Instantaneous Power problem

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  • #1
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Hey, instantaneous power is computed by F dot v, but this equation should only be valid if F is constant correct?
 

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  • #2
berkeman
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Hey, instantaneous power is computed by F dot v, but this equation should only be valid if F is constant correct?
Nope. Why do you say that? F and v can be vector functions of time and space and whatever else.
 
  • #3
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It can still be valid because you use instantaneous velocity and instantaneous force, not constant velocity or constant force. It gives the power output for one instant in time regardless of the operations of the system over time.
 
  • #4
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I'm talking about in the case for which v is a varying vector.

P = dW/dt = (dF/dt) dot s + F dot v

The above only simplifies to P = F dot v in the case that dF/dt = 0, or in other words, if F is constant.
 
  • #5
rcgldr
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The above only simplifies to P = F dot v in the case that dF/dt = 0, or in other words, if F is constant.
The equation should end up as: P(t) = F(t) dot V(t). Note that work is defined as the line intergral of F(s) dot ds.
 
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  • #6
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Can you show the derivation? Where is the fallacy in my mathematics? I simply used work as a function time while you used work as a function of the arc length.
 
  • #7
rock.freak667
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Well here is what I think it is.

W=F.s
When you dot product two vectors you get a scalar.

W=F.s=|F||s|

[tex]P=\frac{W}{t}=\frac{|F||s|}{t}=|F||v|=F.v[/tex]
 
  • #8
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but you assumed F was constant in that...
 
  • #9
Stingray
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The work to move something from point x to point y is given by the line integral
[tex]
W(x \rightarrow y) = \int_x^y F(z) \cdot \mathrm{d} z ,
[/tex]
where I'm leaving off vector notation. If the path is described parametrically by a function y(t) with y(0) = x, this can be rewritten as
[tex]
W(x \rightarrow y) = \int_0^t F(y(s)) \cdot \frac{\mathrm{d} y(s)}{\mathrm{d} s} \mathrm{d} s .
[/tex]

The path parameter here can be anything, but choose it to be time. Differentiating with respect to t only hits the upper limit of integration. The result is that
[tex]
P = \mathrm{d}W/\mathrm{d}t = F(y(t)) \cdot \frac{\mathrm{d} y(t)}{\mathrm{d} t} = F \cdot v .
[/tex]
The point here is that the definition of work does not explicitly depend on time. The work required to apply a given force along a given path is identical whether that path is traversed in a second or a year. This sets the definitions as I've given them, and does not allow any t-dependence inside the integrand.
 
  • #10
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during time interval dt, force F can be regarded as a constant, the work done in dt is dW = F dot ds, power is P = dW/dt = F dot ds/dt = F dot v. so even though force is not constant, P = F dot v is still valid.
 
  • #11
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Ah okay, I see. The function I differentiated didn't make much sense since work isn't F(t) dot s(t), but rather int F(s) dot ds, which can be integrated by switching the parameter to t.
 

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