Potential Gradient relation

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I was just wondering why exactly the force is the negative gradient of the potential, which is shown by the relation $$bf F=−bf∇V$$I know that this equation only holds for conservative forces, where the potential only depends on the position of an object. The only problem I have is why there is a minus sign/ what the minus sign means in a physical context.










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  • See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
    – LonelyProf
    4 hours ago















up vote
2
down vote

favorite












I was just wondering why exactly the force is the negative gradient of the potential, which is shown by the relation $$bf F=−bf∇V$$I know that this equation only holds for conservative forces, where the potential only depends on the position of an object. The only problem I have is why there is a minus sign/ what the minus sign means in a physical context.










share|cite|improve this question























  • See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
    – LonelyProf
    4 hours ago













up vote
2
down vote

favorite









up vote
2
down vote

favorite











I was just wondering why exactly the force is the negative gradient of the potential, which is shown by the relation $$bf F=−bf∇V$$I know that this equation only holds for conservative forces, where the potential only depends on the position of an object. The only problem I have is why there is a minus sign/ what the minus sign means in a physical context.










share|cite|improve this question















I was just wondering why exactly the force is the negative gradient of the potential, which is shown by the relation $$bf F=−bf∇V$$I know that this equation only holds for conservative forces, where the potential only depends on the position of an object. The only problem I have is why there is a minus sign/ what the minus sign means in a physical context.







newtonian-mechanics kinematics potential






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edited 4 hours ago









Garf

1,009117




1,009117










asked 4 hours ago









Tatjana Gobold

325




325











  • See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
    – LonelyProf
    4 hours ago

















  • See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
    – LonelyProf
    4 hours ago
















See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
– LonelyProf
4 hours ago





See: physics.stackexchange.com/questions/16339/… and physics.stackexchange.com/questions/18874/…
– LonelyProf
4 hours ago











3 Answers
3






active

oldest

votes

















up vote
1
down vote



accepted










Well, despite the fact thet the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.



The key idea is that




The minus sign is just a convention.




Forces do exist, and we define the potential based on them, not vice-versa.



By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is



$$ vecF=-vecnablaE_p$$



Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $neq$ joules, you know.



Well, sorry, back to the topic. The thing is that, the only thin we know is:



  • A Conservative force is such that the work done by it does not depend on the path.

  • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated atthe initial point:

$$W_cons=int_vecx_0^vecx_F vecFcdot dvecx=B(vecx_F)-B(vecx_0)$$



That's the only thing we know.



And then, we decide to define a new function, called "potential energy", such that



$$E_p=-B$$



And we do that because



$$W_Total=Delta E_k$$



$$W_total=W_cons+W_not cons$$



So



$$Delta E_k = W_not cons+ Delta B$$



$$Delta E_k - Delta B= W_not cons$$



And that's it. We could just work with that formula. But, we prefer havinga possitive quantity, so we write



$$Delta E_k + Delta E_p= W_not cons$$



And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".



That is the actual reason for the minus sign. But, as I said, it's jsut a convention. We could just work with the opposite funcion, which I called $B$.



Hope I helped.






share|cite|improve this answer




















  • Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
    – Tatjana Gobold
    3 hours ago


















up vote
1
down vote













The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.






share|cite|improve this answer



























    up vote
    1
    down vote













    One of the simplest ways to look at this is in 1 dimension:



    $$F=-fractextdVtextdx$$



    Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like



    enter image description here



    If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.



    If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.



    This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.






    share|cite|improve this answer






















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      3 Answers
      3






      active

      oldest

      votes








      3 Answers
      3






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes








      up vote
      1
      down vote



      accepted










      Well, despite the fact thet the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.



      The key idea is that




      The minus sign is just a convention.




      Forces do exist, and we define the potential based on them, not vice-versa.



      By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is



      $$ vecF=-vecnablaE_p$$



      Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $neq$ joules, you know.



      Well, sorry, back to the topic. The thing is that, the only thin we know is:



      • A Conservative force is such that the work done by it does not depend on the path.

      • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated atthe initial point:

      $$W_cons=int_vecx_0^vecx_F vecFcdot dvecx=B(vecx_F)-B(vecx_0)$$



      That's the only thing we know.



      And then, we decide to define a new function, called "potential energy", such that



      $$E_p=-B$$



      And we do that because



      $$W_Total=Delta E_k$$



      $$W_total=W_cons+W_not cons$$



      So



      $$Delta E_k = W_not cons+ Delta B$$



      $$Delta E_k - Delta B= W_not cons$$



      And that's it. We could just work with that formula. But, we prefer havinga possitive quantity, so we write



      $$Delta E_k + Delta E_p= W_not cons$$



      And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".



      That is the actual reason for the minus sign. But, as I said, it's jsut a convention. We could just work with the opposite funcion, which I called $B$.



      Hope I helped.






      share|cite|improve this answer




















      • Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
        – Tatjana Gobold
        3 hours ago















      up vote
      1
      down vote



      accepted










      Well, despite the fact thet the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.



      The key idea is that




      The minus sign is just a convention.




      Forces do exist, and we define the potential based on them, not vice-versa.



      By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is



      $$ vecF=-vecnablaE_p$$



      Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $neq$ joules, you know.



      Well, sorry, back to the topic. The thing is that, the only thin we know is:



      • A Conservative force is such that the work done by it does not depend on the path.

      • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated atthe initial point:

      $$W_cons=int_vecx_0^vecx_F vecFcdot dvecx=B(vecx_F)-B(vecx_0)$$



      That's the only thing we know.



      And then, we decide to define a new function, called "potential energy", such that



      $$E_p=-B$$



      And we do that because



      $$W_Total=Delta E_k$$



      $$W_total=W_cons+W_not cons$$



      So



      $$Delta E_k = W_not cons+ Delta B$$



      $$Delta E_k - Delta B= W_not cons$$



      And that's it. We could just work with that formula. But, we prefer havinga possitive quantity, so we write



      $$Delta E_k + Delta E_p= W_not cons$$



      And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".



      That is the actual reason for the minus sign. But, as I said, it's jsut a convention. We could just work with the opposite funcion, which I called $B$.



      Hope I helped.






      share|cite|improve this answer




















      • Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
        – Tatjana Gobold
        3 hours ago













      up vote
      1
      down vote



      accepted







      up vote
      1
      down vote



      accepted






      Well, despite the fact thet the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.



      The key idea is that




      The minus sign is just a convention.




      Forces do exist, and we define the potential based on them, not vice-versa.



      By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is



      $$ vecF=-vecnablaE_p$$



      Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $neq$ joules, you know.



      Well, sorry, back to the topic. The thing is that, the only thin we know is:



      • A Conservative force is such that the work done by it does not depend on the path.

      • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated atthe initial point:

      $$W_cons=int_vecx_0^vecx_F vecFcdot dvecx=B(vecx_F)-B(vecx_0)$$



      That's the only thing we know.



      And then, we decide to define a new function, called "potential energy", such that



      $$E_p=-B$$



      And we do that because



      $$W_Total=Delta E_k$$



      $$W_total=W_cons+W_not cons$$



      So



      $$Delta E_k = W_not cons+ Delta B$$



      $$Delta E_k - Delta B= W_not cons$$



      And that's it. We could just work with that formula. But, we prefer havinga possitive quantity, so we write



      $$Delta E_k + Delta E_p= W_not cons$$



      And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".



      That is the actual reason for the minus sign. But, as I said, it's jsut a convention. We could just work with the opposite funcion, which I called $B$.



      Hope I helped.






      share|cite|improve this answer












      Well, despite the fact thet the other answers are interesting, I'd prefer going directly to the "origin" of this thing, rather than its useful physical meaning.



      The key idea is that




      The minus sign is just a convention.




      Forces do exist, and we define the potential based on them, not vice-versa.



      By the way, I am commiting the mistake I hate: we are talking about potentials. But actually, the relation is



      $$ vecF=-vecnablaE_p$$



      Where $E_p$ is the potential energy. You'll say: "that's what I wrote", yes, but we are lazy and we say "potential", but we write potential energy. I curse the person who decided to use $V$ for potential energy, when it was being used for "potential", as in Volts of electric potential. Volts $neq$ joules, you know.



      Well, sorry, back to the topic. The thing is that, the only thin we know is:



      • A Conservative force is such that the work done by it does not depend on the path.

      • But that implies that we can write work as "one function", evaluated at the final point, minus the same function evaluated atthe initial point:

      $$W_cons=int_vecx_0^vecx_F vecFcdot dvecx=B(vecx_F)-B(vecx_0)$$



      That's the only thing we know.



      And then, we decide to define a new function, called "potential energy", such that



      $$E_p=-B$$



      And we do that because



      $$W_Total=Delta E_k$$



      $$W_total=W_cons+W_not cons$$



      So



      $$Delta E_k = W_not cons+ Delta B$$



      $$Delta E_k - Delta B= W_not cons$$



      And that's it. We could just work with that formula. But, we prefer havinga possitive quantity, so we write



      $$Delta E_k + Delta E_p= W_not cons$$



      And so, we can think of potential energy in the same way as kinetic energy, in the sense of, "the more energy, the more work".



      That is the actual reason for the minus sign. But, as I said, it's jsut a convention. We could just work with the opposite funcion, which I called $B$.



      Hope I helped.







      share|cite|improve this answer












      share|cite|improve this answer



      share|cite|improve this answer










      answered 3 hours ago









      FGSUZ

      3,3102521




      3,3102521











      • Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
        – Tatjana Gobold
        3 hours ago

















      • Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
        – Tatjana Gobold
        3 hours ago
















      Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
      – Tatjana Gobold
      3 hours ago





      Great thank you! In a physical context I already got it, so it's nice to have a small deduction of this formula. Actually you would need some vector calculus for F = -dV/dx because it is a gradient, but your answer makes sense, too. And yes I am aware that V stands for potential energy, but it is just convenient to say potential if you know that you actually mean potential energy :D
      – Tatjana Gobold
      3 hours ago











      up vote
      1
      down vote













      The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.






      share|cite|improve this answer
























        up vote
        1
        down vote













        The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.






        share|cite|improve this answer






















          up vote
          1
          down vote










          up vote
          1
          down vote









          The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.






          share|cite|improve this answer












          The gradient is a vector pointing to the direction where the change of $V$ is maximum. If a force $F$ is pointing in the direction of $-nabla V$, it will push you in the direction where $V$ decreases the fastest. Think of a little marble placed on the edge of a bowl - it will roll down, but in which way? It can go down in a helix or just roll down to the center, and it chooses the second - why is that? Because that is the direction of fastest decrease in height (and thus gravitational potential energy). That is the physical meaning of the minus sign. If it was a plus, the ball would roll up the potential.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered 4 hours ago









          Ofek Gillon

          1,139417




          1,139417




















              up vote
              1
              down vote













              One of the simplest ways to look at this is in 1 dimension:



              $$F=-fractextdVtextdx$$



              Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like



              enter image description here



              If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.



              If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.



              This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.






              share|cite|improve this answer


























                up vote
                1
                down vote













                One of the simplest ways to look at this is in 1 dimension:



                $$F=-fractextdVtextdx$$



                Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like



                enter image description here



                If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.



                If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.



                This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.






                share|cite|improve this answer
























                  up vote
                  1
                  down vote










                  up vote
                  1
                  down vote









                  One of the simplest ways to look at this is in 1 dimension:



                  $$F=-fractextdVtextdx$$



                  Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like



                  enter image description here



                  If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.



                  If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.



                  This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.






                  share|cite|improve this answer














                  One of the simplest ways to look at this is in 1 dimension:



                  $$F=-fractextdVtextdx$$



                  Imagine a ball in a hilly landscape. Plotting a graph of gravitational potential energy vs $x$ might look something like



                  enter image description here



                  If the ball is at position $A$, then the gradient of the potential energy with $x$ is negative, and the resulting force will be in the positive $x$-direction.



                  If the ball is at position $B$, then the gradient of potential energy with $x$ is positive, so the force is in the negative $x$ direction.



                  This overall point here is that things like to try and lower their (potential) energy if they can. This means that if in a certain direction the potential energy is going to increase, the ball is going to want to move $away$ from this, and in a direction where the ball is decreasing potential energy, until equilibrium is reached at a stationary point.







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited 4 hours ago

























                  answered 4 hours ago









                  Garf

                  1,009117




                  1,009117



























                       

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