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Acceleration in Circular motion


Physical Variables of Circular MotionTangential acceleration in circular motion?Is this a correct understanding of circular motion?Instantaneous acceleration in non uniform circular motionUniform circular motion dilemmatangential acceleration for uniform circular motionNon Uniform Circular Motion and How External Force Affects The MotionNet acceleration in circular motionCan non-uniform circular motion be called as periodic motion?Intuition for formula of tangential component of acceleration in general curvillinear motion






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2












$begingroup$


Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?










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  • 2




    $begingroup$
    What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
    $endgroup$
    – Bill N
    12 hours ago


















2












$begingroup$


Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?










share|cite|improve this question











$endgroup$








  • 2




    $begingroup$
    What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
    $endgroup$
    – Bill N
    12 hours ago














2












2








2


1



$begingroup$


Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?










share|cite|improve this question











$endgroup$




Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?







newtonian-mechanics forces acceleration rotation






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share|cite|improve this question













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share|cite|improve this question








edited 11 hours ago









Aaron Stevens

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16.9k4 gold badges28 silver badges64 bronze badges










asked 12 hours ago









RiyaRiya

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161 bronze badge








  • 2




    $begingroup$
    What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
    $endgroup$
    – Bill N
    12 hours ago














  • 2




    $begingroup$
    What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
    $endgroup$
    – Bill N
    12 hours ago








2




2




$begingroup$
What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
$endgroup$
– Bill N
12 hours ago




$begingroup$
What discussion, reading, or thoughts have prompted you to ask that question? Do you understand the meaning of the terms "radial" and "tangential"?
$endgroup$
– Bill N
12 hours ago










5 Answers
5






active

oldest

votes


















5












$begingroup$

No. Radial acceleration is necessary in order to change the direction of the velocity.






share|cite|improve this answer









$endgroup$





















    5












    $begingroup$

    Let's look at the general acceleration vector in polar coordinates$^*$:



    $$mathbf a=left(ddot r-rdottheta^2right)hat r+left(rddottheta+2dot rdotthetaright)hattheta$$



    If we want our object to remain on the same circle, we must have $dot r=0$ and $ddot r=0$. This means our acceleration must have the form:
    $$mathbf a=-rdottheta^2hat r+rddotthetahattheta$$



    Since, by Newton's laws, the acceleration vector is proportional to the force via the mass $m$ of our particle, we see that we need a radial force of
    $$F_r=-mrdottheta^2$$
    and a tangential force of
    $$F_theta=mrddottheta$$



    The radial force is responsible for changing the direction of the particle. The tangential force is responsible for changing the speed of the particle as it moves around the circle.



    If we additionally require uniform circular motion, then $ddottheta=0$, and we can only have a radial force without a tangential force. i.e.
    $$mathbf F=-mrdottheta^2hat r$$



    Therefore, the answer to your question is no. You always need a radial force (technically this specific radial force. Not any radial force will do) for circular motion (uniform or not). However, you can have the tangential force as zero (uniform circular motion) or non zero (non-uniform circular motion).





    $^*$ dots represent a rate of change with respect to time if you are not familiar with calculus. for example, $dot r$ is the rate of change of the variable $r$ with respect to time. The derivation of this equation can be found here.






    share|cite|improve this answer











    $endgroup$





















      2












      $begingroup$

      In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.






      share|cite|improve this answer











      $endgroup$





















        0












        $begingroup$

        I think the premise of your question is false, because the accelerated tangential motion will lead to a change in the centrifugal force on the particle, which in turn will cause radial acceleration. You can't have one kind of acceleration without causing the other in the first place.



        But of course, when the acceleration and the resulting adjustment of the radius are finished, you can end up with a new circular orbit at a the new radius. Perhaps this is what you meant?






        share|cite|improve this answer









        $endgroup$





















          -2












          $begingroup$

          For circular motion, we should have
          $$v_r=0,qquad v_{phi}=const.$$
          This means that both the radial as well as tangential acceleration should be zero. If the tangential acceleration is non-zero, this means that the tangential velocity changes which would make the orbit spiral depending on the sign of the acceleration.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
            $endgroup$
            – Aaron Stevens
            12 hours ago














          Your Answer








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          5 Answers
          5






          active

          oldest

          votes








          5 Answers
          5






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          5












          $begingroup$

          No. Radial acceleration is necessary in order to change the direction of the velocity.






          share|cite|improve this answer









          $endgroup$


















            5












            $begingroup$

            No. Radial acceleration is necessary in order to change the direction of the velocity.






            share|cite|improve this answer









            $endgroup$
















              5












              5








              5





              $begingroup$

              No. Radial acceleration is necessary in order to change the direction of the velocity.






              share|cite|improve this answer









              $endgroup$



              No. Radial acceleration is necessary in order to change the direction of the velocity.







              share|cite|improve this answer












              share|cite|improve this answer



              share|cite|improve this answer










              answered 12 hours ago









              garypgaryp

              17.3k1 gold badge31 silver badges65 bronze badges




              17.3k1 gold badge31 silver badges65 bronze badges

























                  5












                  $begingroup$

                  Let's look at the general acceleration vector in polar coordinates$^*$:



                  $$mathbf a=left(ddot r-rdottheta^2right)hat r+left(rddottheta+2dot rdotthetaright)hattheta$$



                  If we want our object to remain on the same circle, we must have $dot r=0$ and $ddot r=0$. This means our acceleration must have the form:
                  $$mathbf a=-rdottheta^2hat r+rddotthetahattheta$$



                  Since, by Newton's laws, the acceleration vector is proportional to the force via the mass $m$ of our particle, we see that we need a radial force of
                  $$F_r=-mrdottheta^2$$
                  and a tangential force of
                  $$F_theta=mrddottheta$$



                  The radial force is responsible for changing the direction of the particle. The tangential force is responsible for changing the speed of the particle as it moves around the circle.



                  If we additionally require uniform circular motion, then $ddottheta=0$, and we can only have a radial force without a tangential force. i.e.
                  $$mathbf F=-mrdottheta^2hat r$$



                  Therefore, the answer to your question is no. You always need a radial force (technically this specific radial force. Not any radial force will do) for circular motion (uniform or not). However, you can have the tangential force as zero (uniform circular motion) or non zero (non-uniform circular motion).





                  $^*$ dots represent a rate of change with respect to time if you are not familiar with calculus. for example, $dot r$ is the rate of change of the variable $r$ with respect to time. The derivation of this equation can be found here.






                  share|cite|improve this answer











                  $endgroup$


















                    5












                    $begingroup$

                    Let's look at the general acceleration vector in polar coordinates$^*$:



                    $$mathbf a=left(ddot r-rdottheta^2right)hat r+left(rddottheta+2dot rdotthetaright)hattheta$$



                    If we want our object to remain on the same circle, we must have $dot r=0$ and $ddot r=0$. This means our acceleration must have the form:
                    $$mathbf a=-rdottheta^2hat r+rddotthetahattheta$$



                    Since, by Newton's laws, the acceleration vector is proportional to the force via the mass $m$ of our particle, we see that we need a radial force of
                    $$F_r=-mrdottheta^2$$
                    and a tangential force of
                    $$F_theta=mrddottheta$$



                    The radial force is responsible for changing the direction of the particle. The tangential force is responsible for changing the speed of the particle as it moves around the circle.



                    If we additionally require uniform circular motion, then $ddottheta=0$, and we can only have a radial force without a tangential force. i.e.
                    $$mathbf F=-mrdottheta^2hat r$$



                    Therefore, the answer to your question is no. You always need a radial force (technically this specific radial force. Not any radial force will do) for circular motion (uniform or not). However, you can have the tangential force as zero (uniform circular motion) or non zero (non-uniform circular motion).





                    $^*$ dots represent a rate of change with respect to time if you are not familiar with calculus. for example, $dot r$ is the rate of change of the variable $r$ with respect to time. The derivation of this equation can be found here.






                    share|cite|improve this answer











                    $endgroup$
















                      5












                      5








                      5





                      $begingroup$

                      Let's look at the general acceleration vector in polar coordinates$^*$:



                      $$mathbf a=left(ddot r-rdottheta^2right)hat r+left(rddottheta+2dot rdotthetaright)hattheta$$



                      If we want our object to remain on the same circle, we must have $dot r=0$ and $ddot r=0$. This means our acceleration must have the form:
                      $$mathbf a=-rdottheta^2hat r+rddotthetahattheta$$



                      Since, by Newton's laws, the acceleration vector is proportional to the force via the mass $m$ of our particle, we see that we need a radial force of
                      $$F_r=-mrdottheta^2$$
                      and a tangential force of
                      $$F_theta=mrddottheta$$



                      The radial force is responsible for changing the direction of the particle. The tangential force is responsible for changing the speed of the particle as it moves around the circle.



                      If we additionally require uniform circular motion, then $ddottheta=0$, and we can only have a radial force without a tangential force. i.e.
                      $$mathbf F=-mrdottheta^2hat r$$



                      Therefore, the answer to your question is no. You always need a radial force (technically this specific radial force. Not any radial force will do) for circular motion (uniform or not). However, you can have the tangential force as zero (uniform circular motion) or non zero (non-uniform circular motion).





                      $^*$ dots represent a rate of change with respect to time if you are not familiar with calculus. for example, $dot r$ is the rate of change of the variable $r$ with respect to time. The derivation of this equation can be found here.






                      share|cite|improve this answer











                      $endgroup$



                      Let's look at the general acceleration vector in polar coordinates$^*$:



                      $$mathbf a=left(ddot r-rdottheta^2right)hat r+left(rddottheta+2dot rdotthetaright)hattheta$$



                      If we want our object to remain on the same circle, we must have $dot r=0$ and $ddot r=0$. This means our acceleration must have the form:
                      $$mathbf a=-rdottheta^2hat r+rddotthetahattheta$$



                      Since, by Newton's laws, the acceleration vector is proportional to the force via the mass $m$ of our particle, we see that we need a radial force of
                      $$F_r=-mrdottheta^2$$
                      and a tangential force of
                      $$F_theta=mrddottheta$$



                      The radial force is responsible for changing the direction of the particle. The tangential force is responsible for changing the speed of the particle as it moves around the circle.



                      If we additionally require uniform circular motion, then $ddottheta=0$, and we can only have a radial force without a tangential force. i.e.
                      $$mathbf F=-mrdottheta^2hat r$$



                      Therefore, the answer to your question is no. You always need a radial force (technically this specific radial force. Not any radial force will do) for circular motion (uniform or not). However, you can have the tangential force as zero (uniform circular motion) or non zero (non-uniform circular motion).





                      $^*$ dots represent a rate of change with respect to time if you are not familiar with calculus. for example, $dot r$ is the rate of change of the variable $r$ with respect to time. The derivation of this equation can be found here.







                      share|cite|improve this answer














                      share|cite|improve this answer



                      share|cite|improve this answer








                      edited 11 hours ago

























                      answered 11 hours ago









                      Aaron StevensAaron Stevens

                      16.9k4 gold badges28 silver badges64 bronze badges




                      16.9k4 gold badges28 silver badges64 bronze badges























                          2












                          $begingroup$

                          In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.






                          share|cite|improve this answer











                          $endgroup$


















                            2












                            $begingroup$

                            In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.






                            share|cite|improve this answer











                            $endgroup$
















                              2












                              2








                              2





                              $begingroup$

                              In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.






                              share|cite|improve this answer











                              $endgroup$



                              In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.







                              share|cite|improve this answer














                              share|cite|improve this answer



                              share|cite|improve this answer








                              edited 3 hours ago









                              Sebastiano

                              3792 silver badges20 bronze badges




                              3792 silver badges20 bronze badges










                              answered 10 hours ago









                              UniqueUnique

                              1,0651 gold badge5 silver badges18 bronze badges




                              1,0651 gold badge5 silver badges18 bronze badges























                                  0












                                  $begingroup$

                                  I think the premise of your question is false, because the accelerated tangential motion will lead to a change in the centrifugal force on the particle, which in turn will cause radial acceleration. You can't have one kind of acceleration without causing the other in the first place.



                                  But of course, when the acceleration and the resulting adjustment of the radius are finished, you can end up with a new circular orbit at a the new radius. Perhaps this is what you meant?






                                  share|cite|improve this answer









                                  $endgroup$


















                                    0












                                    $begingroup$

                                    I think the premise of your question is false, because the accelerated tangential motion will lead to a change in the centrifugal force on the particle, which in turn will cause radial acceleration. You can't have one kind of acceleration without causing the other in the first place.



                                    But of course, when the acceleration and the resulting adjustment of the radius are finished, you can end up with a new circular orbit at a the new radius. Perhaps this is what you meant?






                                    share|cite|improve this answer









                                    $endgroup$
















                                      0












                                      0








                                      0





                                      $begingroup$

                                      I think the premise of your question is false, because the accelerated tangential motion will lead to a change in the centrifugal force on the particle, which in turn will cause radial acceleration. You can't have one kind of acceleration without causing the other in the first place.



                                      But of course, when the acceleration and the resulting adjustment of the radius are finished, you can end up with a new circular orbit at a the new radius. Perhaps this is what you meant?






                                      share|cite|improve this answer









                                      $endgroup$



                                      I think the premise of your question is false, because the accelerated tangential motion will lead to a change in the centrifugal force on the particle, which in turn will cause radial acceleration. You can't have one kind of acceleration without causing the other in the first place.



                                      But of course, when the acceleration and the resulting adjustment of the radius are finished, you can end up with a new circular orbit at a the new radius. Perhaps this is what you meant?







                                      share|cite|improve this answer












                                      share|cite|improve this answer



                                      share|cite|improve this answer










                                      answered 1 hour ago









                                      Thomas BlankenhornThomas Blankenhorn

                                      1,0962 gold badges2 silver badges7 bronze badges




                                      1,0962 gold badges2 silver badges7 bronze badges























                                          -2












                                          $begingroup$

                                          For circular motion, we should have
                                          $$v_r=0,qquad v_{phi}=const.$$
                                          This means that both the radial as well as tangential acceleration should be zero. If the tangential acceleration is non-zero, this means that the tangential velocity changes which would make the orbit spiral depending on the sign of the acceleration.






                                          share|cite|improve this answer









                                          $endgroup$













                                          • $begingroup$
                                            This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                            $endgroup$
                                            – Aaron Stevens
                                            12 hours ago
















                                          -2












                                          $begingroup$

                                          For circular motion, we should have
                                          $$v_r=0,qquad v_{phi}=const.$$
                                          This means that both the radial as well as tangential acceleration should be zero. If the tangential acceleration is non-zero, this means that the tangential velocity changes which would make the orbit spiral depending on the sign of the acceleration.






                                          share|cite|improve this answer









                                          $endgroup$













                                          • $begingroup$
                                            This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                            $endgroup$
                                            – Aaron Stevens
                                            12 hours ago














                                          -2












                                          -2








                                          -2





                                          $begingroup$

                                          For circular motion, we should have
                                          $$v_r=0,qquad v_{phi}=const.$$
                                          This means that both the radial as well as tangential acceleration should be zero. If the tangential acceleration is non-zero, this means that the tangential velocity changes which would make the orbit spiral depending on the sign of the acceleration.






                                          share|cite|improve this answer









                                          $endgroup$



                                          For circular motion, we should have
                                          $$v_r=0,qquad v_{phi}=const.$$
                                          This means that both the radial as well as tangential acceleration should be zero. If the tangential acceleration is non-zero, this means that the tangential velocity changes which would make the orbit spiral depending on the sign of the acceleration.







                                          share|cite|improve this answer












                                          share|cite|improve this answer



                                          share|cite|improve this answer










                                          answered 12 hours ago









                                          RichardRichard

                                          1649 bronze badges




                                          1649 bronze badges












                                          • $begingroup$
                                            This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                            $endgroup$
                                            – Aaron Stevens
                                            12 hours ago


















                                          • $begingroup$
                                            This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                            $endgroup$
                                            – Aaron Stevens
                                            12 hours ago
















                                          $begingroup$
                                          This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                          $endgroup$
                                          – Aaron Stevens
                                          12 hours ago




                                          $begingroup$
                                          This is for uniform circular motion. Non-uniform circular motion is also possible. Your speed can change while still remaining on the same circle.
                                          $endgroup$
                                          – Aaron Stevens
                                          12 hours ago


















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