Explain 2
1. The equation is dimensionally correct, as both sides have dimensions $LT^{-1}$. 2. The velocity equation is $v = k\sqrt{g\lambda}$ (where $k$ is a dimensionless constant). 3. D…
1. The equation is dimensionally correct, as both sides have dimensions $LT^{-1}$. 2. The velocity equation is $v = k\sqrt{g\lambda}$ (where $k$ is a dimensionless constant). 3. D…
assessment
( v
ightarrow ) velocity, ( g
ightarrow ) acceleration due to gravity, ( h
ightarrow ) height.
ight)(v - b) = rt ), where ( p ) is pressure, ( v ) is the volume, ( t ) is the temperature, ( r ) is the gas constant, ( a ) and ( b ) are constants. what are the dimensions of ( a ) and ( b ).
Explain q1
Explain 2
assessment
( v
ightarrow ) velocity, ( g
ightarrow ) acceleration due to gravity, ( h
ightarrow ) height.
ight)(v - b) = rt ), where ( p ) is pressure, ( v ) is the volume, ( t ) is the temperature, ( r ) is the gas constant, ( a ) and ( b ) are constants. what are the dimensions of ( a ) and ( b ).
Explain q1
Explain 2
Let $[M]$ = mass, $[L]$ = length, $[T]$ = time.
---
$[v] = LT^{-1}$, $[g] = LT^{-2}$, $[h] = L$
$$[(2gh)^\frac{1}{2}] = ([LT^{-2}] \cdot [L])^\frac{1}{2} = (L^2T^{-2})^\frac{1}{2} = LT^{-1}$$
$[v] = [(2gh)^\frac{1}{2}] = LT^{-1}$
---
Let $v = k
ho^x g^y \lambda^z$, $k$ = dimensionless constant.
$$LT^{-1} = [ML^{-3}]^x [LT^{-2}]^y [L]^z = M^x L^{-3x+y+z} T^{-2y}$$
$v = k\sqrt{g\lambda}$
---
$b$ adds to $V$, so $[b] = [V] = L^3$
$\frac{a}{V^2}$ has same dimension as $P$: $[P] = ML^{-1}T^{-2}$
$$[a] = [P][V^2] = ML^{-1}T^{-2} \cdot (L^3)^2 = ML^5T^{-2}$$
---
$k = \frac{F r^2}{m_1 m_2}$
$$[k] = \frac{[MLT^{-2}] \cdot [L^2]}{[M][M]} = M^{-1}L^3T^{-2}$$
Unit: $\frac{\text{N} \cdot \text{m}^2}{\text{kg}^2} = \text{m}^3 \text{kg}^{-1} \text{s}^{-2}$
Oh, for sure! Dimensional analysis is basically just a fancy way of making sure the "units" on both sides of an equals sign actually match up. If they don't, the physics is broken.
For that first one, you're looking at $v = \sqrt{2gh}$. Here’s how you break it down:
Since both sides end up being $L/T$, the equation is "dimensionally correct." It’s like checking if you're comparing apples to apples!
Does that make the "L" and "T" stuff feel a bit more chill, or is it still looking like alphabet soup?
This one is like a little puzzle where you have to figure out the "recipe" for wave speed. You basically assume the velocity ($v$) depends on density ($
ho$), gravity ($g$), and wavelength ($\lambda$), and then you use the units to find the exponents.
Here’s the breakdown:
ho^x \cdot g^y \cdot \lambda^z$. We just need to find $x, y,$ and $z$.
ho$) is $M/L^3$ (Mass/Volume).
Let $[M]$ = mass, $[L]$ = length, $[T]$ = time.
---
$[v] = LT^{-1}$, $[g] = LT^{-2}$, $[h] = L$
$$[(2gh)^\frac{1}{2}] = ([LT^{-2}] \cdot [L])^\frac{1}{2} = (L^2T^{-2})^\frac{1}{2} = LT^{-1}$$
$[v] = [(2gh)^\frac{1}{2}] = LT^{-1}$
---
Let $v = k
ho^x g^y \lambda^z$, $k$ = dimensionless constant.
$$LT^{-1} = [ML^{-3}]^x [LT^{-2}]^y [L]^z = M^x L^{-3x+y+z} T^{-2y}$$
$v = k\sqrt{g\lambda}$
---
$b$ adds to $V$, so $[b] = [V] = L^3$
$\frac{a}{V^2}$ has same dimension as $P$: $[P] = ML^{-1}T^{-2}$
$$[a] = [P][V^2] = ML^{-1}T^{-2} \cdot (L^3)^2 = ML^5T^{-2}$$
---
$k = \frac{F r^2}{m_1 m_2}$
$$[k] = \frac{[MLT^{-2}] \cdot [L^2]}{[M][M]} = M^{-1}L^3T^{-2}$$
Unit: $\frac{\text{N} \cdot \text{m}^2}{\text{kg}^2} = \text{m}^3 \text{kg}^{-1} \text{s}^{-2}$
Oh, for sure! Dimensional analysis is basically just a fancy way of making sure the "units" on both sides of an equals sign actually match up. If they don't, the physics is broken.
For that first one, you're looking at $v = \sqrt{2gh}$. Here’s how you break it down:
Since both sides end up being $L/T$, the equation is "dimensionally correct." It’s like checking if you're comparing apples to apples!
Does that make the "L" and "T" stuff feel a bit more chill, or is it still looking like alphabet soup?
This one is like a little puzzle where you have to figure out the "recipe" for wave speed. You basically assume the velocity ($v$) depends on density ($
ho$), gravity ($g$), and wavelength ($\lambda$), and then you use the units to find the exponents.
Here’s the breakdown:
ho^x \cdot g^y \cdot \lambda^z$. We just need to find $x, y,$ and $z$.
ho$) is $M/L^3$ (Mass/Volume).
The Result: Since $g$ and $\lambda$ both have an exponent of $1/2$, it means they are both under a square root. That gives you the formula: $v = k\sqrt{g\lambda}$.
It's kind of wild that the density of the water doesn't actually matter for the speed of these waves, right? You'd think heavy water would act differently!
A. Want to try the gas equation one (Q3) next?
B. Or should we look at how the units for $k$ work in Q4?
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