Acceleration in Circular motionPhysical Variables of Circular MotionTangential acceleration in circular...
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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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$begingroup$
Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?
newtonian-mechanics forces acceleration rotation
$endgroup$
add a comment |
$begingroup$
Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?
newtonian-mechanics forces acceleration rotation
$endgroup$
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
add a comment |
$begingroup$
Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?
newtonian-mechanics forces acceleration rotation
$endgroup$
Can motion of a particle be circular if radial acceleration is zero but tangential acceleration is not 0?
newtonian-mechanics forces acceleration rotation
newtonian-mechanics forces acceleration rotation
edited 11 hours ago
Aaron Stevens
16.9k4 gold badges28 silver badges64 bronze badges
16.9k4 gold badges28 silver badges64 bronze badges
asked 12 hours ago
RiyaRiya
161 bronze badge
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
add a comment |
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
add a comment |
5 Answers
5
active
oldest
votes
$begingroup$
No. Radial acceleration is necessary in order to change the direction of the velocity.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
$begingroup$
In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.
$endgroup$
add a comment |
$begingroup$
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?
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
$begingroup$
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
add a comment |
Your Answer
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5 Answers
5
active
oldest
votes
5 Answers
5
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
No. Radial acceleration is necessary in order to change the direction of the velocity.
$endgroup$
add a comment |
$begingroup$
No. Radial acceleration is necessary in order to change the direction of the velocity.
$endgroup$
add a comment |
$begingroup$
No. Radial acceleration is necessary in order to change the direction of the velocity.
$endgroup$
No. Radial acceleration is necessary in order to change the direction of the velocity.
answered 12 hours ago
garypgaryp
17.3k1 gold badge31 silver badges65 bronze badges
17.3k1 gold badge31 silver badges65 bronze badges
add a comment |
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
add a comment |
$begingroup$
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.
$endgroup$
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.
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
add a comment |
add a comment |
$begingroup$
In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.
$endgroup$
add a comment |
$begingroup$
In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.
$endgroup$
add a comment |
$begingroup$
In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.
$endgroup$
In circular motion, $$vec{a}_{text{radial}}neq0,$$ but $vec{a}_{text{tangential}}$ may or may not be equal to zero.
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
add a comment |
add a comment |
$begingroup$
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?
$endgroup$
add a comment |
$begingroup$
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?
$endgroup$
add a comment |
$begingroup$
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?
$endgroup$
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?
answered 1 hour ago
Thomas BlankenhornThomas Blankenhorn
1,0962 gold badges2 silver badges7 bronze badges
1,0962 gold badges2 silver badges7 bronze badges
add a comment |
add a comment |
$begingroup$
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.
$endgroup$
$begingroup$
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
add a comment |
$begingroup$
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.
$endgroup$
$begingroup$
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
add a comment |
$begingroup$
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.
$endgroup$
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.
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
add a comment |
$begingroup$
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
add a comment |
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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