Solve: #d^2x//dt^2 + g sin theta t =0# if # theta=g//l# , and g and l are constants?

Answer 1

#x(t) = - g sin(g/1) t^2/2 + At + B#

You want to know how to solve:

#(d^2x)/(dt^2) = - g sin(g/1) #
#implies (d x)/(dt) = - g sin(g/1) t + A#
#implies x(t) = - g sin(g/1) t^2/2 + At + B#
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Answer 2

# x = l^2/g \ sin theta t + At + B #

We have:

# (d^2x)/(dt^2) + g sintheta t = 0# where #theta=g/l#, a constant

which we could type as:

# (d^2x)/(dt^2) = - g sintheta t #

It is possible to "separate the variables" and obtain:

# (dx)/(dt) = int \ - g sintheta t \ dt #

Additionally, integrating provides us with:

# (dx)/(dt) = g/theta cos theta t + A #

And when we keep doing so, we obtain:

# x = int \ g/theta cos theta t + A \ dt #

So that:

# x = g/theta^2 sin theta t + At + B #
# \ \ = g/(g/l)^2 sin theta t + At + B #
# \ \ = g l^2/g^2 \ sin theta t + At + B #
# \ \ = l^2/g \ sin theta t + At + B #
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Answer 3

The solution to the differential equation ( \frac{{d^2x}}{{dt^2}} + g \sin(\frac{g}{l} t) = 0 ), where ( \theta = \frac{g}{l} ) and ( g ) and ( l ) are constants, involves solving the second-order linear homogeneous ordinary differential equation. This equation doesn't have a general analytical solution in terms of elementary functions. However, it can be solved numerically or approximated under specific conditions or using numerical methods.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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