Physical Quantities, Units and Dimensions

18 soru

Soru 1Soru

The aerodynamic drag force FF acting on an object moving through a fluid of density ρ\rho with cross-sectional area AA at speed vv is modeled by the equation F=12CdρaAbvcF = \frac{1}{2} C_d \rho^a A^b v^c, where CdC_d is a dimensionless constant. Using dimensional analysis, what is the numerical value of the exponent cc?

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Cevap: 2

Cevap

The numerical value of the exponent cc is 2.
By applying the principle of dimensional homogeneity, the base dimension of time on the left side is T2\text{T}^{-2} (from force [F]=M L T2[F] = \text{M L T}^{-2}). On the right side, the only quantity containing time is velocity [v]=L T1[v] = \text{L T}^{-1}, raised to power cc, giving Tc\text{T}^{-c}. Equating the exponents gives 2=c-2 = -c, so c=2c = 2.

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1
Identify the base dimensions of each physical quantity in the given equation.
[F]=M L T2[F] = \text{M L T}^{-2}, [ρ]=M L3[\rho] = \text{M L}^{-3}, [A]=L2[A] = \text{L}^2, and [v]=L T1[v] = \text{L T}^{-1}. CdC_d is dimensionless ([Cd]=1[C_d] = 1).
Dimensional homogeneity requires both sides of a physical equation to have identical base dimensions.
2
Substitute the base dimensions into the formula F=12CdρaAbvcF = \frac{1}{2} C_d \rho^a A^b v^c and simplify.
\text{M L T}^{-2} = (\text{M L}^{-3})^a (\text{L}^2)^b (\text{L T}^{-1})^c = \text{M}^a \text{L}^{-3a + 2b + c} \text{T}^{-c}.
Combining powers of base dimensions allows direct comparison of corresponding exponents.
3
Equate the exponent of time (T) on both sides of the dimensional equation.
-2 = -c \implies c = 2.
The exponent of T on the left side is -2, which must equal the exponent of T on the right side (-c).

Anahtar Kavram

Principle of Dimensional Homogeneity
Tahmini Süre:1m 15s
Soru 2Soru

The physical quantity impulse is defined as the product of force and time. Which of the following physical quantities has the same dimensions as impulse?

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Cevap: Linear momentum

Cevap

Linear momentum
Linear momentum is calculated as mass times velocity, which yields the base dimensions [MLT1][M L T^{-1}]. This is identical to impulse, which is force times time ([MLT2]×[T]=[MLT1][M L T^{-2}] \times [T] = [M L T^{-1}]).

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1
Determine the dimensions of impulse.
Impulse=Force×Time=[MLT2][T]=[MLT1]\text{Impulse} = \text{Force} \times \text{Time} = [M L T^{-2}][T] = [M L T^{-1}]
Force has base dimensions [MLT2][M L T^{-2}] and time has dimension [T][T].
2
Determine the dimensions of linear momentum.
Linear Momentum=Mass×Velocity=[M][LT1]=[MLT1]\text{Linear Momentum} = \text{Mass} \times \text{Velocity} = [M][L T^{-1}] = [M L T^{-1}]
Mass has base dimension [M][M] and velocity has dimensions [LT1][L T^{-1}].
3
Compare the dimensions of impulse and linear momentum.
Both quantities have identical dimensions of [MLT1][M L T^{-1}].
By the impulse-momentum theorem, impulse equals change in momentum.

Anahtar Kavram

Dimensional analysis of physical quantities
Soru 3Soru

The mechanical power PP dissipated by a circular disc of radius RR rotating at an angular velocity ω\omega in a fluid of density ρ\rho is given by the relation P=kρaωbRcP = k \cdot \rho^a \cdot \omega^b \cdot R^c, where kk is a dimensionless constant. Using dimensional analysis, which of the following represents the correct values of the exponents aa, bb, and cc?

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Cevap: a=1,b=3,c=5a = 1, b = 3, c = 5

Cevap

a=1,b=3,c=5a = 1, b = 3, c = 5
By writing the dimensions of power as [ML2T3][M L^2 T^{-3}], density as [ML3][M L^{-3}], angular velocity as [T1][T^{-1}], and radius as [L][L], dimensional homogeneity requires that ML2T3=MaL3a+cTbM L^2 T^{-3} = M^a L^{-3a + c} T^{-b}. Equating powers gives a=1a = 1, b=3b = 3, and c=5c = 5.

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1
Express the base dimensions for each physical quantity
Power [P]=ML2T3[P] = M L^2 T^{-3}, Density [ρ]=ML3[\rho] = M L^{-3}, Angular velocity [ω]=T1[\omega] = T^{-1}, and Radius [R]=L[R] = L.
Dimensional analysis requires decomposing derived physical quantities into fundamental dimensions of mass (MM), length (LL), and time (TT).
2
Substitute dimensions into the given equation P=kρaωbRcP = k \cdot \rho^a \cdot \omega^b \cdot R^c
ML2T3=(ML3)a(T1)b(L)c=MaL3a+cTbM L^2 T^{-3} = (M L^{-3})^a \cdot (T^{-1})^b \cdot (L)^c = M^a \cdot L^{-3a + c} \cdot T^{-b}.
The constant kk is dimensionless, so its dimension is 1.
3
Equate the powers of MM, LL, and TT on both sides of the equation
For mass MM: a=1a = 1. For time TT: b=3    b=3-b = -3 \implies b = 3. For length LL: 3a+c=2    3(1)+c=2    c=5-3a + c = 2 \implies -3(1) + c = 2 \implies c = 5.
According to the principle of dimensional homogeneity, powers of fundamental dimensions must be equal on both sides of a physically correct equation.

Anahtar Kavram

Dimensional Homogeneity and Formula Derivation
Tahmini Süre:2m 0s
Soru 4Soru
The volume flow rate QQ of a viscous liquid flowing through a pipe of radius rr under a pressure gradient ΔPl\frac{\Delta P}{l} is modeled by the equation:
Q=kηxry(ΔPl)zQ = k \eta^x r^y \left(\frac{\Delta P}{l}\right)^z
where η\eta is the coefficient of dynamic viscosity and kk is a dimensionless constant. What are the values of the exponents xx, yy, and zz respectively?
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Cevap: x=1,y=4,z=1x = -1, y = 4, z = 1

Cevap

x=1x = -1, y=4y = 4, and z=1z = 1
The dimensional representation of volume flow rate is [L3T1][L^3 T^{-1}], dynamic viscosity is [ML1T1][M L^{-1} T^{-1}], radius is [L][L], and pressure gradient is [ML2T2][M L^{-2} T^{-2}]. Equating the powers of MM, LL, and TT gives x+z=0x + z = 0, x2z=1-x - 2z = -1, and x+y2z=3-x + y - 2z = 3. Solving these simultaneously yields x=1x = -1, y=4y = 4, and z=1z = 1.

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1
Determine the fundamental dimensions of each physical quantity
Volume flow rate Q=VolumeTime=[L3T1]Q = \frac{\text{Volume}}{\text{Time}} = [L^3 T^{-1}];
Dynamic viscosity η=[ML1T1]\eta = [M L^{-1} T^{-1}];
Radius r=[L]r = [L];
Pressure gradient ΔPl=PressureLength=[ML1T2][L]=[ML2T2]\frac{\Delta P}{l} = \frac{\text{Pressure}}{\text{Length}} = \frac{[M L^{-1} T^{-2}]}{[L]} = [M L^{-2} T^{-2}].
Correct base dimensions are required for dimensional analysis.
2
Set up the dimensional equation by substituting the base dimensions into the formula
[L3T1]=[ML1T1]x[L]y[ML2T2]z=Mx+zLx+y2zTx2z[L^3 T^{-1}] = [M L^{-1} T^{-1}]^x [L]^y [M L^{-2} T^{-2}]^z = M^{x+z} L^{-x + y - 2z} T^{-x - 2z}.
The principle of dimensional homogeneity requires both sides of the equation to have matching exponents for MM, LL, and TT.
3
Equate exponents for MM, TT, and LL to form algebraic equations
For MM: x+z=0    z=xx + z = 0 \implies z = -x
For TT: x2z=1-x - 2z = -1
For LL: x+y2z=3-x + y - 2z = 3.
This creates a linear system of equations for the exponents xx, yy, and zz.
4
Solve the system of linear equations
Substituting z=xz = -x into the TT equation: x2(x)=1    x=1-x - 2(-x) = -1 \implies x = -1.
Hence z=(1)=1z = -(-1) = 1.
Substituting x=1x = -1 and z=1z = 1 into the LL equation: (1)+y2(1)=3    1+y2=3    y=4-(-1) + y - 2(1) = 3 \implies 1 + y - 2 = 3 \implies y = 4.
Yields the unique set of exponents x=1,y=4,z=1x = -1, y = 4, z = 1.

Anahtar Kavram

Dimensional Analysis and Homogeneity
Tahmini Süre:2m 0s
Soru 5Soru

The speed vv of a transverse wave traveling along a stretched string under tension TT with mass per unit length μ\mu is given by v=kTxμyv = k T^x \mu^y, where kk is a dimensionless constant. What is the numerical value of the exponent xx?

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Cevap: 0.5

Cevap

The numerical value of the exponent xx is 0.5.
Applying the principle of dimensional homogeneity, the dimensions on both sides must match. Speed [v]=LT1[v] = L T^{-1}, tension force [T]=MLT2[T] = M L T^{-2}, and mass per unit length [μ]=ML1[\mu] = M L^{-1}. Substituting these into v=kTxμyv = k T^x \mu^y yields M0L1T1=Mx+yLxyT2xM^0 L^1 T^{-1} = M^{x+y} L^{x-y} T^{-2x}. Comparing the exponents of TT gives 2x=1-2x = -1, leading to x=0.5x = 0.5.

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1
Determine the dimensions of speed vv, tension force TT, and linear density μ\mu.
[v]=LT1[v] = L T^{-1}, [T]=MLT2[T] = M L T^{-2}, [μ]=ML1[\mu] = M L^{-1}
Tension is a force (F=maF=ma) with dimensions [MLT2][M L T^{-2}], and μ\mu is mass per unit length (m/lm/l) with dimensions [ML1][M L^{-1}].
2
Substitute the dimensional formulas into the equation v=kTxμyv = k T^x \mu^y and collect powers of base dimensions.
M0L1T1=Mx+yLxyT2xM^0 L^1 T^{-1} = M^{x+y} L^{x-y} T^{-2x}
Combining exponents for base dimensions MM, LL, and TT allows applying the principle of dimensional homogeneity.
3
Equate the exponent of TT on both sides to solve for xx.
2x=1    x=0.5-2x = -1 \implies x = 0.5
The exponent of TT on the left side is 1-1 and on the right side is 2x-2x.

Anahtar Kavram

Dimensional Analysis and Determination of Exponents
Tahmini Süre:1m 30s
Soru 6Soru

The viscous drag force FF acting on a spherical body moving through a fluid at speed vv is given by Stokes' law, F=6πηrvF = 6 \pi \eta r v, where rr is the radius of the sphere and η\eta is the coefficient of viscosity. What is the dimensional formula of the coefficient of viscosity η\eta?

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Cevap: M L1T1\text{M L}^{-1} \text{T}^{-1}

Cevap

The dimensional formula of the coefficient of viscosity is M L1T1\text{M L}^{-1} \text{T}^{-1}.
Isolating the coefficient of viscosity from Stokes' law yields η=F6πrv\eta = \frac{F}{6\pi r v}. Substituting the dimensions [F]=M L T2[F] = \text{M L T}^{-2}, [r]=L[r] = \text{L}, and [v]=L T1[v] = \text{L T}^{-1} gives [η]=M L T2L2T1=M L1T1[\eta] = \frac{\text{M L T}^{-2}}{\text{L}^2 \text{T}^{-1}} = \text{M L}^{-1} \text{T}^{-1}.

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1
Identify the dimensional formulas for force, radius, and velocity.
[F]=M L T2[F] = \text{M L T}^{-2}, [r]=L[r] = \text{L}, and [v]=L T1[v] = \text{L T}^{-1}.
Base physical quantities must be represented by their fundamental dimensions.
2
Rearrange Stokes' law to express η\eta in terms of the other variables, treating 6π6\pi as a dimensionless constant.
[η]=[F][r][v][\eta] = \frac{[F]}{[r][v]}.
Numerical constants do not carry physical dimensions.
3
Substitute the base dimensions into the formula and simplify using index rules.
[η]=M L T2LL T1=M L T2L2T1=M L1T1[\eta] = \frac{\text{M L T}^{-2}}{\text{L} \cdot \text{L T}^{-1}} = \frac{\text{M L T}^{-2}}{\text{L}^2 \text{T}^{-1}} = \text{M L}^{-1} \text{T}^{-1}.
Subtracting denominator indices from numerator indices yields the final dimensional expression.

Anahtar Kavram

Dimensional analysis of physical constants and equations
Soru 7Soru

In Newton's law of universal gravitation, the gravitational force FF between two point masses m1m_1 and m2m_2 separated by a distance rr is expressed as F=Gm1m2r2F = G \frac{m_1 m_2}{r^2}, where GG is the universal gravitational constant. What is the dimensional formula of GG in terms of mass (M\text{M}), length (L\text{L}), and time (T\text{T})?

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Cevap: M1L3T2\text{M}^{-1}\text{L}^3\text{T}^{-2}

Cevap

M1L3T2\text{M}^{-1}\text{L}^3\text{T}^{-2}
The dimensional formula of the universal gravitational constant GG is derived by expressing G=Fr2m1m2G = \frac{F r^2}{m_1 m_2}. Substituting the basic dimensions of force (MLT2\text{M}\text{L}\text{T}^{-2}), radius squared (L2\text{L}^2), and mass squared (M2\text{M}^2) gives (MLT2)(L2)M2=M1L3T2\frac{(\text{M}\text{L}\text{T}^{-2})(\text{L}^2)}{\text{M}^2} = \text{M}^{-1}\text{L}^3\text{T}^{-2}.

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1
Make GG the subject of the formula
G=Fr2m1m2G = \frac{F \cdot r^2}{m_1 \cdot m_2}
To analyze the dimensions of GG, isolate it on one side of the equation.
2
Substitute the fundamental dimensions for force, distance, and mass
[F] = \text{M}\text{L}\text{T}^{-2}, [r^2] = \text{L}^2, [m_1 m_2] = \text{M}^2
Force is mass times acceleration, giving dimensions MLT2\text{M}\text{L}\text{T}^{-2}, while distance squared gives L2\text{L}^2 and the product of two masses gives M2\text{M}^2.
3
Simplify the dimensional expression
[G] = \frac{(\text{M}\text{L}\text{T}^{-2}) \cdot \text{L}^2}{\text{M}^2} = \text{M}^{1-2} \text{L}^{1+2} \text{T}^{-2} = \text{M}^{-1}\text{L}^3\text{T}^{-2}
Apply laws of indices for fundamental dimensions M\text{M}, L\text{L}, and T\text{T}.

Anahtar Kavram

Dimensional Analysis of Physical Constants
Tahmini Süre:1m 15s
Soru 8Soru

The speed vv of a longitudinal wave propagating through a gas depends on the pressure PP of the gas and its density ρ\rho according to the dimensional relationship v=CPxρyv = C P^x \rho^y, where CC is a dimensionless constant. Using dimensional analysis, what is the numerical value of xyx - y?

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Cevap: 1

Cevap

The numerical value of xyx - y is 1.0.
By applying the principle of dimensional homogeneity, the exponents are determined as x=0.5x = 0.5 (for pressure) and y=0.5y = -0.5 (for density). Thus, xy=0.5(0.5)=1.0x - y = 0.5 - (-0.5) = 1.0.

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1
Determine the dimensions of speed, pressure, and density.
[v]=[LT1][v] = [L T^{-1}], [P]=[ML1T2][P] = [M L^{-1} T^{-2}], and [ρ]=[ML3][\rho] = [M L^{-3}].
Dimensional homogeneity requires expressed physical quantities to be broken down into fundamental dimensions (MM, LL, TT).
2
Substitute dimensions into the relationship v=CPxρyv = C P^x \rho^y.
[LT1]=[ML1T2]x[ML3]y=Mx+yLx3yT2x[L T^{-1}] = [M L^{-1} T^{-2}]^x \, [M L^{-3}]^y = M^{x+y} \, L^{-x-3y} \, T^{-2x}.
This establishes a system of algebraic equations by equating exponents of corresponding fundamental dimensions.
3
Solve for exponents xx and yy.
From time TT: 2x=1    x=0.5-2x = -1 \implies x = 0.5. From mass MM: x+y=0    y=0.5x + y = 0 \implies y = -0.5.
Equating the powers of fundamental dimensions on both sides yields the values of xx and yy.
4
Calculate the required expression (xy)(x - y).
xy=0.5(0.5)=1.0x - y = 0.5 - (-0.5) = 1.0.
Subtracting negative 0.50.5 from 0.50.5 results in 1.01.0.

Anahtar Kavram

Dimensional Analysis and Homogeneity
Soru 9Soru

The critical velocity vcv_c of a fluid flowing through a cylindrical pipe of diameter DD depends on the dynamic viscosity η\eta of the fluid, its density ρ\rho, and the pipe diameter DD according to the empirical relationship vc=ReηxρyDzv_c = R_e \eta^x \rho^y D^z, where ReR_e is the dimensionless Reynolds number. Using dimensional analysis, calculate the numerical value of the sum of the exponents x+y+zx + y + z.

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Cevap: -1

Cevap

The sum of the exponents x+y+zx + y + z is 1-1.
Using the principle of dimensional homogeneity, the dimensions of both sides of the formula vc=ReηxρyDzv_c = R_e \eta^x \rho^y D^z must be equal. Equating the powers of Mass, Length, and Time yields x=1x = 1, y=1y = -1, and z=1z = -1. Summing these three values gives 1+(1)+(1)=11 + (-1) + (-1) = -1.

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1
Determine the dimensions of all physical quantities involved
Critical velocity [vc]=L T1[v_c] = \text{L T}^{-1}, dynamic viscosity [η]=M L1T1[\eta] = \text{M L}^{-1} \text{T}^{-1}, fluid density [ρ]=M L3[\rho] = \text{M L}^{-3}, and diameter [D]=L[D] = \text{L}. The Reynolds number ReR_e is dimensionless.
Dimensional analysis requires replacing physical quantities with their base SI dimensions.
2
Formulate the dimensional homogeneity equation
\text{M}^0 \text{L}^1 \text{T}^{-1} = (\text{M L}^{-1} \text{T}^{-1})^x (\text{M L}^{-3})^y (\text{L})^z = \text{M}^{x+y} \text{L}^{-x-3y+z} \text{T}^{-x}.
By the principle of dimensional homogeneity, the total exponent of each fundamental dimension must match on both sides of the equation.
3
Solve the system of simultaneous linear equations for xx, yy, and zz
From T\text{T}: x=1    x=1-x = -1 \implies x = 1.
From M\text{M}: x+y=0    y=1x + y = 0 \implies y = -1.
From L\text{L}: x3y+z=1    1+3+z=1    z=1-x - 3y + z = 1 \implies -1 + 3 + z = 1 \implies z = -1.
Equating powers of fundamental quantities yields explicit values for each dimensional power.
4
Calculate the target sum x+y+zx + y + z
x + y + z = 1 + (-1) + (-1) = -1.
Combining the calculated exponents gives the required numerical value.

Anahtar Kavram

Principle of Dimensional Homogeneity and Derivation of Physical Formulas
Soru 10Soru

The frequency of oscillation ff of a small liquid droplet executing spherical oscillations depends on the surface tension γ\gamma of the liquid, its mass density ρ\rho, and the radius rr of the droplet according to the relationship f=kγaρbrcf = k \gamma^a \rho^b r^c, where kk is a dimensionless constant. Which of the following represents the correct value of the exponent cc?

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Cevap: 32-\frac{3}{2}

Cevap

The correct value of the exponent cc is 32-\frac{3}{2}.
By writing the dimensional equation [M0L0T1]=[MT2]a[ML3]b[L]c[M^0 L^0 T^{-1}] = [M T^{-2}]^a [M L^{-3}]^b [L]^c, we solve for the exponents: 2a=1-2a = -1 gives a=1/2a = 1/2, a+b=0a + b = 0 gives b=1/2b = -1/2, and 3b+c=0-3b + c = 0 gives 3/2+c=0    c=3/23/2 + c = 0 \implies c = -3/2. Thus, the option equal to 3/2-3/2 is correct.

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1
Express each physical quantity in terms of its base dimensions [M][M], [L][L], and [T][T].
Frequency f=[T1]f = [T^{-1}], Surface tension γ=ForceLength=[MT2]\gamma = \frac{\text{Force}}{\text{Length}} = [M T^{-2}], Density ρ=[ML3]\rho = [M L^{-3}], and Radius r=[L]r = [L].
Dimensional analysis requires reducing derived physical quantities to their base units.
2
Substitute dimensions into the given formula f=kγaρbrcf = k \gamma^a \rho^b r^c.
[M0L0T1]=[MT2]a[ML3]b[L]c=Ma+bL3b+cT2a[M^0 L^0 T^{-1}] = [M T^{-2}]^a [M L^{-3}]^b [L]^c = M^{a+b} L^{-3b+c} T^{-2a}.
The principle of dimensional homogeneity requires both sides of a physical equation to have matching dimensions.
3
Equate exponents for each base dimension MM, LL, and TT.
For TT: 2a=1    a=12-2a = -1 \implies a = \frac{1}{2}. For MM: a+b=0    b=a=12a + b = 0 \implies b = -a = -\frac{1}{2}. For LL: 3b+c=0    3(12)+c=0-3b + c = 0 \implies -3\left(-\frac{1}{2}\right) + c = 0.
Matching powers across orthogonal base dimensions provides a system of linear equations.
4
Solve for the target exponent cc.
\frac{3}{2} + c = 0 \implies c = -\frac{3}{2}.
Subtracting 3/23/2 from both sides gives the exact value of exponent cc.

Anahtar Kavram

Dimensional Homogeneity and Dimensional Analysis
Tahmini Süre:2m 0s
Soru 11Soru

The physical quantity work is defined as the product of force and displacement. What are the dimensional exponents aa, bb, and cc for mass, length, and time respectively in the dimensional formula for work, [MaLbTc][M^a L^b T^c]?

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Cevap: 1,2,21, 2, -2

Cevap

The dimensional exponents for mass, length, and time in the expression for work are a=1a = 1, b=2b = 2, and c=2c = -2.
Work is calculated as force multiplied by displacement. Since force has dimensions [MLT2][M L T^{-2}] and displacement has dimension [L][L], the resulting dimensional formula for work is [M1L2T2][M^1 L^2 T^{-2}]. The exponents of MM, LL, and TT are therefore 11, 22, and 2-2 respectively.

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1
Express the dimensions of force using base quantities
\text{Force} = \text{mass} \times \text{acceleration} = [M] \times [L T^{-2}] = [M L T^{-2}]
Acceleration has the dimensions of length divided by time squared.
2
Multiply force dimensions by displacement dimension to find the dimensions of work
\text{Work} = \text{Force} \times \text{Displacement} = [M L T^{-2}] \times [L] = [M^1 L^2 T^{-2}]
Displacement is a measure of length, contributing an additional factor of [L][L].
3
Extract the exponents aa, bb, and cc
a = 1, b = 2, c = -2
Comparing [MaLbTc][M^a L^b T^c] to [M1L2T2][M^1 L^2 T^{-2}] gives the values of aa, bb, and cc.

Anahtar Kavram

Dimensional analysis of work
Soru 12Soru

The acoustic intensity SS (defined as power per unit area) of a sound wave propagating through a medium of density ρ\rho at speed vv is given by the empirical relationship S=kAxω2ρvwS = k A^x \omega^2 \rho v^w, where AA is the wave displacement amplitude, ω\omega is the angular frequency, and kk is a dimensionless constant. Using the principles of dimensional analysis, calculate the numerical value of the exponent xx.

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Cevap: 2

Cevap

The numerical value of the exponent xx is 2.
By applying the principle of dimensional homogeneity, the dimensions of intensity [S]=MT3[S] = M T^{-3} are equated to [A]x[ω]2[ρ][v]w=MLx3+wT2w[A]^x [\omega]^2 [\rho] [v]^w = M L^{x - 3 + w} T^{-2 - w}. Equating time exponents yields 3=2w    w=1-3 = -2 - w \implies w = 1. Equating length exponents yields 0=x3+w    x=20 = x - 3 + w \implies x = 2.

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1
Determine the fundamental dimensions of acoustic intensity SS
[S]=[Power][Area]=ML2T3L2=ML0T3[S] = \frac{[\text{Power}]}{[\text{Area}]} = \frac{M L^2 T^{-3}}{L^2} = M L^0 T^{-3}
Intensity is defined as power delivered per unit surface area perpendicular to the direction of propagation.
2
Write the dimensional formulas for all variables in the given equation S=kAxω2ρ1vwS = k A^x \omega^2 \rho^1 v^w
[A]=L[A] = L, [ω]=T1[\omega] = T^{-1}, [ρ]=ML3[\rho] = M L^{-3}, [v]=LT1[v] = L T^{-1}
Each physical quantity must be resolved into fundamental SI dimensions of Mass (MM), Length (LL), and Time (TT).
3
Formulate the dimensional balance equation
M1L0T3=LxT2M1L3LwTw=M1Lx3+wT2wM^1 L^0 T^{-3} = L^x \cdot T^{-2} \cdot M^1 L^{-3} \cdot L^w T^{-w} = M^1 L^{x - 3 + w} T^{-2 - w}
For physical validity, the dimensions on both sides of an equation must be identical (principle of dimensional homogeneity).
4
Equate the exponents of Time (TT) to solve for ww
3=2w    w=1-3 = -2 - w \implies w = 1
The power of TT on the left side must equal the sum of powers of TT on the right side.
5
Equate the exponents of Length (LL) to find xx
0=x3+w    0=x3+1    x=20 = x - 3 + w \implies 0 = x - 3 + 1 \implies x = 2
Substituting w=1w = 1 into the length exponent balance yields the value of xx.

Anahtar Kavram

Principle of Dimensional Homogeneity
Tahmini Süre:2m 0s
Soru 13Soru

The couple per unit twist CC (torque per unit angle of twist) of a solid wire of length LL, radius rr, and shear modulus η\eta is modeled by the equation:

C=πηrx2LC = \frac{\pi \eta r^x}{2 L}

Using dimensional analysis, determine the numerical value of the exponent xx.

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Cevap: 4

Cevap

The numerical value of the exponent x is 4.
Applying the principle of dimensional homogeneity requires the dimensions of couple per unit twist [M L2T2][\text{M L}^2 \text{T}^{-2}] to equal the dimensions of ηrxL\frac{\eta r^x}{L}, which simplifies to [M Lx2T2][\text{M L}^{x-2} \text{T}^{-2}]. Equating exponents of length gives 2=x22 = x - 2, yielding x=4x = 4.

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1
Determine the dimensional formula of couple per unit twist CC.
[C]=M L2T2[C] = \text{M L}^2 \text{T}^{-2}
Couple (torque) is force multiplied by perpendicular distance, which has dimensions [M L T2][L]=[M L2T2][\text{M L T}^{-2}][\text{L}] = [\text{M L}^2 \text{T}^{-2}]. The angle of twist (in radians) is dimensionless.
2
Determine the dimensional formula of shear modulus η\eta.
[η]=M L1T2[\eta] = \text{M L}^{-1} \text{T}^{-2}
Shear modulus is defined as shear stress divided by shear strain. Stress has dimensions of force per unit area [M L T2]/[L2]=[M L1T2][\text{M L T}^{-2}]/[\text{L}^2] = [\text{M L}^{-1} \text{T}^{-2}], while strain is dimensionless.
3
Set up the dimensional equation for the relation C=πηrx2LC = \frac{\pi \eta r^x}{2 L}.
[M L2T2]=[M L1T2][L]x[L]=[M Lx2T2][\text{M L}^2 \text{T}^{-2}] = \frac{[\text{M L}^{-1} \text{T}^{-2}][\text{L}]^x}{[\text{L}]} = [\text{M L}^{x-2} \text{T}^{-2}]
Pure numerical constants such as π\pi and 22 are dimensionless. Length LL and radius rr both have dimension [L][\text{L}].
4
Equate the exponents of length L\text{L} on both sides of the dimensional equation.
x=4x = 4
Comparing powers of L\text{L} on both sides gives 2=x22 = x - 2, which solves to x=4x = 4.

Anahtar Kavram

Dimensional Homogeneity in Mechanics
Soru 14Soru

The tensile stress σ\sigma on a solid wire subjected to a stretching force FF is defined as force per unit cross-sectional area, while the fractional change in length is the tensile strain ϵ\epsilon. If Young's modulus YY of the material is given by Y=σϵY = \frac{\sigma}{\epsilon}, which of the following is the SI unit of Young's modulus expressed in fundamental SI base units?

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Cevap: kgm1s2\text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}

Cevap

kgm1s2\text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}
Young's modulus is calculated as tensile stress divided by tensile strain. Since tensile strain is the ratio of change in length to original length, it has no units. Therefore, the SI unit of Young's modulus is identical to that of stress. Stress is force divided by area: kgms2m2=kgm1s2\frac{\text{kg}\cdot\text{m}\cdot\text{s}^{-2}}{\text{m}^2} = \text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}.

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1
Determine the dimensions of the force component
Force F=ma    [F]=kgms2F = ma \implies [F] = \text{kg}\cdot\text{m}\cdot\text{s}^{-2}
Mass has fundamental unit kg\text{kg} and acceleration has derived unit ms2\text{m}\cdot\text{s}^{-2}.
2
Determine the SI base units of tensile stress σ\sigma
[\sigma] = \frac{[F]}{\text{Area}} = \frac{\text{kg}\cdot\text{m}\cdot\text{s}^{-2}}{\text{m}^2} = \text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}$
Stress is defined as force divided by cross-sectional area (A=m2A = \text{m}^2).
3
Evaluate the unit of Young's modulus YY
[Y] = \frac{[\sigma]}{[\epsilon]} = \frac{\text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}}{1} = \text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-2}$
Strain ϵ=ΔLL\epsilon = \frac{\Delta L}{L} is the ratio of two lengths and is dimensionless.

Anahtar Kavram

Derivation of SI base units for mechanical moduli from physical definitions
Tahmini Süre:1m 15s
Soru 15Soru

The centripetal acceleration aa of a particle moving in a circular path depends on its linear speed vv and the radius rr of the path according to the formula a=kvxrya = k v^x r^y, where kk is a dimensionless constant. Using dimensional analysis, what is the numerical value of the product xyx \cdot y?

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Cevap: -2

Cevap

The numerical value of the product xyx \cdot y is 2-2.
By dimensional analysis, centripetal acceleration has dimensions [a]=L T2[a] = \text{L T}^{-2}, velocity [v]=L T1[v] = \text{L T}^{-1}, and radius [r]=L[r] = \text{L}. Substituting into a=kvxrya = k v^x r^y gives L T2=Lx+yTx\text{L T}^{-2} = \text{L}^{x+y} \text{T}^{-x}. Equating exponents of time yields x=2    x=2-x = -2 \implies x = 2. Equating exponents of length gives x+y=1    2+y=1    y=1x + y = 1 \implies 2 + y = 1 \implies y = -1. Consequently, xy=2(1)=2x \cdot y = 2 \cdot (-1) = -2.

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1
Identify the base dimensions for each physical quantity.
[a]=M0L1T2[a] = \text{M}^0 \text{L}^1 \text{T}^{-2}, [v]=M0L1T1[v] = \text{M}^0 \text{L}^1 \text{T}^{-1}, and [r]=M0L1T0[r] = \text{M}^0 \text{L}^1 \text{T}^0.
Dimensional analysis requires substituting fundamental dimensions of mass, length, and time.
2
Set up the dimensional homogeneity equation.
\text{L}^1 \text{T}^{-2} = (\text{L T}^{-1})^x \cdot (\text{L})^y = \text{L}^{x+y} \text{T}^{-x}.
Since kk is dimensionless, the net dimensions on both sides of the equation must be identical.
3
Solve for exponents xx and yy by equating powers of corresponding base units.
For \text{T}: x=2    x=2-x = -2 \implies x = 2. For \text{L}: x+y=1    2+y=1    y=1x + y = 1 \implies 2 + y = 1 \implies y = -1.
Equating coefficients of identical base dimensions gives a system of linear equations.
4
Multiply the derived values of xx and yy.
xy=2(1)=2x \cdot y = 2 \cdot (-1) = -2.
The question asks specifically for the product of exponents xx and yy.

Anahtar Kavram

Dimensional Homogeneity and Exponent Analysis
Soru 16Soru

The energy density uu (defined as energy per unit volume) stored in an electrostatic field is related to the permittivity of free space ϵ0\epsilon_0 and the electric field strength EE by the dimensional formula u=kϵ0xEyu = k \epsilon_0^x E^y, where kk is a dimensionless constant. What is the value of the numerical exponent yy?

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Cevap: 2

Cevap

The value of the exponent yy is 2.
By writing the dimensions of energy density [ML1T2][M L^{-1} T^{-2}], permittivity [M1L3T4I2][M^{-1} L^{-3} T^4 I^2], and electric field strength [MLT3I1][M L T^{-3} I^{-1}], equating powers of electric current II yields 2xy=02x - y = 0 (or y=2xy = 2x). Substituting this into the equation for powers of mass MM, x+y=1-x + y = 1, yields x+2x=1-x + 2x = 1, so x=1x = 1 and y=2y = 2.

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1
Derive the dimensional formulas for energy density uu, permittivity ϵ0\epsilon_0, and electric field EE.
[u] = M L^{-1} T^{-2}, [\epsilon_0] = M^{-1} L^{-3} T^4 I^2, [E] = M L T^{-3} I^{-1}.
Expressing quantities in terms of base dimensions (M, L, T, I) is required for dimensional homogeneity.
2
Form the dimensional equation u=kϵ0xEyu = k \epsilon_0^x E^y and combine powers.
M L^{-1} T^{-2} = M^{-x+y} L^{-3x+y} T^{4x-3y} I^{2x-y}.
Applies the principle of dimensional consistency across the formula.
3
Equate corresponding powers of base dimensions to set up equations for xx and yy.
For I: 2x - y = 0; for M: -x + y = 1.
Base unit exponents on both sides of a physically valid equation must match.
4
Solve the algebraic equations for the unknown exponent yy.
x = 1, y = 2.
Substituting y = 2x into -x + y = 1 directly gives x = 1 and y = 2.

Anahtar Kavram

Dimensional Analysis and Dimensional Homogeneity
Tahmini Süre:1m 30s
Soru 17Soru

The torque τ\tau required to rotate a thin flat disk of radius rr at a constant angular velocity ω\omega in a fluid of dynamic viscosity η\eta is expressed by the dimensional formula τ=kηxωyrz\tau = k \eta^x \omega^y r^z, where kk is a dimensionless constant. What is the value of the sum of the exponents x+y+zx + y + z?

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Cevap: 5

Cevap

The sum of the exponents x+y+zx + y + z is 5.
By substituting the base dimensions into τ=kηxωyrz\tau = k \eta^x \omega^y r^z, we get ML2T2=(ML1T1)x(T1)yLz=MxLx+zTxyM L^2 T^{-2} = (M L^{-1} T^{-1})^x (T^{-1})^y L^z = M^x L^{-x+z} T^{-x-y}. Equating exponents of MM gives x=1x = 1. Equating exponents of TT gives 1y=2    y=1-1 - y = -2 \implies y = 1. Equating exponents of LL gives 1+z=2    z=3-1 + z = 2 \implies z = 3. Thus, x+y+z=1+1+3=5x + y + z = 1 + 1 + 3 = 5.

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1
Determine the dimensions of torque, dynamic viscosity, angular velocity, and radius in base mechanical dimensions (M, L, T).
[τ]=ML2T2[\tau] = M L^2 T^{-2}, [η]=ML1T1[\eta] = M L^{-1} T^{-1}, [ω]=T1[\omega] = T^{-1}, and [r]=L[r] = L.
Dimensional analysis requires converting all parameters into base dimensions.
2
Apply the principle of dimensional homogeneity to set up exponential equations for each base dimension.
M1L2T2=MxLx+zTxyM^1 L^2 T^{-2} = M^x L^{-x+z} T^{-x-y}.
Both sides of a physically valid equation must share identical net dimensions.
3
Solve for each exponent individually by comparing indices.
x=1x = 1, y=1y = 1, z=3z = 3.
Matching powers of M yields x=1x=1, matching powers of T yields y=1y=1, and matching powers of L yields z=3z=3.
4
Sum the three calculated exponent values.
1+1+3=51 + 1 + 3 = 5.
The question asks specifically for the value of x+y+zx + y + z.

Anahtar Kavram

Dimensional analysis and dimensional homogeneity
Tahmini Süre:1m 30s
Soru 18Soru

The resistive force FF experienced by a small sphere of radius rr moving at velocity vv through a viscous fluid is given by Stokes' law: F=6πηrvF = 6\pi \eta r v, where η\eta is the coefficient of viscosity. What is the dimensional formula of η\eta?

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Cevap: M L1T1\text{M L}^{-1}\text{T}^{-1}

Cevap

The dimensional formula of the coefficient of viscosity η\eta is M L1T1\text{M L}^{-1}\text{T}^{-1}.
Rearranging Stokes' law gives η=F6πrv\eta = \frac{F}{6\pi r v}. Since the constant 6π6\pi has no dimensions, substituting [F]=M L T2[F] = \text{M L T}^{-2}, [r]=L[r] = \text{L}, and [v]=L T1[v] = \text{L T}^{-1} yields [η]=M L T2L2T1=M L1T1[\eta] = \frac{\text{M L T}^{-2}}{\text{L}^2 \text{T}^{-1}} = \text{M L}^{-1}\text{T}^{-1}.

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1
Isolate the coefficient of viscosity η\eta from Stokes' formula
η=F6πrv\eta = \frac{F}{6\pi r v}
Numerical constants like 6π6\pi are dimensionless, so [η]=[F][r][v][\eta] = \frac{[F]}{[r][v]}.
2
Substitute the fundamental dimensions for force, radius, and velocity
[F]=M L T2[F] = \text{M L T}^{-2}, [r]=L[r] = \text{L}, and [v]=L T1[v] = \text{L T}^{-1}
Force is mass times acceleration, radius is length, and velocity is displacement per unit time.
3
Perform exponent simplification for like base dimensions
[η]=M L T2LL T1=M L T2L2T1=M L12T2(1)=M L1T1[\eta] = \frac{\text{M L T}^{-2}}{\text{L} \cdot \text{L T}^{-1}} = \frac{\text{M L T}^{-2}}{\text{L}^2 \text{T}^{-1}} = \text{M L}^{1-2} \text{T}^{-2-(-1)} = \text{M L}^{-1}\text{T}^{-1}
Subtract indices of denominator dimensions from those in the numerator.

Anahtar Kavram

Dimensional Analysis of Viscosity

Alternatif Yöntem

Alternatively, unit derivation can be used: the SI unit of viscosity is Nsm2\text{N}\cdot\text{s}\cdot\text{m}^{-2}. Replacing Newtons with fundamental SI units (kgms2\text{kg}\cdot\text{m}\cdot\text{s}^{-2}) gives (kgms2)sm2=kgm1s1(\text{kg}\cdot\text{m}\cdot\text{s}^{-2}) \cdot \text{s} \cdot \text{m}^{-2} = \text{kg}\cdot\text{m}^{-1}\cdot\text{s}^{-1}, which corresponds directly to [M L1T1][\text{M L}^{-1}\text{T}^{-1}].
Tahmini Süre:1m 0s