The person catches the ball at exactly the same height it was thrown from.", we can isolate t by solving yb(t) = v0*sin(theta)*t - (1/2)*g*(t^2) = 0:
yb(t) = v0*sin(theta)*t - (1/2)*g*(t^2) = 0
v0*sin(theta)*t = (1/2)*g*(t^2)
2*v0*sin(theta) = g*t
t = 2*v0*sin(theta) / g

2) At the time of the catch, the person and the ball have the same x coordinate so we can set xp(t) = xb(t) and plug in t
d + (1/6)*B*(t^3) = v0*cos(theta)*t
B*(t^3) = 6*v0*cos(theta)*t - 6*d
B = (6*v0*cos(theta)*t - 6*d) / (t^3)
B = (6*v0*cos(theta)*t - 6*d) / (2*v0*sin(theta) / g)^3

I believe this is the correct answer. My purpose for posting this here is two fold; to see if I've done it correctly and to try and understand how to physically interpret this outcome so that it intuitively makes sense as well. One way I was thinking about physically interpreting it was through dimensional analysis and checking that there are no lingering dimensions. However, am curious about other modes of approach.
 

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  • #2
If you wish somebody to take the time to check your work you need to use LaTex for the equations. Yes there is a learning curve. See "LaTeX Guide below
 
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  • #3
Will do.
 
  • #4
giodude said:
B = (6*v0*cos(theta)*t - 6*d) / (2*v0*sin(theta) / g)^3

I believe this is the correct answer.
It is not, quite, an answer to the question posed because you still have a t in there.
Did you check the dimensions? Looks ok to me.
Often, a useful sanity check is a special case for which the answer is obvious, but I don't see such an option here. One special case would be d=0, but the answer is still not obvious for that. ##d=v_0\cos(\theta)t## works, but is too trivial.
 
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  • #5
haruspex said:
It is not, quite, an answer to the question posed because you still have a t in there.
Did you check the dimensions? Looks ok to me.
Often, a useful sanity check is a special case for which the answer is obvious, but I don't see such an option here. One special case would be d=0, but the answer is still not obvious for that. ##d=v_0\cos(\theta)t## works, but is too trivial.
Oh, yes! It looks like I forgot to convert that value.

Dimensions seem to properly cancel out. Thanks!
 

Related to 8.01 MIT OCW PS1.4: Throw and Catch (Kinematics)

What is the main objective of the "Throw and Catch" problem in 8.01 MIT OCW PS1.4?

The main objective of the "Throw and Catch" problem is to apply principles of kinematics to analyze the motion of an object that is thrown and caught. This involves understanding concepts like initial velocity, acceleration due to gravity, time of flight, and displacement.

How do you determine the time of flight for an object thrown vertically upwards?

The time of flight for an object thrown vertically upwards can be determined by using the kinematic equation for motion under constant acceleration. The total time of flight is twice the time taken to reach the maximum height. This can be calculated using the formula: \( t = \frac{2v_0 \sin(\theta)}{g} \), where \( v_0 \) is the initial velocity, \( \theta \) is the angle of projection (90 degrees for vertical throw), and \( g \) is the acceleration due to gravity.

What equations are used to calculate the maximum height reached by the object?

The maximum height \( h \) reached by the object can be calculated using the kinematic equation: \( h = \frac{v_0^2 \sin^2(\theta)}{2g} \), where \( v_0 \) is the initial velocity, \( \theta \) is the angle of projection, and \( g \) is the acceleration due to gravity. For a vertical throw, \( \theta \) is 90 degrees, simplifying the equation to \( h = \frac{v_0^2}{2g} \).

How do you calculate the initial velocity needed for the object to reach a specific height?

To calculate the initial velocity \( v_0 \) needed for the object to reach a specific height \( h \), you can rearrange the kinematic equation for maximum height: \( v_0 = \sqrt{2gh} \), where \( g \) is the acceleration due to gravity and \( h \) is the desired height.

What role does air resistance play in the "Throw and Catch" problem?

In the context of the "Throw and Catch" problem as typically presented in introductory physics courses like 8.01 MIT OCW, air resistance is often neglected to simplify the calculations. The focus is primarily on idealized motion under the influence of gravity alone. However, in real-world scenarios, air resistance would affect the object's trajectory, reducing its maximum height and altering its time of flight.

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