Problem 63
Question
(III) A particle rotates in a circle of radius \(3.80 \mathrm{~m}\). At a particular instant its acceleration is \(1.15 \mathrm{~m} / \mathrm{s}^{2}\) in a direction that makes an angle of \(38.0^{\circ}\) to its direction of motion. Determine its speed \((a)\) at this moment and \((b) 2.00 \mathrm{~s}\) later, assuming constant tangential acceleration.
Step-by-Step Solution
Verified Answer
Speed initially is approximately 1.86 m/s; after 2 seconds, it's 3.28 m/s.
1Step 1: Understand the Given Information
We have a particle moving in a circle of radius \( r = 3.80 \text{ m} \). The particle's acceleration is \( 1.15 \text{ m/s}^2 \), which is at an angle of \( 38.0^{\circ} \) to its direction of motion. We need to find (a) the speed at this instant and (b) the speed 2 seconds later with constant tangential acceleration.
2Step 2: Resolve Acceleration into Components
The given acceleration can be resolved into two components: radial acceleration (\( a_r \)) and tangential acceleration (\( a_t \)). The radial acceleration is given by \( a \cos(38.0^{\circ}) \) and the tangential acceleration by \( a \sin(38.0^{\circ}) \), where \( a = 1.15 \text{ m/s}^2 \).
3Step 3: Calculate Radial Acceleration
Calculate the radial component of the acceleration: \[ a_r = a \cos(38.0^{\circ}) = 1.15 \times \cos(38.0^{\circ}) \approx 0.91 \text{ m/s}^2 \] This radial component is also equal to \( \frac{v^2}{r} \), where \( v \) is the speed we want to find.
4Step 4: Solve for Initial Speed
Set the radial acceleration equal to \( \frac{v^2}{r} \) to solve for the speed:\[ 0.91 = \frac{v^2}{3.80} \]Multiply both sides by 3.80 and solve for \( v \): \[ v^2 = 3.80 \times 0.91 \]\[ v^2 = 3.458 \]\[ v = \sqrt{3.458} \approx 1.86 \text{ m/s} \].
5Step 5: Calculate Tangential Acceleration
Calculate the tangential component of the acceleration: \[ a_t = a \sin(38.0^{\circ}) = 1.15 \times \sin(38.0^{\circ}) \approx 0.71 \text{ m/s}^2 \].This tangential acceleration is constant and will be used to calculate the speed after 2 seconds.
6Step 6: Calculate Speed After 2 Seconds
Using the formula for speed with constant tangential acceleration: \[ v_f = v_i + a_t \times t \]where \( v_i = 1.86 \text{ m/s} \) and \( t = 2 \text{ s} \), \[ v_f = 1.86 + 0.71 \times 2 \]\[ v_f = 1.86 + 1.42 = 3.28 \text{ m/s} \].
Key Concepts
Tangential AccelerationRadial AccelerationSpeed Calculation
Tangential Acceleration
When an object is rotating in a circle, its velocity isn't constant because the direction is constantly changing. However, if there is also a change in speed along the circular path, this is due to tangential acceleration.
The tangential acceleration, often denoted as \(a_t\), affects how fast or slow an object speeds up or slows down while moving along the circular path. This is analogous to the acceleration in linear motion, just along the tangent to the circular path.
The tangential acceleration, often denoted as \(a_t\), affects how fast or slow an object speeds up or slows down while moving along the circular path. This is analogous to the acceleration in linear motion, just along the tangent to the circular path.
- The formula for tangential acceleration when the component of total acceleration and the angle is known is: \\[a_t = a \sin(\theta)\]
- In this exercise, where \(a = 1.15 \, \text{m/s}^2\) and \(\theta = 38.0^\circ\), we find \(a_t\) to be approximately \(0.71 \, \text{m/s}^2\).
- It is constant in this problem, allowing the use of simple kinematic equations to find the change in speed over time.
Radial Acceleration
Another critical component when dealing with circular motion is radial acceleration, which is directed towards the center of the circular path.
This inward acceleration keeps the particle moving in a circle rather than flying off in a straight line. Radial acceleration is also known as centripetal acceleration and is given by the formula \[a_r = \frac{v^2}{r}\]where \(v\) is the speed of the particle and \(r\) is the radius of the circle.
This inward acceleration keeps the particle moving in a circle rather than flying off in a straight line. Radial acceleration is also known as centripetal acceleration and is given by the formula \[a_r = \frac{v^2}{r}\]where \(v\) is the speed of the particle and \(r\) is the radius of the circle.
- It stems from the component of acceleration that points towards the center, calculated as: \\[a_r = a \cos(\theta)\]
- For the particle in the problem: with \(a = 1.15 \, \text{m/s}^2\) and \(\theta = 38.0^\circ\), the radial acceleration \(a_r\) equals approximately \(0.91 \, \text{m/s}^2\).
- It ensures the particle maintains its circular path by constantly changing the direction of the velocity.
Speed Calculation
Calculating speed in circular motion can involve several steps depending on if we are finding the speed at one instant or after a period, accounting for tangential acceleration.
The initial speed \(v\) can be solved by equating the radial acceleration to the centripetal formula: \[a_r = \frac{v^2}{r}\]From this, in the exercise, we solved for \(v\) to find it was \(1.86 \,\text{m/s}\).
The initial speed \(v\) can be solved by equating the radial acceleration to the centripetal formula: \[a_r = \frac{v^2}{r}\]From this, in the exercise, we solved for \(v\) to find it was \(1.86 \,\text{m/s}\).
- Once the initial speed \(v_i\) is determined, future speed can be calculated using the formula for constant acceleration: \\[v_f = v_i + a_t \times t\]
- Since the tangential acceleration \(a_t\) is constant, the final speed after 2 seconds, as calculated in the exercise, becomes \(3.28 \,\text{m/s}\).
- This process highlights how both types of acceleration impact speed: radial acceleration affects direction, while tangential acceleration affects magnitude.
Other exercises in this chapter
Problem 60
(II) A particle starting from rest revolves with uniformly increasing speed in a clockwise circle in the \(x y\) plane. The center of the circle is at the origi
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(II) An object moves in a circle of radius \(22 \mathrm{~m}\) with its speed given by \(v=3.6+1.5 t^{2},\) with \(v\) in meters per second and \(t\) in seconds.
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(III) An object of mass \(m\) is constrained to move in a circle of radius \(r\). Its tangential acceleration as a function of time is given by \(a_{\tan }=b+c
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(II) The terminal velocity of a \(3 \times 10^{-5} \mathrm{~kg}\) raindrop is about \(9 \mathrm{~m} / \mathrm{s}\). Assuming a drag force \(F_{\mathrm{D}}=-b v\
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