Why is the maximum height of a mountain about $\sim 10 \ km$ on Earth?

Vedclass pdf generator app on play store
Vedclass iOS app on app store
(N/A) The maximum height of a mountain on Earth depends upon the shear modulus of the rock.
$A$ mountain base is not under uniform compression,and this provides some shearing stress to the rocks,under which they can flow.
The stress due to all the material on the top should be less than the critical shearing stress at which the rocks flow.
At the bottom of a mountain of height $h$,the force per unit area due to the weight of the mountain is $h \rho g$,where $\rho$ is the density of the material of the mountain and $g$ is the acceleration due to gravity.
The material at the bottom experiences this force in the vertical direction,and the sides of the mountain are free.
This creates a shear component,which is approximately $h \rho g$ itself.
The elastic limit for a typical rock is $30 \times 10^{7} \ N \ m^{-2}$.
Therefore,$h \rho g = \text{elastic limit}$.
$h \rho g = 30 \times 10^{7}$.
$h = \frac{30 \times 10^{7}}{\rho g}$.
Substituting $\rho = 3 \times 10^{3} \ kg \ m^{-3}$ and $g = 10 \ m \ s^{-2}$:
$h = \frac{30 \times 10^{7}}{3 \times 10^{3} \times 10} = 10^{4} \ m = 10 \ km$.
This value is consistent with the height of Mt. Everest $(8848 \ m)$.

Explore More

Similar Questions

Copper has a face-centered cubic $(fcc)$ lattice with an interatomic spacing equal to $2.54 \ \mathring{A}$. The value of the lattice constant for this lattice is .... $\mathring{A}$ $[AIPMT \ 2005]$

Difficult
View Solution

$A$ body of mass $10 \, kg$ is attached to the end of a wire of length $0.3 \, m$. If the breaking stress of the wire is $4.8 \times 10^7 \, N/m^2$ and its cross-sectional area is $10^{-6} \, m^2$,what is the maximum angular velocity in $rad/sec$ with which it can be rotated in a horizontal plane without breaking the wire?

$A$ string of cross-sectional area $4 \times 10^{-6} \, m^{2}$ and length $0.5 \, m$ is connected to a rigid body of mass $2 \, kg$. The body is rotated in a vertical circular path of radius $0.5 \, m$. The body acquires a speed of $5 \, m/s$ at the bottom of the circular path. The strain produced in the string when the body is at the bottom of the circle is $\dots \times 10^{-5}$. (Use Young's modulus $Y = 10^{11} \, N/m^{2}$ and $g = 10 \, m/s^{2}$)

To break a wire,a breaking stress of $10^6 \, N/m^2$ is required. If the density of the material is $3 \times 10^3 \, kg/m^3$,then the length of the wire which will break by its own weight will be......... $m$ (Take $g = 10 \, m/s^2$)

Difficult
View Solution

Match the following:
Column $I$Column $II$
$A$. Hooke's law$1$. Tangential strain
$B$. Shearing strain$2$. Temporary loss of elastic property
$C$. Bulk strain$3$. Elastic limit
$D$. Elastic fatigue$4$. $3$ times the linear strain

Vedclass Products

For Students

Vedclass Test Series

Mock tests in real JEE/NEET style with performance analysis. 5-day free trial.

Start Free Trial
For Teachers

Exam Paper Generator

Generate Set A/B/C/D exam papers from 7.5L+ questions in 2 minutes. 3 chapters free.

Try Free
For Institutes

Online Exam Module

Live online exams with unlimited students, 360° analytics & white-label branding.

See Demo