Find the velocity of the shadow variation

AI Thread Summary
The discussion revolves around calculating the velocity of a shadow cast by a person moving away from a spotlight. The initial calculations yielded a shadow velocity of -0.366 m/s, which differed from the book's solution of -1.22 m/s. Participants suggested using differentiation to simplify the problem and derive the correct relationship between the variables involved. The final approach involved combining equations to express the shadow height as a function of time and applying calculus to find the shadow's velocity. Ultimately, the correct solution was confirmed to align with the textbook answer.
adriaat
Messages
9
Reaction score
0
Helo,
I've been working out this exercise, but my solution and the text's aren't the same.

Homework Statement
We have a spotlight on the floor located at a distance of 30.5 m from a wall of a building. There is a person 1.83 m tall between the spotlight and the wall moving away from the spotlight at a constant velocity of 1.83 m/s. Calculate the velocity of the shadow variation when the person is at 9.14 m from the spotlight.

So, let's name
x_{1}=9.14 m
x_{2}=30.5 m
y_{1}=the height of the shadow when the person is on x_{1}
y_{2}=the height of the shadow when the person is on x_{2}
h=1.83 m (height of the person)
v=1.83 m/s (velocity)

The attempt to a solution

1) I find the height of the shadow projected on the wall when the body is on x1. To do this, I consider the spotlight and the person make a right triangle, with angle \alpha which is the same of the triangle made with the height of the shadow y1 and the distance between the spotlight and the wall.

\alpha=arctan(\frac{h}{x_{1}})

And now I find y_{1}

y_{1}=tan \alpha·x_{2}=6.11 m

Then the height of the shadow at x_{2} will be y_{2}=1.83 m. I think this is obvious.

Afterwards, I want to find the time that took place moving from x_{1} to x_{2} because this will be the same time from y_{1} to y_{2}

\Delta t=\frac{\Delta x}{v}=11.67 s

Then, to conclude

v_{shadow}=\frac{\Delta y}{\Delta t}=-0.366 m/s

The solution of the book is
v_{shadow}=-1.22 m/s

Anyone can help me, please?
 
Last edited:
Physics news on Phys.org
Where does the x_1 = 9.14 \ \mathrm{m} come from? I see it written down in your variable name definitions, but it's not in the original problem statement.

Is this a calculus based class? The easiest way (at least for me) to approach this problem involves differentiation. Maybe we can solve this problem by other means, but if you are allowed to use differential calculus, I would advise using it.

---------------------

You can combine your

\alpha = \arctan \frac{h}{x_1}

and

y_1 = x_2 \tan \alpha

into one simple equation that doesn't involve any trigonometric functions. That will make the coming math quite a bit easier.

After that, don't plug any numbers in just yet. Now is the time for differentiation. :wink:
 
  • Like
Likes 1 person
Thank you, I didn't write that [...]calculate the velocity of the shadow variation when the person is at 9.14 m from the spotlight.

Yes, it is a calculus based class, but I just started calculus classes, so I'm not familiar with differentiation.
---------------------
To combine the equations I do:
\arctan \frac{y_1}{x_2} = \alpha
\alpha = \arctan \frac{h}{x_1}

Then
\frac{y_2}{x_2} = \frac{h}{x_1}

I get stuck here. Do not know sure how to differentiate this equation or if it's possible.
 
adriaat said:
Thank you, I didn't write that [...]calculate the velocity of the shadow variation when the person is at 9.14 m from the spotlight.
That makes sense.

Yes, it is a calculus based class, but I just started calculus classes, so I'm not familiar with differentiation.
I can't think of any other way to solve the problem at the moment. I'm afraid you're going to have to take a derivative, one way or the other.

To combine the equations I do:
\arctan \frac{y_1}{x_2} = \alpha
\alpha = \arctan \frac{h}{x_1}

Then
\frac{y_2}{x_2} = \frac{h}{x_1}

I get stuck here. Do not know sure how to differentiate this equation or if it's possible.

So far so good. :approve:

But allow me to rearrange some variables:

y_2 = \frac{x_2 h}{x_1}
Note that x_2 and h are constants. They don't change with time. On the other hand, x_1 is not constant. x_1 is a function of time. Also, y_2 is a function of x_1 making y_2 also a function of time.

Ultimately what you are looking for is \frac{dy_2}{dt}, the velocity of the shadow.

You have a choice of different approaches at this point.

You could take the derivative of the equation with respect to time, paying special attention to the fact that x_1 is itself a function of time.

Or you could take an intermediate step and find \frac{dy_2}{dx_1}, and then find a relationship between \frac{dy_2}{dx_1} and \frac{dy_2}{dt} as a second step.

[Edit: minor rewording.]
 
Last edited:
  • Like
Likes 1 person
I found a solution which agrees with my text's.

Here is what I did:

1st equation: \frac{dy_2}{dt}=x_2·h·\frac{1}{x_1}=x_2·h·\frac{1}{v·t}

I derivated the above equation, which is the velocity of the shadow's variation, and found time for x_1

2nd equation: t=\frac{x_1}{v}

I combined the 2nd equation into the first one derivated, calculated and as a result I got -1.22 \text m\text / \text s

I think it's OK,

Thank you a lot for your dedication (:
 
Last edited:
adriaat said:
I found a solution which agrees with my text's.
Your approach isn't the approach I would have taken, but it's still valid. However, there are some things that don't seem quite right, as I'll describe below.

Here is what I did:

1st equation: \frac{dy_2}{dt}=x_2·h·\frac{1}{x_1}=x_2·h·\frac{1}{v·t}
Although it's not necessary, it is okay to make the vt = x_1 substitution, since the person is moving at a constant velocity. It also assumes that x_1 = 0 at time t = 0, which is fine for the purposes of this problem.

The problem I see is that the right hand side of your above equation is before the derivative is taken, not after.

y_2 = x_2 h \left( \frac{1}{vt} \right) = \frac{x_2 h}{v} \left(\frac{1}{t} \right)

But that's the relationship before the derivative, not after. Now take the derivative,

\frac{dy_2}{dt} = \frac{d}{dt} \left\{\frac{x_2 h}{v} \left(\frac{1}{t} \right) \right\} = \frac{x_2 h}{v} \frac{d}{dt} \left\{ \frac{1}{t} \right\}

I derivated the above equation, which is the velocity of the shadow's variation, and found time for x_1

2nd equation: t=\frac{x_1}{v}

I combined the 2nd equation into the first one derivated, calculated and as a result I got -1.22 \text m\text / \text s

I think it's OK,

Thank you a lot for your dedication (:
I'm glad you got the answer you were looking for, but I'm just hoping that you didn't stumble upon the right answer for the wrong reasons, by sheer coincidence.

Personally, I solved the problem by differentiating with respect to x_1, obtaining an expression for \frac{dy_2}{dx_1}. Then realizing \frac{dy_2}{dx_1} = \frac{dy_2}{dt} \frac{dt}{dx_1}, also realizing that v = \frac{dx_1}{dt}, substituting, and finally solving for \frac{dy_2}{dt}.
 
Last edited:
  • Like
Likes 1 person
TL;DR Summary: I came across this question from a Sri Lankan A-level textbook. Question - An ice cube with a length of 10 cm is immersed in water at 0 °C. An observer observes the ice cube from the water, and it seems to be 7.75 cm long. If the refractive index of water is 4/3, find the height of the ice cube immersed in the water. I could not understand how the apparent height of the ice cube in the water depends on the height of the ice cube immersed in the water. Does anyone have an...
Thread 'Variable mass system : water sprayed into a moving container'
Starting with the mass considerations #m(t)# is mass of water #M_{c}# mass of container and #M(t)# mass of total system $$M(t) = M_{C} + m(t)$$ $$\Rightarrow \frac{dM(t)}{dt} = \frac{dm(t)}{dt}$$ $$P_i = Mv + u \, dm$$ $$P_f = (M + dm)(v + dv)$$ $$\Delta P = M \, dv + (v - u) \, dm$$ $$F = \frac{dP}{dt} = M \frac{dv}{dt} + (v - u) \frac{dm}{dt}$$ $$F = u \frac{dm}{dt} = \rho A u^2$$ from conservation of momentum , the cannon recoils with the same force which it applies. $$\quad \frac{dm}{dt}...
Back
Top