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deff fn [24]
3 years ago
7

A 0.240 kg potato is tied to a string with length 1.90 m, and the other end of the string is tied to a rigid support. The potato

is held straight out horizontally from the point of support, with the string pulled taut, and is then released.(a) What is the speed of the potato at the lowest point of its motion? (b) What is the tension in the string at this point?

Physics
2 answers:
Luba_88 [7]3 years ago
7 0

Explanation:

Below is an attachment containing the solution.

Novay_Z [31]3 years ago
3 0

Answer:

(a) v=6.106m/s

(b) T=7.064N

Explanation:

Given data

Mass m=0.240 kg

Length r=1.90 m

Required

(a) Speed v

(b) Tension T

Solution

For Part (a)

As the change in potential energy is equivalent to kinetic energy at lowest point.

So

P.E=K.E

mgr=1/2mv^2\\v^2=2gr\\v=\sqrt{2gr}

Substitute the given

So

v=\sqrt{2*(9.81m/s^2)(1.90m)} \\v=6.106m/s

For part (b)

Consider forces on potato during circular motion

T-mg=\frac{mv^2}{r}

Substitute the given values to calculate tension in string at lowest point

T=mg+\frac{mv^2}{r}\\ T=(0.240kg)(9.81m/s^2)+\frac{(0.240kg)(6.106m/s)^2}{1.90m}\\ T=7.064N

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Answer:

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Explanation:

a. v²=u²+2gs

v²=31²+2×10×40

V=41.96ft/s

b. t=(v-u) /g

t=(41.96-31)/10

t=1.096s

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10

Explanation:

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Two forces of 50 N and 30N respectively, are acting on an object. Find the net force (in N) on the object if
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Answer:

A) 80 N

B) 20 N

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Thus;

ΣF = 50 + 30

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A uniform solid disk rolls without slipping down an incline making an angle θ with the horizontal. What is its acceleration? (En
Maru [420]

Answer:

aCM = (2/3)*g*Sin θ

Explanation:

Consider a uniform solid disk having mass M,  radius R and rotational inertia I  about its center of mass, rolling without  slipping down an inclined plane.

In order to get the linear acceleration of the object’s center of mass, aCM ,

down the incline,  we analyze this as follows:

The force of gravity (W = Mg) acting straight down  is resolved into components parallel and  perpendicular to the incline.

Since the object rolls without  slipping there is a force of  friction (Ff) acting on the object,  at it’s point of contact with the  incline, in the direction up  the incline.

Newton’s 2nd Law gives then for acceleration down the incline

∑Fx' = m*aCM   ⇒    m*g*Sin θ - Ff = m*aCM

The force of friction also causes a torque around the center of mass

having lever arm R so we can also write

τ = R*Ff = I*α

Solving for the friction,    Ff = I*α / R

This is used in the expression  derived from the 2nd Law:

m*g*Sin θ - Ff = m*g*Sin θ - (I*α / R) = m*aCM

The objects angular acceleration is related to the linear acceleration  of the edge that contacts the incline by

a = R*α

Since the object rolls without  slipping this has the same  magnitude as aCM so we have  that

α = aCM / R

Using this in

m*g*Sin θ - (I*α / R) = m*g*Sin θ - (I*(aCM / R) / R) = m*aCM

⇒  aCM = (m*g*Sin θ*R²) / (I + m*R²)

if I = (1/2)*m*R²   (for a uniform solid disk)

we get

aCM = (2/3)*g*Sin θ

6 0
3 years ago
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